master
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a Code for the Combination of Indirect and Direct Constraints on High Energy Physics Models |
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master
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a Code for the Combination of Indirect and Direct Constraints on High Energy Physics Models |
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A class for the caching of some THDM objects. More...
#include <THDMcache.h>
A class for the caching of some THDM objects.
At the moment the Passarino-Veltman functions for STU and the calculation of the Higgs observables ( \(h\) signal strengths and searches for \(H\) and \(A\)) are cached. The tables are also read here.
Definition at line 29 of file THDMcache.h.
Public Member Functions | |
| gslpp::complex | A_A_D (const double mA2, const double cW2, const double Ms, const double Mb, const double MZ) const |
| Amplitude for a CP-odd Higgs boson decay to a photon and a Z boson including the strange and bottom quarks in the loop. More... | |
| gslpp::complex | A_A_L (const double mA2, const double cW2, const double Mmu, const double Mtau, const double MZ) const |
| Amplitude for a CP-odd Higgs boson decay to a photon and a Z boson including muons and taus in the loop. More... | |
| gslpp::complex | A_A_U (const double mA2, const double cW2, const double Mc, const double Mt, const double MZ) const |
| Amplitude for a CP-odd Higgs boson decay to a photon and a Z boson including the charm and top quarks in the loop. More... | |
| gslpp::complex | A_h_D (const double mHl2, const double cW2, const double Md, const double Ms, const double Mb, const double MZ) const |
| Amplitude for the SM Higgs boson decay to a photon and a Z boson including the down-type quarks in the loop. More... | |
| gslpp::complex | A_H_Hp (const double mHp2, const double mH, const double cW2, const double MZ) const |
| Amplitude for a CP-even Higgs boson decay to a photon and a Z boson including the charged Higgs boson in the loop. More... | |
| gslpp::complex | A_h_L (const double mHl2, const double cW2, const double Me, const double Mmu, const double Mtau, const double MZ) const |
| Amplitude for the SM Higgs boson decay to a photon and a Z boson including the leptons in the loop. More... | |
| gslpp::complex | A_h_U (const double mHl2, const double cW2, const double Mu, const double Mc, const double Mt, const double MZ) const |
| Amplitude for the SM Higgs boson decay to a photon and a Z boson including the up-type quarks in the loop. More... | |
| gslpp::complex | A_H_W (const double mH, const double cW2, const double MW, const double MZ) const |
| Amplitude for a CP-even Higgs boson decay to a photon and a Z boson including the W boson in the loop. More... | |
| gslpp::complex | A_HH_D (const double mHh2, const double cW2, const double Ms, const double Mb, const double MZ) const |
| Amplitude for a heavy CP-even Higgs boson decay to a photon and a Z boson including the strange and bottom quarks in the loop. More... | |
| gslpp::complex | A_HH_L (const double mHh2, const double cW2, const double Mmu, const double Mtau, const double MZ) const |
| Amplitude for a heavy CP-even Higgs boson decay to a photon and a Z boson including muons and taus in the loop. More... | |
| gslpp::complex | A_HH_U (const double mHh2, const double cW2, const double Mc, const double Mt, const double MZ) const |
| Amplitude for a heavy CP-even Higgs boson decay to a photon and a Z boson including the charm and top quarks in the loop. More... | |
| gslpp::complex | B00_MZ2_0_mA2_mHp2 (const double MZ2, const double mA2, const double mHp2) const |
| \(B_{00}(0; mA2, mHp2)\). More... | |
| gslpp::complex | B00_MZ2_0_mHh2_mA2 (const double MZ2, const double mHh2, const double mA2) const |
| \(B_{00}(0; mHh2, mA2)\). More... | |
| gslpp::complex | B00_MZ2_0_mHh2_mHp2 (const double MZ2, const double mHh2, const double mHp2) const |
| \(B_{00}(0; mHh2, mHp2)\). More... | |
| gslpp::complex | B00_MZ2_0_mHl2_mA2 (const double MZ2, const double mHl2, const double mA2) const |
| \(B_{00}(0; mHl2, mA2)\). More... | |
| gslpp::complex | B00_MZ2_0_mHl2_mHp2 (const double MZ2, const double mHl2, const double mHp2) const |
| \(B_{00}(0; mHl2, mHp2)\). More... | |
| gslpp::complex | B00_MZ2_0_mHp2_mHp2 (const double MZ2, const double mHp2) const |
| \(B_{00}(0; mHl2, mHp2)\). More... | |
| gslpp::complex | B00_MZ2_0_MW2_mHh2 (const double MZ2, const double MW2, const double mHh2) const |
| \(B_{00}(0; MW2, mHh2)\). More... | |
| gslpp::complex | B00_MZ2_0_MW2_mHl2 (const double MZ2, const double MW2, const double mHl2) const |
| \(B_{00}(0; MW2, mHl2)\). More... | |
| gslpp::complex | B00_MZ2_0_MZ2_mHh2 (const double MZ2, const double mHh2) const |
| \(B_{00}(0; MZ2, mHh2)\). More... | |
| gslpp::complex | B00_MZ2_0_MZ2_mHl2 (const double MZ2, const double mHl2) const |
| \(B_{00}(0; MZ2, mHl2)\). More... | |
| gslpp::complex | B00_MZ2_MW2_mA2_mHp2 (const double MZ2, const double MW2, const double mA2, const double mHp2) const |
| \(B_{00}(MW2; mA2, mHp2)\). More... | |
| gslpp::complex | B00_MZ2_MW2_mHh2_mHp2 (const double MZ2, const double MW2, const double mHh2, const double mHp2) const |
| \(B_{00}(MW2; mHh2, mHp2)\). More... | |
| gslpp::complex | B00_MZ2_MW2_mHl2_mHp2 (const double MZ2, const double MW2, const double mHl2, const double mHp2) const |
| \(B_{00}(MW2; mHl2, mHp2)\). More... | |
| gslpp::complex | B00_MZ2_MW2_mHp2_mHp2 (const double MZ2, const double MW2, const double mHp2) const |
| \(B_{00}(MW2; mHp2, mHp2)\). More... | |
| gslpp::complex | B00_MZ2_MW2_MW2_mHh2 (const double MZ2, const double MW2, const double mHh2) const |
| \(B_{00}(MW2; MW2, mHh2)\). More... | |
| gslpp::complex | B00_MZ2_MW2_MW2_mHl2 (const double MZ2, const double MW2, const double mHl2) const |
| \(B_{00}(MW2; MW2, mHl2)\). More... | |
| gslpp::complex | B00_MZ2_MZ2_mHh2_mA2 (const double MZ2, const double mHh2, const double mA2) const |
| \(B_{00}(MZ2; mHh2, mA2)\). More... | |
| gslpp::complex | B00_MZ2_MZ2_mHl2_mA2 (const double MZ2, const double mHl2, const double mA2) const |
| \(B_{00}(MZ2; mHh2, mA2)\). More... | |
| gslpp::complex | B00_MZ2_MZ2_mHp2_mHp2 (const double MZ2, const double mHp2) const |
| \(B_{00}(MZ2; mHp2, mHp2)\). More... | |
| gslpp::complex | B00_MZ2_MZ2_MZ2_mHh2 (const double MZ2, const double mHh2) const |
| \(B_{00}(MZ2; MZ2, mHh2)\). More... | |
| gslpp::complex | B00_MZ2_MZ2_MZ2_mHl2 (const double MZ2, const double mHl2) const |
| \(B_{00}(MZ2; MZ2, mHl2)\). More... | |
| gslpp::complex | B0_MZ2_0_0_mHh2 (const double MZ2, const double mHh2) const |
| \(B_0(0; 0, mHh2)\). More... | |
| gslpp::complex | B0_MZ2_0_0_mHl2 (const double MZ2, const double mHl2) const |
| \(B_0(0; 0, mHl2)\). More... | |
| gslpp::complex | B0_MZ2_0_mA2_mHh2 (const double MZ2, const double mA2, const double mHh2) const |
| \(B_0(0; mA2, mHh2)\). More... | |
| gslpp::complex | B0_MZ2_0_mA2_mHl2 (const double MZ2, const double mA2, const double mHl2) const |
| \(B_0(0; mA2, mHl2)\). More... | |
| gslpp::complex | B0_MZ2_0_mHp2_mHh2 (const double MZ2, const double mHp2, const double mHh2) const |
| \(B_0(0; mHp2, mHh2)\). More... | |
| gslpp::complex | B0_MZ2_0_mHp2_mHl2 (const double MZ2, const double mHp2, const double mHl2) const |
| \(B_0(0; mHp2, mHl2)\). More... | |
| gslpp::complex | B0_MZ2_0_MW2_mHh2 (const double MZ2, const double MW2, const double mHh2) const |
| \(B_0(0; MW2, mHh2)\). More... | |
| gslpp::complex | B0_MZ2_0_MW2_mHl2 (const double MZ2, const double MW2, const double mHl2) const |
| \(B_0(0; MW2, mHl2)\). More... | |
| gslpp::complex | B0_MZ2_0_MZ2_mHh2 (const double MZ2, const double mHh2) const |
| \(B_0(0; MZ2, mHh2)\). More... | |
| gslpp::complex | B0_MZ2_0_MZ2_mHl2 (const double MZ2, const double mHl2) const |
| \(B_0(0; MZ2, mHl2)\). More... | |
| gslpp::complex | B0_MZ2_mA2_0_mHh2 (const double MZ2, const double mA2, const double mHh2) const |
| \(B_0(mA2; 0, mHh2)\). More... | |
| gslpp::complex | B0_MZ2_mA2_0_mHl2 (const double MZ2, const double mA2, const double mHl2) const |
| \(B_0(mA2; 0, mHl2)\). More... | |
| gslpp::complex | B0_MZ2_mA2_mA2_mHh2 (const double MZ2, const double mA2, const double mHh2) const |
| \(B_0(mA2; mA2, mHh2)\). More... | |
| gslpp::complex | B0_MZ2_mA2_mA2_mHl2 (const double MZ2, const double mA2, const double mHl2) const |
| \(B_0(mA2; mA2, mHl2)\). More... | |
| gslpp::complex | B0_MZ2_mHh2_0_0 (const double MZ2, const double mHh2) const |
| \(B_0(mHh2; 0, 0)\). More... | |
| gslpp::complex | B0_MZ2_mHh2_0_mA2 (const double MZ2, const double mHh2, const double mA2) const |
| \(B_0(mHh2; 0, mA2)\). More... | |
| gslpp::complex | B0_MZ2_mHh2_0_mHp2 (const double MZ2, const double mHh2, const double mHp2) const |
| \(B_0(mHh2; 0, mHp2)\). More... | |
| gslpp::complex | B0_MZ2_mHh2_mA2_mA2 (const double MZ2, const double mHh2, const double mA2) const |
| \(B_0(mHh2; mA2, mA2)\). More... | |
| gslpp::complex | B0_MZ2_mHh2_mHh2_mHh2 (const double MZ2, const double mHh2) const |
| \(B_0(mHh2; mHh2, mHh2)\). More... | |
| gslpp::complex | B0_MZ2_mHh2_mHh2_mHl2 (const double MZ2, const double mHh2, const double mHl2) const |
| \(B_0(mHh2; mHh2, mHl2)\). More... | |
| gslpp::complex | B0_MZ2_mHh2_mHl2_mHl2 (const double MZ2, const double mHh2, const double mHl2) const |
| \(B_0(mHh2; mHl2, mHl2)\). More... | |
| gslpp::complex | B0_MZ2_mHh2_mHp2_mHp2 (const double MZ2, const double mHh2, const double mHp2) const |
| \(B_0(mHh2; mHp2, mHp2)\). More... | |
| gslpp::complex | B0_MZ2_mHl2_0_0 (const double MZ2, const double mHl2) const |
| \(B_0(mHl2; 0, 0)\). More... | |
| gslpp::complex | B0_MZ2_mHl2_0_mA2 (const double MZ2, const double mHl2, const double mA2) const |
| \(B_0(mHl2; 0, mHp2)\). More... | |
| gslpp::complex | B0_MZ2_mHl2_0_mHp2 (const double MZ2, const double mHl2, const double mHp2) const |
| \(B_0(mHl2; 0, mHp2)\). More... | |
| gslpp::complex | B0_MZ2_mHl2_mA2_mA2 (const double MZ2, const double mHl2, const double mA2) const |
| \(B_0(mHl2; mA2, mA2)\). More... | |
| gslpp::complex | B0_MZ2_mHl2_mHh2_mHh2 (const double MZ2, const double mHl2, const double mHh2) const |
| \(B_0(mHl2; mHh2, mHh2)\). More... | |
| gslpp::complex | B0_MZ2_mHl2_mHh2_mHl2 (const double MZ2, const double mHl2, const double mHh2) const |
| \(B_0(mHl2; mHh2, mHl2)\). More... | |
| gslpp::complex | B0_MZ2_mHl2_mHl2_mHl2 (const double MZ2, const double mHl2) const |
| \(B_0(mHl2; mHl2, mHl2)\). More... | |
| gslpp::complex | B0_MZ2_mHl2_mHp2_mHp2 (const double MZ2, const double mHl2, const double mHp2) const |
| \(B_0(mHl2; mHp2, mHp2)\). More... | |
| gslpp::complex | B0_MZ2_mHp2_0_mHh2 (const double MZ2, const double mHp2, const double mHh2) const |
| \(B_0(mHp2; 0, mHh2)\). More... | |
| gslpp::complex | B0_MZ2_mHp2_0_mHl2 (const double MZ2, const double mHp2, const double mHl2) const |
| \(B_0(mHp2; 0, mHl2)\). More... | |
| gslpp::complex | B0_MZ2_mHp2_mHp2_mHh2 (const double MZ2, const double mHp2, const double mHh2) const |
| \(B_0(mHp2; mHp2, mHh2)\). More... | |
| gslpp::complex | B0_MZ2_mHp2_mHp2_mHl2 (const double MZ2, const double mHp2, const double mHl2) const |
| \(B_0(mHp2; mHp2, mHl2)\). More... | |
| gslpp::complex | B0_MZ2_MW2_MW2_mHh2 (const double MZ2, const double MW2, const double mHh2) const |
| \(B_0(MW2; MW2, mHh2)\). More... | |
| gslpp::complex | B0_MZ2_MW2_MW2_mHl2 (const double MZ2, const double MW2, const double mHl2) const |
| \(B_0(MW2; MW2, mHl2)\). More... | |
| gslpp::complex | B0_MZ2_MZ2_MZ2_mHh2 (const double MZ2, const double mHh2) const |
| \(B_0(MZ2; MZ2, mHh2)\). More... | |
| gslpp::complex | B0_MZ2_MZ2_MZ2_mHl2 (const double MZ2, const double mHl2) const |
| \(B_0(MZ2; MZ2, mHl2)\). More... | |
| gslpp::complex | B0p_MZ2_0_0_mHh2 (const double MZ2, const double mHh2) const |
| \(B_{0p}(0; 0, mHh2)\). More... | |
| gslpp::complex | B0p_MZ2_0_0_mHl2 (const double MZ2, const double mHl2) const |
| \(B_{0p}(0; 0, mHl2)\). More... | |
| gslpp::complex | B0p_MZ2_0_mA2_mHh2 (const double MZ2, const double mA2, const double mHh2) const |
| \(B_{0p}(0; mA2, mHh2)\). More... | |
| gslpp::complex | B0p_MZ2_0_mA2_mHl2 (const double MZ2, const double mA2, const double mHl2) const |
| \(B_{0p}(0; mA2, mHl2)\). More... | |
| gslpp::complex | B0p_MZ2_0_mHp2_mA2 (const double MZ2, const double mHp2, const double mA2) const |
| \(B_{0p}(0; mHp2, mHA2)\). More... | |
| gslpp::complex | B0p_MZ2_0_mHp2_mHh2 (const double MZ2, const double mHp2, const double mHh2) const |
| \(B_{0p}(0; mHp2, mHh2)\). More... | |
| gslpp::complex | B0p_MZ2_0_mHp2_mHl2 (const double MZ2, const double mHp2, const double mHl2) const |
| \(B_{0p}(0; mHp2, mHl2)\). More... | |
| gslpp::complex | B0p_MZ2_mA2_0_mHh2 (const double MZ2, const double mA2, const double mHh2) const |
| \(B_{0p}(mA2; 0, mHh2)\). More... | |
| gslpp::complex | B0p_MZ2_mA2_0_mHl2 (const double MZ2, const double mA2, const double mHl2) const |
| \(B_{0p}(mA2; 0, mHl2)\). More... | |
| gslpp::complex | B0p_MZ2_mA2_0_mHp2 (const double MZ2, const double mA2, const double mHp2) const |
| \(B_{0p}(mA2; 0, mHp2)\). More... | |
| gslpp::complex | B0p_MZ2_mA2_mA2_mHh2 (const double MZ2, const double mA2, const double mHh2) const |
| \(B_{0p}(mA2; mA2, mHh2)\). More... | |
| gslpp::complex | B0p_MZ2_mA2_mA2_mHl2 (const double MZ2, const double mA2, const double mHl2) const |
| \(B_{0p}(mA2; mA2, mHl2)\). More... | |
| gslpp::complex | B0p_MZ2_mHh2_0_0 (const double MZ2, const double mHh2) const |
| \(B_{0p}(mHh2; 0, 0)\). More... | |
| gslpp::complex | B0p_MZ2_mHh2_0_mA2 (const double MZ2, const double mHh2, const double mA2) const |
| \(B_{0p}(mHh2; 0, mA2)\). More... | |
| gslpp::complex | B0p_MZ2_mHh2_0_mHp2 (const double MZ2, const double mHh2, const double mHp2) const |
| \(B_{0p}(mHh2; 0, mHp2)\). More... | |
| gslpp::complex | B0p_MZ2_mHh2_mA2_mA2 (const double MZ2, const double mHh2, const double mA2) const |
| \(B_{0p}(mHh2; mA2, mA2)\). More... | |
| gslpp::complex | B0p_MZ2_mHh2_mHh2_mHh2 (const double MZ2, const double mHh2) const |
| \(B_{0p}(mHh2; mHh2, mHh2)\). More... | |
| gslpp::complex | B0p_MZ2_mHh2_mHh2_mHl2 (const double MZ2, const double mHh2, const double mHl2) const |
| \(B_{0p}(mHh2; mHh2, mHl2)\). More... | |
| gslpp::complex | B0p_MZ2_mHh2_mHl2_mHl2 (const double MZ2, const double mHh2, const double mHl2) const |
| \(B_{0p}(mHh2; mHl2, mHl2)\). More... | |
| gslpp::complex | B0p_MZ2_mHh2_mHp2_mHp2 (const double MZ2, const double mHh2, const double mHp2) const |
| \(B_{0p}(mHh2; mHp2, mHp2)\). More... | |
| gslpp::complex | B0p_MZ2_mHl2_0_0 (const double MZ2, const double mHl2) const |
| \(B_{0p}(mHl2; 0, 0)\). More... | |
| gslpp::complex | B0p_MZ2_mHl2_0_mA2 (const double MZ2, const double mHl2, const double mA2) const |
| \(B_{0p}(mHl2; 0, mHp2)\). More... | |
| gslpp::complex | B0p_MZ2_mHl2_0_mHp2 (const double MZ2, const double mHl2, const double mHp2) const |
| \(B_{0p}(mHl2; 0, mHp2)\). More... | |
| gslpp::complex | B0p_MZ2_mHl2_mA2_mA2 (const double MZ2, const double mHl2, const double mA2) const |
| \(B_{0p}(mHl2; mA2, mA2)\). More... | |
| gslpp::complex | B0p_MZ2_mHl2_mHh2_mHh2 (const double MZ2, const double mHl2, const double mHh2) const |
| \(B_{0p}(mHl2; mHh2, mHh2)\). More... | |
| gslpp::complex | B0p_MZ2_mHl2_mHh2_mHl2 (const double MZ2, const double mHl2, const double mHh2) const |
| \(B_{0p}(mHl2; mHh2, mHl2)\). More... | |
| gslpp::complex | B0p_MZ2_mHl2_mHl2_mHl2 (const double MZ2, const double mHl2) const |
| \(B_{0p}(mHl2; mHl2, mHl2)\). More... | |
| gslpp::complex | B0p_MZ2_mHl2_mHp2_mHp2 (const double MZ2, const double mHl2, const double mHp2) const |
| \(B_{0p}(mHl2; mHp2, mHp2)\). More... | |
| gslpp::complex | B0p_MZ2_mHp2_0_mA2 (const double MZ2, const double mHp2, const double mA2) const |
| \(B_{0p}(mHp2; 0, mHA2)\). More... | |
| gslpp::complex | B0p_MZ2_mHp2_0_mHh2 (const double MZ2, const double mHp2, const double mHh2) const |
| \(B_{0p}(mHp2; 0, mHh2)\). More... | |
| gslpp::complex | B0p_MZ2_mHp2_0_mHl2 (const double MZ2, const double mHp2, const double mHl2) const |
| \(B_{0p}(mHp2; 0, mHl2)\). More... | |
| gslpp::complex | B0p_MZ2_mHp2_mHp2_mHh2 (const double MZ2, const double mHp2, const double mHh2) const |
| \(B_{0p}(mHp2; mHp2, mHh2)\). More... | |
| gslpp::complex | B0p_MZ2_mHp2_mHp2_mHl2 (const double MZ2, const double mHp2, const double mHl2) const |
| \(B_{0p}(mHp2; mHp2, mHl2)\). More... | |
| int | CacheCheck (const gslpp::complex cache[][CacheSize], const int NumPar, const double params[]) const |
| Check whether for the latest set of parameters a value is in the cache. More... | |
| int | CacheCheckReal (const double cache[][CacheSize], const int NumPar, const double params[]) const |
| Check whether for the latest set of parameters a value is in the cache. More... | |
| void | CacheShift (gslpp::complex cache[][CacheSize], const int NumPar, const double params[], const gslpp::complex newResult) const |
| Adds a new result and its parameters into the cache. More... | |
| void | CacheShiftReal (double cache[][CacheSize], const int NumPar, const double params[], const double newResult) const |
| Adds a new result and its parameters into the cache. More... | |
| void | computeAlimits () |
| void | computeAquantities () |
| void | computeHHlimits () |
| void | computeHHquantities () |
| void | computeHpquantities () |
| void | computeSignalStrengthQuantities () |
| void | computeWFRcombinations () |
| double | cW2THDM (const double c02) const |
| double | g_HH_HpHm (const double mHp2, const double mHh2, const double tanb, const double m12_2, const double bma, const double vev) const |
| const PVfunctions | getPV () const |
| double | ghHpHm (const double mHp2, const double tanb, const double m12_2, const double bma, const double mHl2, const double vev) const |
| gslpp::complex | I_A_D (const double mA2, const double Ms, const double Mb) const |
| Amplitude for a CP-odd Higgs boson decay to diphotons including the strange and bottom quarks in the loop. More... | |
| gslpp::complex | I_A_L (const double mA2, const double Mmu, const double Mtau) const |
| Amplitude for a CP-odd Higgs boson decay to diphotons including muons and taus in the loop. More... | |
| gslpp::complex | I_A_U (const double mA2, const double Mc, const double Mt) const |
| Amplitude for a CP-odd Higgs boson decay to diphotons including the charm and top quarks in the loop. More... | |
| gslpp::complex | I_h_D (const double mHl2, const double Md, const double Ms, const double Mb) const |
| Amplitude for the SM Higgs boson decay to diphotons including the down-type quarks in the loop. More... | |
| gslpp::complex | I_H_Hp (const double mHp2, const double mH) const |
| Amplitude for a CP-even Higgs boson decay to diphotons including the charged Higgs boson in the loop. More... | |
| gslpp::complex | I_h_L (const double mHl2, const double Me, const double Mmu, const double Mtau) const |
| Amplitude for the SM Higgs boson decay to diphotons including the leptons in the loop. More... | |
| gslpp::complex | I_h_U (const double mHl2, const double Mu, const double Mc, const double Mt) const |
| Amplitude for the SM Higgs boson decay to diphotons including the up-type quarks in the loop. More... | |
| gslpp::complex | I_H_W (const double mH, const double MW) const |
| Amplitude for a CP-even Higgs boson decay to diphotons including the W boson in the loop. More... | |
| gslpp::complex | I_HH_D (const double mHh2, const double Ms, const double Mb) const |
| Amplitude for a heavy CP-even Higgs boson decay to diphotons including the strange and bottom quarks in the loop. More... | |
| gslpp::complex | I_HH_L (const double mHh2, const double Mmu, const double Mtau) const |
| Amplitude for a heavy CP-even Higgs boson decay to diphotons including muons and taus in the loop. More... | |
| gslpp::complex | I_HH_U (const double mHh2, const double Mc, const double Mt) const |
| Amplitude for a heavy CP-even Higgs boson decay to diphotons including the charm and top quarks in the loop. More... | |
| double | ie1 (double mass) |
| double | ie10 (double mass) |
| double | ie10e (double mass) |
| double | ie11 (double mass) |
| double | ie11e (double mass) |
| double | ie12 (double mass) |
| double | ie12e (double mass) |
| double | ie13 (double mass) |
| double | ie13e (double mass) |
| double | ie14 (double mass) |
| double | ie14e (double mass) |
| double | ie15 (double mass) |
| double | ie15e (double mass) |
| double | ie16 (double mass) |
| double | ie16e (double mass) |
| double | ie17 (double mass) |
| double | ie17e (double mass) |
| double | ie18 (double mass) |
| double | ie18e (double mass) |
| double | ie19 (double mass) |
| double | ie19e (double mass) |
| double | ie1e (double mass) |
| double | ie2 (double mass) |
| double | ie20 (double mass) |
| double | ie20e (double mass) |
| double | ie21 (double mass) |
| double | ie21e (double mass) |
| double | ie22 (double mass) |
| double | ie22e (double mass) |
| double | ie23 (double mass) |
| double | ie23e (double mass) |
| double | ie24 (double mass) |
| double | ie24e (double mass) |
| double | ie25 (double mass) |
| double | ie25e (double mass) |
| double | ie26 (double mass) |
| double | ie26e (double mass) |
| double | ie27 (double mass) |
| double | ie27e (double mass) |
| double | ie28 (double mass) |
| double | ie28e (double mass) |
| double | ie29 (double mass) |
| double | ie29e (double mass) |
| double | ie2e (double mass) |
| double | ie3 (double mass) |
| double | ie30 (double mass) |
| double | ie30e (double mass) |
| double | ie31 (double mass) |
| double | ie31e (double mass) |
| double | ie32 (double mass) |
| double | ie32e (double mass) |
| double | ie33 (double mass) |
| double | ie33e (double mass) |
| double | ie34 (double mass) |
| double | ie34e (double mass) |
| double | ie35 (double mass) |
| double | ie35e (double mass) |
| double | ie36 (double mass) |
| double | ie36e (double mass) |
| double | ie37 (double mass) |
| double | ie37e (double mass) |
| double | ie38 (double mass) |
| double | ie38e (double mass) |
| double | ie39 (double mass) |
| double | ie39e (double mass) |
| double | ie3e (double mass) |
| double | ie4 (double mass) |
| double | ie40 (double mass) |
| double | ie40e (double mass) |
| double | ie4e (double mass) |
| double | ie5 (double mass) |
| double | ie5e (double mass) |
| double | ie6 (double mass) |
| double | ie6e (double mass) |
| double | ie7 (double mass) |
| double | ie7e (double mass) |
| double | ie8 (double mass) |
| double | ie8e (double mass) |
| double | ie9 (double mass) |
| double | ie9e (double mass) |
| double | interpolate (gslpp::matrix< double > arrayTab, double x) |
| Linearly interpolates a table with one parameter dimension. More... | |
| double | interpolate2D (gslpp::matrix< double > arrayTab, double x, double y) |
| Linearly interpolates a table with two parameter dimensions. More... | |
| double | ip_Br_HPtobb (double mass) |
| Interpolating function for the SM branching ratio to two bottom quarks. More... | |
| double | ip_Br_HPtocc (double mass) |
| Interpolating function for the SM branching ratio to two charm quarks. More... | |
| double | ip_Br_HPtomumu (double mass) |
| Interpolating function for the SM branching ratio to two muons. More... | |
| double | ip_Br_HPtotautau (double mass) |
| Interpolating function for the SM branching ratio to two tau leptons. More... | |
| double | ip_Br_HPtott (double mass) |
| Interpolating function for the SM branching ratio to two top quarks. More... | |
| double | ip_Br_HPtoWW (double mass) |
| Interpolating function for the SM branching ratio to two \(W\) bosons. More... | |
| double | ip_Br_HPtoZZ (double mass) |
| Interpolating function for the SM branching ratio to two \(Z\) bosons. More... | |
| double | ip_cs_ggtoA_13 (double mass) |
| Interpolating function for the A production cross section via gluon-gluon fusion at 13 TeV. More... | |
| double | ip_cs_ggtoA_8 (double mass) |
| Interpolating function for the A production cross section via gluon-gluon fusion at 8 TeV. More... | |
| double | ip_cs_ggtoH_13 (double mass) |
| Interpolating function for the H production cross section via gluon-gluon fusion at 13 TeV. More... | |
| double | ip_cs_ggtoH_8 (double mass) |
| Interpolating function for the H production cross section via gluon-gluon fusion at 8 TeV. More... | |
| double | ip_cs_ggtoHp_13 (double mHp, double logtb) |
| Interpolating function for the H+ production cross section from two gluons at 13 TeV. More... | |
| double | ip_cs_ggtoHp_8 (double mHp, double logtb) |
| Interpolating function for the H+ production cross section from two gluons at 8 TeV. More... | |
| double | ip_cs_pptobbA_13 (double mass) |
| Interpolating function for the bottom associated A production cross section at 13 TeV. More... | |
| double | ip_cs_pptobbA_8 (double mass) |
| Interpolating function for the bottom associated A production cross section at 8 TeV. More... | |
| double | ip_cs_pptobbH_13 (double mass) |
| Interpolating function for the bottom associated H production cross section at 13 TeV. More... | |
| double | ip_cs_pptobbH_8 (double mass) |
| Interpolating function for the bottom associated H production cross section at 8 TeV. More... | |
| double | ip_cs_pptottA_13 (double mass) |
| Interpolating function for the top associated A production cross section at 13 TeV. More... | |
| double | ip_cs_pptottA_8 (double mass) |
| Interpolating function for the top associated A production cross section at 8 TeV. More... | |
| double | ip_cs_pptottH_13 (double mass) |
| Interpolating function for the top associated H production cross section at 13 TeV. More... | |
| double | ip_cs_pptottH_8 (double mass) |
| Interpolating function for the top associated H production cross section at 8 TeV. More... | |
| double | ip_cs_VBFtoH_13 (double mass) |
| Interpolating function for the H production cross section via vector boson fusion at 13 TeV. More... | |
| double | ip_cs_VBFtoH_8 (double mass) |
| Interpolating function for the H production cross section via vector boson fusion at 8 TeV. More... | |
| double | ip_cs_WtoWH_13 (double mass) |
| Interpolating function for the W associated H production cross section at 13 TeV. More... | |
| double | ip_cs_WtoWH_8 (double mass) |
| Interpolating function for the W associated H production cross section at 8 TeV. More... | |
| double | ip_cs_ZtoZH_13 (double mass) |
| Interpolating function for the Z associated H production cross section at 13 TeV. More... | |
| double | ip_cs_ZtoZH_8 (double mass) |
| Interpolating function for the Z associated H production cross section at 8 TeV. More... | |
| double | ip_csr_ggA_b_13 (double mass) |
| Interpolating function for the gluon-gluon fusion A cross section ratio of the bottom-loop and the total contribution at 13 TeV. More... | |
| double | ip_csr_ggA_b_8 (double mass) |
| Interpolating function for the gluon-gluon fusion A cross section ratio of the bottom-loop and the total contribution at 8 TeV. More... | |
| double | ip_csr_ggA_t_13 (double mass) |
| Interpolating function for the gluon-gluon fusion A cross section ratio of the top-loop and the total contribution at 13 TeV. More... | |
| double | ip_csr_ggA_t_8 (double mass) |
| Interpolating function for the gluon-gluon fusion A cross section ratio of the top-loop and the total contribution at 8 TeV. More... | |
| double | ip_csr_ggH_b_13 (double mass) |
| Interpolating function for the gluon-gluon fusion H cross section ratio of the bottom-loop and the total contribution at 13 TeV. More... | |
| double | ip_csr_ggH_b_8 (double mass) |
| Interpolating function for the gluon-gluon fusion H cross section ratio of the bottom-loop and the total contribution at 8 TeV. More... | |
| double | ip_csr_ggH_t_13 (double mass) |
| Interpolating function for the gluon-gluon fusion H cross section ratio of the top-loop and the total contribution at 13 TeV. More... | |
| double | ip_csr_ggH_t_8 (double mass) |
| Interpolating function for the gluon-gluon fusion H cross section ratio of the top-loop and the total contribution at 8 TeV. More... | |
| double | ip_ex_bb_A_Zh_Zbb_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a bb associated pseudoscalar resonance decaying to a \(Z\) and an \(h\) boson, of which the latter further decays to a b quark pair. More... | |
| double | ip_ex_bb_A_Zh_Zbb_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a bb associated pseudoscalar resonance decaying to a \(Z\) and an \(h\) boson, of which the latter further decays to a b quark pair. More... | |
| double | ip_ex_bb_phi_bb_CMS8 (double mass) |
| Interpolating function for the observed CMS upper limit on a bottom quark produced scalar resonance decaying to two bottom quarks. More... | |
| double | ip_ex_bb_phi_bb_CMS8_e (double mass) |
| Interpolating function for the expected CMS upper limit on a bottom quark produced scalar resonance decaying to two bottom quarks. More... | |
| double | ip_ex_bb_phi_tautau_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a bb associated scalar resonance decaying to two tau leptons. More... | |
| double | ip_ex_bb_phi_tautau_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a bb associated scalar resonance decaying to two tau leptons. More... | |
| double | ip_ex_bb_phi_tautau_ATLAS8 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a bottom quark produced scalar resonance decaying to two tau leptons. More... | |
| double | ip_ex_bb_phi_tautau_ATLAS8_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a bottom quark produced scalar resonance decaying to two tau leptons. More... | |
| double | ip_ex_bb_phi_tautau_CMS13 (double mass) |
| Interpolating function for the observed CMS upper limit on a b associated scalar resonance decaying to two tau leptons. More... | |
| double | ip_ex_bb_phi_tautau_CMS13_e (double mass) |
| Interpolating function for the expected CMS upper limit on a b associated scalar resonance decaying to two tau leptons. More... | |
| double | ip_ex_bb_phi_tautau_CMS8 (double mass) |
| Interpolating function for the observed CMS upper limit on a bottom quark produced scalar resonance decaying to two tau leptons. More... | |
| double | ip_ex_bb_phi_tautau_CMS8_e (double mass) |
| Interpolating function for the expected CMS upper limit on a bottom quark produced scalar resonance decaying to two tau leptons. More... | |
| double | ip_ex_bb_phi_tt_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a bb associated scalar resonance decaying to t quarks. More... | |
| double | ip_ex_bb_phi_tt_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a bb associated scalar resonance decaying to t quarks. More... | |
| double | ip_ex_bsgamma (double logtb, double logmHp) |
| Interpolating function for the NNLO value for the branching ratio of \(b\to s \gamma\) decays in the THDM. More... | |
| double | ip_ex_gg_A_hZ_bbll_CMS8 (double mass) |
| Interpolating function for the observed CMS upper limit on a gluon-gluon produced pseudoscalar resonance decaying to \(hZ\) which further decay to a bottom quark pair and a light lepton pair. More... | |
| double | ip_ex_gg_A_hZ_bbll_CMS8_e (double mass) |
| Interpolating function for the expected CMS upper limit on a gluon-gluon produced pseudoscalar resonance decaying to \(hZ\) which further decay to a bottom quark pair and a light lepton pair. More... | |
| double | ip_ex_gg_A_hZ_bbZ_ATLAS8 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced pseudoscalar resonance decaying to \(hZ\) of which the Higgs further decays to a bottom quark pair. More... | |
| double | ip_ex_gg_A_hZ_bbZ_ATLAS8_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced pseudoscalar resonance decaying to \(hZ\) of which the Higgs further decays to a bottom quark pair. More... | |
| double | ip_ex_gg_A_hZ_tautaull_CMS8 (double mass) |
| Interpolating function for the observed CMS upper limit on a gluon-gluon produced pseudoscalar resonance decaying to \(hZ\) which further decay to a \(\tau\) lepton pair and a light lepton pair. More... | |
| double | ip_ex_gg_A_hZ_tautaull_CMS8_e (double mass) |
| Interpolating function for the expected CMS upper limit on a gluon-gluon produced pseudoscalar resonance decaying to \(hZ\) which further decay to a \(\tau\) lepton pair and a light lepton pair. More... | |
| double | ip_ex_gg_A_hZ_tautauZ_ATLAS8 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced pseudoscalar resonance decaying to \(hZ\) of which the Higgs further decays to a \(\tau\) lepton pair. More... | |
| double | ip_ex_gg_A_hZ_tautauZ_ATLAS8_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced pseudoscalar resonance decaying to \(hZ\) of which the Higgs further decays to a \(\tau\) lepton pair. More... | |
| double | ip_ex_gg_A_Zh_Zbb_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced pseudoscalar resonance decaying to a \(Z\) and an \(h\) boson, of which the latter further decays to a b quark pair. More... | |
| double | ip_ex_gg_A_Zh_Zbb_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced pseudoscalar resonance decaying to a \(Z\) and an \(h\) boson, of which the latter further decays to a b quark pair. More... | |
| double | ip_ex_gg_H_hh_ATLAS8 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(h\) bosons. More... | |
| double | ip_ex_gg_H_hh_ATLAS8_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(h\) bosons. More... | |
| double | ip_ex_gg_H_hh_bbtautau_CMS8 (double mass) |
| Interpolating function for the observed CMS upper limit on a gluon-gluon produced scalar resonance decaying to two \(h\) bosons which further decay to a bottom quark pair and a \(\tau\) lepton pair. More... | |
| double | ip_ex_gg_H_hh_bbtautau_CMS8_e (double mass) |
| Interpolating function for the expected CMS upper limit on a gluon-gluon produced scalar resonance decaying to two \(h\) bosons which further decay to a bottom quark pair and a \(\tau\) lepton pair. More... | |
| double | ip_ex_gg_H_WW_ATLAS8 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(W\) bosons. More... | |
| double | ip_ex_gg_H_WW_ATLAS8_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(W\) bosons. More... | |
| double | ip_ex_gg_H_WW_enumunu_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(W\) bosons which further decay to two lepton-neutrino pairs. More... | |
| double | ip_ex_gg_H_WW_enumunu_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(W\) bosons which further decay to two lepton-neutrino pairs. More... | |
| double | ip_ex_gg_H_WW_lnuqq_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(W\) bosons which further decay to a lepton-neutrino pair and a pair of quarks. More... | |
| double | ip_ex_gg_H_WW_lnuqq_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(W\) bosons which further decay to a lepton-neutrino pair and a pair of quarks. More... | |
| double | ip_ex_gg_H_ZZ_ATLAS8 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons. More... | |
| double | ip_ex_gg_H_ZZ_ATLAS8_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons. More... | |
| double | ip_ex_gg_H_ZZ_llll_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to four leptons. More... | |
| double | ip_ex_gg_H_ZZ_llll_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to four leptons. More... | |
| double | ip_ex_gg_H_ZZ_llllnunu_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two neutrinos or two leptons. More... | |
| double | ip_ex_gg_H_ZZ_llllnunu_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two neutrinos or two leptons. More... | |
| double | ip_ex_gg_H_ZZ_llnunu_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two neutrinos. More... | |
| double | ip_ex_gg_H_ZZ_llnunu_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two neutrinos. More... | |
| double | ip_ex_gg_H_ZZ_llnunu_CMS13 (double mass) |
| Interpolating function for the observed CMS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two neutrinos. More... | |
| double | ip_ex_gg_H_ZZ_llnunu_CMS13_e (double mass) |
| Interpolating function for the expected CMS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two neutrinos. More... | |
| double | ip_ex_gg_H_ZZ_llqq_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two quarks. More... | |
| double | ip_ex_gg_H_ZZ_llqq_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two quarks. More... | |
| double | ip_ex_gg_H_ZZ_nunuqq_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to two neutrinos and two quarks. More... | |
| double | ip_ex_gg_H_ZZ_nunuqq_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to two neutrinos and two quarks. More... | |
| double | ip_ex_gg_H_ZZ_qqllnunu_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to two quarks and two neutrinos or two leptons. More... | |
| double | ip_ex_gg_H_ZZ_qqllnunu_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to two quarks and two neutrinos or two leptons. More... | |
| double | ip_ex_gg_phi_gaga_CMS13 (double mass) |
| Interpolating function for the observed CMS upper limit on a gluon-gluon produced scalar resonance decaying to two photons. More... | |
| double | ip_ex_gg_phi_gaga_CMS13_e (double mass) |
| Interpolating function for the expected CMS upper limit on a gluon-gluon produced scalar resonance decaying to two photons. More... | |
| double | ip_ex_gg_phi_gaga_CMS8 (double mass) |
| Interpolating function for the observed CMS upper limit on a gluon-gluon produced scalar resonance decaying to two photons. More... | |
| double | ip_ex_gg_phi_gaga_CMS8_e (double mass) |
| Interpolating function for the expected CMS upper limit on a gluon-gluon produced scalar resonance decaying to two photons. More... | |
| double | ip_ex_gg_phi_tautau_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two tau leptons. More... | |
| double | ip_ex_gg_phi_tautau_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two tau leptons. More... | |
| double | ip_ex_gg_phi_tautau_ATLAS8 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two tau leptons. More... | |
| double | ip_ex_gg_phi_tautau_ATLAS8_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two tau leptons. More... | |
| double | ip_ex_gg_phi_tautau_CMS13 (double mass) |
| Interpolating function for the observed CMS upper limit on a gluon-gluon produced scalar resonance decaying to two tau leptons. More... | |
| double | ip_ex_gg_phi_tautau_CMS13_e (double mass) |
| Interpolating function for the expected CMS upper limit on a gluon-gluon produced scalar resonance decaying to two tau leptons. More... | |
| double | ip_ex_gg_phi_tautau_CMS8 (double mass) |
| Interpolating function for the observed CMS upper limit on a gluon-gluon produced scalar resonance decaying to two tau leptons. More... | |
| double | ip_ex_gg_phi_tautau_CMS8_e (double mass) |
| Interpolating function for the expected CMS upper limit on a gluon-gluon produced scalar resonance decaying to two tau leptons. More... | |
| double | ip_ex_gg_phi_tt_ATLAS8 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to a top quark pair. More... | |
| double | ip_ex_gg_phi_tt_ATLAS8_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to a top quark pair. More... | |
| double | ip_ex_gg_phi_Zga_llga_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to a \(Z\) boson and a photon, of which the \(Z\) further decays to two leptons. More... | |
| double | ip_ex_gg_phi_Zga_llga_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to a \(Z\) boson and a photon, of which the \(Z\) further decays to two leptons. More... | |
| double | ip_ex_ggF_H_hh_bbbb_CMS13 (double mass) |
| Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to four b quarks. More... | |
| double | ip_ex_ggF_H_hh_bbbb_CMS13_e (double mass) |
| Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to four b quarks. More... | |
| double | ip_ex_ggF_phi_Zga_CMS13 (double mass) |
| Interpolating function for the observed CMS upper limit on a gluon-gluon produced scalar resonance decaying to a \(Z\) boson and a photon. More... | |
| double | ip_ex_ggF_phi_Zga_CMS13_e (double mass) |
| Interpolating function for the expected CMS upper limit on a gluon-gluon produced scalar resonance decaying to a \(Z\) boson and a photon. More... | |
| double | ip_ex_ggVV_H_WW_lnulnu_CMS13 (double mass) |
| Interpolating function for the observed CMS upper limit on a gluon-gluon or vector boson fusion produced scalar resonance decaying to two \(W\) bosons which further decay to two lepton-neutrino pairs. More... | |
| double | ip_ex_ggVV_H_WW_lnulnu_CMS13_e (double mass) |
| Interpolating function for the expected CMS upper limit on a gluon-gluon or vector boson fusion produced scalar resonance decaying to two \(W\) bosons which further decay to two lepton-neutrino pairs. More... | |
| double | ip_ex_mu_pp_H_VV_CMS8 (double mass) |
| Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two massive vector bosons. More... | |
| double | ip_ex_mu_pp_H_VV_CMS8_e (double mass) |
| Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two massive vector bosons. More... | |
| double | ip_ex_pp_A_HZ_bbll_CMS8 (double mA, double mH) |
| Interpolating function for the observed CMS upper limit on a pseudoscalar resonance decaying to \(HZ\) which further decay to a \(b\) quark pair and a light lepton pair. More... | |
| double | ip_ex_pp_A_HZ_tautaull_CMS8 (double mA, double mH) |
| Interpolating function for the observed CMS upper limit on a pseudoscalar resonance decaying to \(HZ\) which further decay to a \(\tau\) lepton pair and a light lepton pair. More... | |
| double | ip_ex_pp_A_Zga_llga_CMS8 (double mass) |
| Interpolating function for the observed CMS upper limit on a pseudoscalar resonance decaying to a Z boson and a photon which further decay into two leptons and a photon. More... | |
| double | ip_ex_pp_A_Zga_llga_CMS8_e (double mass) |
| Interpolating function for the expected CMS upper limit on a pseudoscalar resonance decaying to a Z boson and a photon which further decay into two leptons and a photon. More... | |
| double | ip_ex_pp_H_AZ_bbll_CMS8 (double mA, double mH) |
| Interpolating function for the observed CMS upper limit on a scalar resonance decaying to \(AZ\) which further decay to a \(b\) quark pair and a light lepton pair. More... | |
| double | ip_ex_pp_H_AZ_tautaull_CMS8 (double mA, double mH) |
| Interpolating function for the observed CMS upper limit on a scalar resonance decaying to \(AZ\) which further decay to a \(\tau\) lepton pair and a light lepton pair. More... | |
| double | ip_ex_pp_H_hh_bbbb_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a spin-2 resonance decaying to two \(h\) bosons which further decay to four b quarks. More... | |
| double | ip_ex_pp_H_hh_bbbb_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a spin-2 resonance decaying to two \(h\) bosons which further decay to four b quarks. More... | |
| double | ip_ex_pp_H_hh_bbbb_CMS13 (double mass) |
| Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to four b quarks. More... | |
| double | ip_ex_pp_H_hh_bbbb_CMS13_e (double mass) |
| Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to four b quarks. More... | |
| double | ip_ex_pp_H_hh_bblnulnu_CMS13 (double mass) |
| Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to a b quark pair and two lepton-neutrino pairs. More... | |
| double | ip_ex_pp_H_hh_bblnulnu_CMS13_e (double mass) |
| Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to a b quark pair and two lepton-neutrino pairs. More... | |
| double | ip_ex_pp_H_hh_bbtautau1_CMS13 (double mass) |
| Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to a b quark pair and two tau leptons. More... | |
| double | ip_ex_pp_H_hh_bbtautau1_CMS13_e (double mass) |
| Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to a b quark pair and two tau leptons. More... | |
| double | ip_ex_pp_H_hh_bbtautau_CMS13 (double mass) |
| Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to a b quark pair and two tau leptons. More... | |
| double | ip_ex_pp_H_hh_bbtautau_CMS13_e (double mass) |
| Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to a b quark pair and two tau leptons. More... | |
| double | ip_ex_pp_H_hh_bbVV_CMS13 (double mass) |
| Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to a b quark pair, two leptons and two neutrinos. More... | |
| double | ip_ex_pp_H_hh_bbVV_CMS13_e (double mass) |
| Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to a b quark pair, two leptons and two neutrinos. More... | |
| double | ip_ex_pp_H_hh_CMS8 (double mass) |
| Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(h\) bosons. More... | |
| double | ip_ex_pp_H_hh_CMS8_e (double mass) |
| Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(h\) bosons. More... | |
| double | ip_ex_pp_H_hh_gagabb_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to two photons and a b quark pair. More... | |
| double | ip_ex_pp_H_hh_gagabb_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to two photons and a b quark pair. More... | |
| double | ip_ex_pp_H_hh_gagabb_CMS13 (double mass) |
| Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to two photons and a b quark pair. More... | |
| double | ip_ex_pp_H_hh_gagabb_CMS13_e (double mass) |
| Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to two photons and a b quark pair. More... | |
| double | ip_ex_pp_H_hh_gagaWW_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(h\) bosons which further decay to two photons and two \(W\) bosons. More... | |
| double | ip_ex_pp_H_hh_gagaWW_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(h\) bosons which further decay to two photons and two \(W\) bosons. More... | |
| double | ip_ex_pp_H_VV_qqqq_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a scalar resonance decaying to two \(W\) or \(Z\) bosons which further decay hadronically. More... | |
| double | ip_ex_pp_H_VV_qqqq_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a scalar resonance decaying to two \(W\) or \(Z\) bosons which further decay hadronically. More... | |
| double | ip_ex_pp_H_ZZ_llll_CMS13 (double mass) |
| Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(Z\) bosons which further decay to four leptons. More... | |
| double | ip_ex_pp_H_ZZ_llll_CMS13_e (double mass) |
| Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(Z\) bosons which further decay to four leptons. More... | |
| double | ip_ex_pp_H_ZZ_llnunu_CMS13 (double mass) |
| Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two neutrinos. More... | |
| double | ip_ex_pp_H_ZZ_llnunu_CMS13_e (double mass) |
| Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two neutrinos. More... | |
| double | ip_ex_pp_H_ZZ_llqq_CMS13 (double mass) |
| Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two quarks. More... | |
| double | ip_ex_pp_H_ZZ_llqq_CMS13_e (double mass) |
| Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two quarks. More... | |
| double | ip_ex_pp_Hp_taunu_CMS8 (double mass) |
| Interpolating function for the observed CMS upper limit on a singly charged scalar resonance decaying to a \(\tau\) lepton and a neutrino. More... | |
| double | ip_ex_pp_Hp_taunu_CMS8_e (double mass) |
| Interpolating function for the expected CMS upper limit on a singly charged scalar resonance decaying to a \(\tau\) lepton and a neutrino. More... | |
| double | ip_ex_pp_Hp_tb_ATLAS13_1 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a singly charged scalar resonance decaying to a \(t\) quark and a \(b\) quark. More... | |
| double | ip_ex_pp_Hp_tb_ATLAS13_1_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a singly charged scalar resonance decaying to a \(t\) quark and a \(b\) quark. More... | |
| double | ip_ex_pp_Hp_tb_ATLAS13_2 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a singly charged scalar resonance decaying to a \(t\) quark and a \(b\) quark. More... | |
| double | ip_ex_pp_Hp_tb_ATLAS13_2_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a singly charged scalar resonance decaying to a \(t\) quark and a \(b\) quark. More... | |
| double | ip_ex_pp_Hp_tb_CMS8 (double mass) |
| Interpolating function for the observed CMS upper limit on a singly charged scalar resonance decaying to a \(t\) quark and a \(b\) quark. More... | |
| double | ip_ex_pp_Hp_tb_CMS8_e (double mass) |
| Interpolating function for the expected CMS upper limit on a singly charged scalar resonance decaying to a \(t\) quark and a \(b\) quark. More... | |
| double | ip_ex_pp_Hpm_taunu_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a singly charged scalar resonance decaying to a \(\tau\) lepton and a neutrino. More... | |
| double | ip_ex_pp_Hpm_taunu_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a singly charged scalar resonance decaying to a \(\tau\) lepton and a neutrino. More... | |
| double | ip_ex_pp_Hpm_taunu_ATLAS8 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a singly charged scalar resonance decaying to a \(\tau\) lepton and a neutrino. More... | |
| double | ip_ex_pp_Hpm_taunu_ATLAS8_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a singly charged scalar resonance decaying to a \(\tau\) lepton and a neutrino. More... | |
| double | ip_ex_pp_Hpm_taunu_CMS13 (double mass) |
| Interpolating function for the observed CMS upper limit on a singly charged scalar resonance decaying to a \(\tau\) lepton and a neutrino. More... | |
| double | ip_ex_pp_Hpm_taunu_CMS13_e (double mass) |
| Interpolating function for the expected CMS upper limit on a singly charged scalar resonance decaying to a \(\tau\) lepton and a neutrino. More... | |
| double | ip_ex_pp_Hpm_tb_ATLAS8 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a singly charged scalar resonance decaying to a \(t\) quark and a \(b\) quark. More... | |
| double | ip_ex_pp_Hpm_tb_ATLAS8_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a singly charged scalar resonance decaying to a \(t\) quark and a \(b\) quark. More... | |
| double | ip_ex_pp_phi_bb_CMS13 (double mass) |
| Interpolating function for the observed CMS upper limit on a scalar resonance decaying to a b quark pair. More... | |
| double | ip_ex_pp_phi_bb_CMS13_e (double mass) |
| Interpolating function for the expected CMS upper limit on a scalar resonance decaying to a b quark pair. More... | |
| double | ip_ex_pp_phi_gaga_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a scalar resonance decaying to two photons. More... | |
| double | ip_ex_pp_phi_gaga_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a scalar resonance decaying to two photons. More... | |
| double | ip_ex_pp_phi_gaga_ATLAS8 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a scalar resonance decaying to two photons. More... | |
| double | ip_ex_pp_phi_gaga_ATLAS8_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a scalar resonance decaying to two photons. More... | |
| double | ip_ex_pp_phi_hh_bbbb_CMS8 (double mass) |
| Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to two bottom quark pairs. More... | |
| double | ip_ex_pp_phi_hh_bbbb_CMS8_e (double mass) |
| Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to two bottom quark pairs. More... | |
| double | ip_ex_pp_phi_hh_gagabb_CMS8 (double mass) |
| Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to a photon pair and a bottom quark pair. More... | |
| double | ip_ex_pp_phi_hh_gagabb_CMS8_e (double mass) |
| Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to a photon pair and a bottom quark pair. More... | |
| double | ip_ex_pp_phi_Zga_llga_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a scalar resonance decaying to a \(Z\) boson and a photon, of which the \(Z\) further decays to two leptons. More... | |
| double | ip_ex_pp_phi_Zga_llga_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a scalar resonance decaying to a \(Z\) boson and a photon, of which the \(Z\) further decays to two leptons. More... | |
| double | ip_ex_pp_phi_Zga_llga_ATLAS8 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a pseudoscalar resonance decaying to a Z boson and a photon which further decay into two leptons and a photon. More... | |
| double | ip_ex_pp_phi_Zga_llga_ATLAS8_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a pseudoscalar resonance decaying to a Z boson and a photon which further decay into two leptons and a photon. More... | |
| double | ip_ex_pp_phi_Zga_llga_CMS13 (double mass) |
| Interpolating function for the observed CMS upper limit on a scalar resonance decaying to a \(Z\) boson and a photon, of which the \(Z\) further decays to two leptons. More... | |
| double | ip_ex_pp_phi_Zga_llga_CMS13_e (double mass) |
| Interpolating function for the expected CMS upper limit on a scalar resonance decaying to a \(Z\) boson and a photon, of which the \(Z\) further decays to two leptons. More... | |
| double | ip_ex_pp_phi_Zga_qqga_CMS13 (double mass) |
| Interpolating function for the observed CMS upper limit on a scalar resonance decaying to a \(Z\) boson and a photon, of which the \(Z\) further decays to two quarks. More... | |
| double | ip_ex_pp_phi_Zga_qqga_CMS13_e (double mass) |
| Interpolating function for the expected CMS upper limit on a scalar resonance decaying to a \(Z\) boson and a photon, of which the \(Z\) further decays to two quarks. More... | |
| double | ip_ex_tt_phi_tt_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a tt associated scalar resonance decaying to t quarks. More... | |
| double | ip_ex_tt_phi_tt_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a tt associated scalar resonance decaying to t quarks. More... | |
| double | ip_ex_VBF_H_WW_ATLAS8 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a vector boson fusion produced scalar resonance decaying to two \(W\) bosons. More... | |
| double | ip_ex_VBF_H_WW_ATLAS8_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a vector boson fusion produced scalar resonance decaying to two \(W\) bosons. More... | |
| double | ip_ex_VBF_H_WW_enumunu_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a vector boson fusion produced scalar resonance decaying to two \(W\) bosons which further decay to two lepton-neutrino pairs. More... | |
| double | ip_ex_VBF_H_WW_enumunu_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a vector boson fusion produced scalar resonance decaying to two \(W\) bosons which further decay to two lepton-neutrino pairs. More... | |
| double | ip_ex_VBF_H_WW_lnuqq_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a VBF produced scalar resonance decaying to two \(W\) bosons which further decay to a lepton-neutrino pair and a pair of quarks. More... | |
| double | ip_ex_VBF_H_WW_lnuqq_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a VBF produced scalar resonance decaying to two \(W\) bosons which further decay to a lepton-neutrino pair and a pair of quarks. More... | |
| double | ip_ex_VBF_H_ZZ_ATLAS8 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a vector boson fusion produced scalar resonance decaying to two \(Z\) bosons. More... | |
| double | ip_ex_VBF_H_ZZ_ATLAS8_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a vector boson fusion produced scalar resonance decaying to two \(Z\) bosons. More... | |
| double | ip_ex_VBF_H_ZZ_llll_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a vector boson fusion produced scalar resonance decaying to two \(Z\) bosons which further decay to four leptons. More... | |
| double | ip_ex_VBF_H_ZZ_llll_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a vector boson fusion produced scalar resonance decaying to two \(Z\) bosons which further decay to four leptons. More... | |
| double | ip_ex_VBF_H_ZZ_llllnunu_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a VBF produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two neutrinos or two leptons. More... | |
| double | ip_ex_VBF_H_ZZ_llllnunu_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a VBF produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two neutrinos or two leptons. More... | |
| double | ip_ex_VBF_H_ZZ_llnunu_CMS13 (double mass) |
| Interpolating function for the observed CMS upper limit on a VBF produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two neutrinos. More... | |
| double | ip_ex_VBF_H_ZZ_llnunu_CMS13_e (double mass) |
| Interpolating function for the expected CMS upper limit on a VBF produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two neutrinos. More... | |
| double | ip_ex_VBF_H_ZZ_llqq_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a vector boson fusion produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two quarks. More... | |
| double | ip_ex_VBF_H_ZZ_llqq_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a vector boson fusion produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two quarks. More... | |
| double | ip_ex_VBF_H_ZZ_qqllnunu_ATLAS13 (double mass) |
| Interpolating function for the observed ATLAS upper limit on a VBF produced scalar resonance decaying to two \(Z\) bosons which further decay to two quarks and two neutrinos or two leptons. More... | |
| double | ip_ex_VBF_H_ZZ_qqllnunu_ATLAS13_e (double mass) |
| Interpolating function for the expected ATLAS upper limit on a VBF produced scalar resonance decaying to two \(Z\) bosons which further decay to two quarks and two neutrinos or two leptons. More... | |
| double | ip_ex_VBF_VH_H_ZZ_llll_CMS13 (double mass) |
| Interpolating function for the observed CMS upper limit on a vector boson fusion produced scalar resonance decaying to two \(Z\) bosons which further decay to four leptons. More... | |
| double | ip_ex_VBF_VH_H_ZZ_llll_CMS13_e (double mass) |
| Interpolating function for the expected CMS upper limit on a vector boson fusion produced scalar resonance decaying to two \(Z\) bosons which further decay to four leptons. More... | |
| double | ip_GammaHPtotSM (double mass) |
| Interpolating function for the total SM Higgs decay width. More... | |
| double | KaellenFunction (const double a2, const double b2, const double c2) const |
| Kaellen function. More... | |
| double | MWTHDM (const double MW) const |
| void | read () |
| Fills all required arrays with the values read from the tables. More... | |
| gslpp::matrix< double > | readTable (std::string filename, int rowN, int colN) |
| This function reads values from a table and returns them as an array. More... | |
| void | runTHDMparameters () |
| THDMcache (const StandardModel &SM_i) | |
| THDMcache constructor. More... | |
| double | updateCache () |
| ~THDMcache () | |
| THDMcache destructor. More... | |
Static Public Attributes | |
| static const int | CacheSize = 5 |
| Cache size. More... | |
Private Member Functions | |
| gslpp::complex | f_func (const double x) const |
| f function for the gamma gamma coupling to h, H and A More... | |
| gslpp::complex | g_func (const double x) const |
| g function for the Int1 function More... | |
| int | HSTheta (const double x) const |
| Heaviside \(\Theta\) function. More... | |
| gslpp::complex | Int1 (const double tau, const double lambda) const |
| \(I_1\) function for Z gamma coupling to h, H and A More... | |
| gslpp::complex | Int2 (const double tau, const double lambda) const |
| \(I_2\) function for Z gamma coupling to h, H and A More... | |
| THDMcache::THDMcache | ( | const StandardModel & | SM_i | ) |
THDMcache constructor.
Reads all the tables values and stores them in the memory.
| THDMcache::~THDMcache | ( | ) |
THDMcache destructor.
| gslpp::complex THDMcache::A_A_D | ( | const double | mA2, |
| const double | cW2, | ||
| const double | Ms, | ||
| const double | Mb, | ||
| const double | MZ | ||
| ) | const |
Amplitude for a CP-odd Higgs boson decay to a photon and a Z boson including the strange and bottom quarks in the loop.
This function can also be used for the gluon fusion production adding the appropriate factor
| gslpp::complex THDMcache::A_A_L | ( | const double | mA2, |
| const double | cW2, | ||
| const double | Mmu, | ||
| const double | Mtau, | ||
| const double | MZ | ||
| ) | const |
Amplitude for a CP-odd Higgs boson decay to a photon and a Z boson including muons and taus in the loop.
| gslpp::complex THDMcache::A_A_U | ( | const double | mA2, |
| const double | cW2, | ||
| const double | Mc, | ||
| const double | Mt, | ||
| const double | MZ | ||
| ) | const |
Amplitude for a CP-odd Higgs boson decay to a photon and a Z boson including the charm and top quarks in the loop.
| gslpp::complex THDMcache::A_h_D | ( | const double | mHl2, |
| const double | cW2, | ||
| const double | Md, | ||
| const double | Ms, | ||
| const double | Mb, | ||
| const double | MZ | ||
| ) | const |
Amplitude for the SM Higgs boson decay to a photon and a Z boson including the down-type quarks in the loop.
This function can also be used for the gluon fusion production adding the appropriate factor
| gslpp::complex THDMcache::A_H_Hp | ( | const double | mHp2, |
| const double | mH, | ||
| const double | cW2, | ||
| const double | MZ | ||
| ) | const |
Amplitude for a CP-even Higgs boson decay to a photon and a Z boson including the charged Higgs boson in the loop.
| gslpp::complex THDMcache::A_h_L | ( | const double | mHl2, |
| const double | cW2, | ||
| const double | Me, | ||
| const double | Mmu, | ||
| const double | Mtau, | ||
| const double | MZ | ||
| ) | const |
Amplitude for the SM Higgs boson decay to a photon and a Z boson including the leptons in the loop.
| gslpp::complex THDMcache::A_h_U | ( | const double | mHl2, |
| const double | cW2, | ||
| const double | Mu, | ||
| const double | Mc, | ||
| const double | Mt, | ||
| const double | MZ | ||
| ) | const |
Amplitude for the SM Higgs boson decay to a photon and a Z boson including the up-type quarks in the loop.
| gslpp::complex THDMcache::A_H_W | ( | const double | mH, |
| const double | cW2, | ||
| const double | MW, | ||
| const double | MZ | ||
| ) | const |
Amplitude for a CP-even Higgs boson decay to a photon and a Z boson including the W boson in the loop.
| gslpp::complex THDMcache::A_HH_D | ( | const double | mHh2, |
| const double | cW2, | ||
| const double | Ms, | ||
| const double | Mb, | ||
| const double | MZ | ||
| ) | const |
Amplitude for a heavy CP-even Higgs boson decay to a photon and a Z boson including the strange and bottom quarks in the loop.
| gslpp::complex THDMcache::A_HH_L | ( | const double | mHh2, |
| const double | cW2, | ||
| const double | Mmu, | ||
| const double | Mtau, | ||
| const double | MZ | ||
| ) | const |
Amplitude for a heavy CP-even Higgs boson decay to a photon and a Z boson including muons and taus in the loop.
| gslpp::complex THDMcache::A_HH_U | ( | const double | mHh2, |
| const double | cW2, | ||
| const double | Mc, | ||
| const double | Mt, | ||
| const double | MZ | ||
| ) | const |
Amplitude for a heavy CP-even Higgs boson decay to a photon and a Z boson including the charm and top quarks in the loop.
| gslpp::complex THDMcache::B00_MZ2_0_mA2_mHp2 | ( | const double | MZ2, |
| const double | mA2, | ||
| const double | mHp2 | ||
| ) | const |
\(B_{00}(0; mA2, mHp2)\).
For more details look at \(B_{00}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mA2,squared | CP-odd Higgs mass |
| [in] | mHp2,squared | charged Higgs mass |
| gslpp::complex THDMcache::B00_MZ2_0_mHh2_mA2 | ( | const double | MZ2, |
| const double | mHh2, | ||
| const double | mA2 | ||
| ) | const |
\(B_{00}(0; mHh2, mA2)\).
For more details look at \(B_{00}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| [in] | mA2,squared | CP-odd Higgs mass |
| gslpp::complex THDMcache::B00_MZ2_0_mHh2_mHp2 | ( | const double | MZ2, |
| const double | mHh2, | ||
| const double | mHp2 | ||
| ) | const |
\(B_{00}(0; mHh2, mHp2)\).
For more details look at \(B_{00}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| [in] | mHp2,squared | charged Higgs mass |
| gslpp::complex THDMcache::B00_MZ2_0_mHl2_mA2 | ( | const double | MZ2, |
| const double | mHl2, | ||
| const double | mA2 | ||
| ) | const |
\(B_{00}(0; mHl2, mA2)\).
For more details look at \(B_{00}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHl2,squared | mass of the Higgs boson |
| [in] | mA2,squared | CP-odd Higgs mass |
| gslpp::complex THDMcache::B00_MZ2_0_mHl2_mHp2 | ( | const double | MZ2, |
| const double | mHl2, | ||
| const double | mHp2 | ||
| ) | const |
\(B_{00}(0; mHl2, mHp2)\).
For more details look at \(B_{00}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHl2,squared | mass of the Higgs boson |
| [in] | mHp2,squared | charged Higgs mass |
| gslpp::complex THDMcache::B00_MZ2_0_mHp2_mHp2 | ( | const double | MZ2, |
| const double | mHp2 | ||
| ) | const |
\(B_{00}(0; mHl2, mHp2)\).
For more details look at \(B_{00}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHp2,squared | charged Higgs mass |
| gslpp::complex THDMcache::B00_MZ2_0_MW2_mHh2 | ( | const double | MZ2, |
| const double | MW2, | ||
| const double | mHh2 | ||
| ) | const |
\(B_{00}(0; MW2, mHh2)\).
For more details look at \(B_{00}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | MW2,the | W boson mass square |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B00_MZ2_0_MW2_mHl2 | ( | const double | MZ2, |
| const double | MW2, | ||
| const double | mHl2 | ||
| ) | const |
\(B_{00}(0; MW2, mHl2)\).
For more details look at \(B_{00}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | MW2,the | W boson mass square |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B00_MZ2_0_MZ2_mHh2 | ( | const double | MZ2, |
| const double | mHh2 | ||
| ) | const |
\(B_{00}(0; MZ2, mHh2)\).
For more details look at \(B_{00}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B00_MZ2_0_MZ2_mHl2 | ( | const double | MZ2, |
| const double | mHl2 | ||
| ) | const |
\(B_{00}(0; MZ2, mHl2)\).
For more details look at \(B_{00}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B00_MZ2_MW2_mA2_mHp2 | ( | const double | MZ2, |
| const double | MW2, | ||
| const double | mA2, | ||
| const double | mHp2 | ||
| ) | const |
\(B_{00}(MW2; mA2, mHp2)\).
For more details look at \(B_{00}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | MW2,the | W boson mass square |
| [in] | mA2,squared | CP-odd Higgs mass |
| [in] | mHp2,squared | charged Higgs mass |
| gslpp::complex THDMcache::B00_MZ2_MW2_mHh2_mHp2 | ( | const double | MZ2, |
| const double | MW2, | ||
| const double | mHh2, | ||
| const double | mHp2 | ||
| ) | const |
\(B_{00}(MW2; mHh2, mHp2)\).
For more details look at \(B_{00}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | MW2,the | W boson mass square |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| [in] | mHp2,squared | charged Higgs mass |
| gslpp::complex THDMcache::B00_MZ2_MW2_mHl2_mHp2 | ( | const double | MZ2, |
| const double | MW2, | ||
| const double | mHl2, | ||
| const double | mHp2 | ||
| ) | const |
\(B_{00}(MW2; mHl2, mHp2)\).
For more details look at \(B_{00}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | MW2,the | W boson mass square |
| [in] | mHl2,squared | mass of the Higgs boson |
| [in] | mHp2,squared | charged Higgs mass |
| gslpp::complex THDMcache::B00_MZ2_MW2_mHp2_mHp2 | ( | const double | MZ2, |
| const double | MW2, | ||
| const double | mHp2 | ||
| ) | const |
\(B_{00}(MW2; mHp2, mHp2)\).
For more details look at \(B_{00}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | MW2,the | W boson mass square |
| [in] | mHp2,squared | charged Higgs mass |
| gslpp::complex THDMcache::B00_MZ2_MW2_MW2_mHh2 | ( | const double | MZ2, |
| const double | MW2, | ||
| const double | mHh2 | ||
| ) | const |
\(B_{00}(MW2; MW2, mHh2)\).
For more details look at \(B_{00}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | MW2,the | W boson mass square |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B00_MZ2_MW2_MW2_mHl2 | ( | const double | MZ2, |
| const double | MW2, | ||
| const double | mHl2 | ||
| ) | const |
\(B_{00}(MW2; MW2, mHl2)\).
For more details look at \(B_{00}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | MW2,the | W boson mass square |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B00_MZ2_MZ2_mHh2_mA2 | ( | const double | MZ2, |
| const double | mHh2, | ||
| const double | mA2 | ||
| ) | const |
\(B_{00}(MZ2; mHh2, mA2)\).
For more details look at \(B_{00}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| [in] | mA2,squared | CP-odd Higgs mass |
| gslpp::complex THDMcache::B00_MZ2_MZ2_mHl2_mA2 | ( | const double | MZ2, |
| const double | mHl2, | ||
| const double | mA2 | ||
| ) | const |
\(B_{00}(MZ2; mHh2, mA2)\).
For more details look at \(B_{00}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHl2,squared | mass of the Higgs boson |
| [in] | mA2,squared | CP-odd Higgs mass |
| gslpp::complex THDMcache::B00_MZ2_MZ2_mHp2_mHp2 | ( | const double | MZ2, |
| const double | mHp2 | ||
| ) | const |
\(B_{00}(MZ2; mHp2, mHp2)\).
For more details look at \(B_{00}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHp2,squared | charged Higgs mass |
| gslpp::complex THDMcache::B00_MZ2_MZ2_MZ2_mHh2 | ( | const double | MZ2, |
| const double | mHh2 | ||
| ) | const |
\(B_{00}(MZ2; MZ2, mHh2)\).
For more details look at \(B_{00}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B00_MZ2_MZ2_MZ2_mHl2 | ( | const double | MZ2, |
| const double | mHl2 | ||
| ) | const |
\(B_{00}(MZ2; MZ2, mHl2)\).
For more details look at \(B_{00}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B0_MZ2_0_0_mHh2 | ( | const double | MZ2, |
| const double | mHh2 | ||
| ) | const |
\(B_0(0; 0, mHh2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B0_MZ2_0_0_mHl2 | ( | const double | MZ2, |
| const double | mHl2 | ||
| ) | const |
\(B_0(0; 0, mHl2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B0_MZ2_0_mA2_mHh2 | ( | const double | MZ2, |
| const double | mA2, | ||
| const double | mHh2 | ||
| ) | const |
\(B_0(0; mA2, mHh2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mA2,squared | CP-odd Higgs mass |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B0_MZ2_0_mA2_mHl2 | ( | const double | MZ2, |
| const double | mA2, | ||
| const double | mHl2 | ||
| ) | const |
\(B_0(0; mA2, mHl2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mA2,squared | CP-odd Higgs mass |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B0_MZ2_0_mHp2_mHh2 | ( | const double | MZ2, |
| const double | mHp2, | ||
| const double | mHh2 | ||
| ) | const |
\(B_0(0; mHp2, mHh2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHp2,squared | charged Higgs mass |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B0_MZ2_0_mHp2_mHl2 | ( | const double | MZ2, |
| const double | mHp2, | ||
| const double | mHl2 | ||
| ) | const |
\(B_0(0; mHp2, mHl2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHp2,squared | charged Higgs mass |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B0_MZ2_0_MW2_mHh2 | ( | const double | MZ2, |
| const double | MW2, | ||
| const double | mHh2 | ||
| ) | const |
\(B_0(0; MW2, mHh2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| [in] | MW2,the | W boson mass square |
| gslpp::complex THDMcache::B0_MZ2_0_MW2_mHl2 | ( | const double | MZ2, |
| const double | MW2, | ||
| const double | mHl2 | ||
| ) | const |
\(B_0(0; MW2, mHl2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHl2,squared | mass of the Higgs boson |
| [in] | MW2,the | W boson mass square |
| gslpp::complex THDMcache::B0_MZ2_0_MZ2_mHh2 | ( | const double | MZ2, |
| const double | mHh2 | ||
| ) | const |
\(B_0(0; MZ2, mHh2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) and the \( m_0^2 \) of \(B_0(p^2; m_0^2, m_1^2)\) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B0_MZ2_0_MZ2_mHl2 | ( | const double | MZ2, |
| const double | mHl2 | ||
| ) | const |
\(B_0(0; MZ2, mHl2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) and the \( m_0^2 \) of \(B_0(p^2; m_0^2, m_1^2)\) |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B0_MZ2_mA2_0_mHh2 | ( | const double | MZ2, |
| const double | mA2, | ||
| const double | mHh2 | ||
| ) | const |
\(B_0(mA2; 0, mHh2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mA2,squared | CP-odd Higgs mass |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B0_MZ2_mA2_0_mHl2 | ( | const double | MZ2, |
| const double | mA2, | ||
| const double | mHl2 | ||
| ) | const |
\(B_0(mA2; 0, mHl2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mA2,squared | CP-odd Higgs mass |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B0_MZ2_mA2_mA2_mHh2 | ( | const double | MZ2, |
| const double | mA2, | ||
| const double | mHh2 | ||
| ) | const |
\(B_0(mA2; mA2, mHh2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mA2,squared | CP-odd Higgs mass |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B0_MZ2_mA2_mA2_mHl2 | ( | const double | MZ2, |
| const double | mA2, | ||
| const double | mHl2 | ||
| ) | const |
\(B_0(mA2; mA2, mHl2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mA2,squared | CP-odd Higgs mass |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B0_MZ2_mHh2_0_0 | ( | const double | MZ2, |
| const double | mHh2 | ||
| ) | const |
\(B_0(mHh2; 0, 0)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B0_MZ2_mHh2_0_mA2 | ( | const double | MZ2, |
| const double | mHh2, | ||
| const double | mA2 | ||
| ) | const |
\(B_0(mHh2; 0, mA2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| [in] | mA2,squared | CP-odd Higgs mass |
| gslpp::complex THDMcache::B0_MZ2_mHh2_0_mHp2 | ( | const double | MZ2, |
| const double | mHh2, | ||
| const double | mHp2 | ||
| ) | const |
\(B_0(mHh2; 0, mHp2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| [in] | mHp2,squared | charged Higgs mass |
| gslpp::complex THDMcache::B0_MZ2_mHh2_mA2_mA2 | ( | const double | MZ2, |
| const double | mHh2, | ||
| const double | mA2 | ||
| ) | const |
\(B_0(mHh2; mA2, mA2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| [in] | mA2,squared | CP-odd Higgs mass |
| gslpp::complex THDMcache::B0_MZ2_mHh2_mHh2_mHh2 | ( | const double | MZ2, |
| const double | mHh2 | ||
| ) | const |
\(B_0(mHh2; mHh2, mHh2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B0_MZ2_mHh2_mHh2_mHl2 | ( | const double | MZ2, |
| const double | mHh2, | ||
| const double | mHl2 | ||
| ) | const |
\(B_0(mHh2; mHh2, mHl2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B0_MZ2_mHh2_mHl2_mHl2 | ( | const double | MZ2, |
| const double | mHh2, | ||
| const double | mHl2 | ||
| ) | const |
\(B_0(mHh2; mHl2, mHl2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B0_MZ2_mHh2_mHp2_mHp2 | ( | const double | MZ2, |
| const double | mHh2, | ||
| const double | mHp2 | ||
| ) | const |
\(B_0(mHh2; mHp2, mHp2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| [in] | mHp2,squared | charged Higgs mass |
| gslpp::complex THDMcache::B0_MZ2_mHl2_0_0 | ( | const double | MZ2, |
| const double | mHl2 | ||
| ) | const |
\(B_0(mHl2; 0, 0)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B0_MZ2_mHl2_0_mA2 | ( | const double | MZ2, |
| const double | mHl2, | ||
| const double | mA2 | ||
| ) | const |
\(B_0(mHl2; 0, mHp2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHl2,squared | mass of the Higgs boson |
| [in] | mA2,squared | CP-odd Higgs mass |
| gslpp::complex THDMcache::B0_MZ2_mHl2_0_mHp2 | ( | const double | MZ2, |
| const double | mHl2, | ||
| const double | mHp2 | ||
| ) | const |
\(B_0(mHl2; 0, mHp2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHl2,squared | mass of the Higgs boson |
| [in] | mHp2,squared | charged Higgs mass |
| gslpp::complex THDMcache::B0_MZ2_mHl2_mA2_mA2 | ( | const double | MZ2, |
| const double | mHl2, | ||
| const double | mA2 | ||
| ) | const |
\(B_0(mHl2; mA2, mA2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHl2,squared | mass of the Higgs boson |
| [in] | mA2,squared | CP-odd Higgs mass |
| gslpp::complex THDMcache::B0_MZ2_mHl2_mHh2_mHh2 | ( | const double | MZ2, |
| const double | mHl2, | ||
| const double | mHh2 | ||
| ) | const |
\(B_0(mHl2; mHh2, mHh2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHl2,squared | mass of the Higgs boson |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B0_MZ2_mHl2_mHh2_mHl2 | ( | const double | MZ2, |
| const double | mHl2, | ||
| const double | mHh2 | ||
| ) | const |
\(B_0(mHl2; mHh2, mHl2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHl2,squared | mass of the Higgs boson |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B0_MZ2_mHl2_mHl2_mHl2 | ( | const double | MZ2, |
| const double | mHl2 | ||
| ) | const |
\(B_0(mHl2; mHl2, mHl2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B0_MZ2_mHl2_mHp2_mHp2 | ( | const double | MZ2, |
| const double | mHl2, | ||
| const double | mHp2 | ||
| ) | const |
\(B_0(mHl2; mHp2, mHp2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHl2,squared | mass of the Higgs boson |
| [in] | mHp2,squared | charged Higgs mass |
| gslpp::complex THDMcache::B0_MZ2_mHp2_0_mHh2 | ( | const double | MZ2, |
| const double | mHp2, | ||
| const double | mHh2 | ||
| ) | const |
\(B_0(mHp2; 0, mHh2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHp2,squared | charged Higgs mass |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B0_MZ2_mHp2_0_mHl2 | ( | const double | MZ2, |
| const double | mHp2, | ||
| const double | mHl2 | ||
| ) | const |
\(B_0(mHp2; 0, mHl2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHp2,squared | charged Higgs mass |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B0_MZ2_mHp2_mHp2_mHh2 | ( | const double | MZ2, |
| const double | mHp2, | ||
| const double | mHh2 | ||
| ) | const |
\(B_0(mHp2; mHp2, mHh2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHp2,squared | charged Higgs mass |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B0_MZ2_mHp2_mHp2_mHl2 | ( | const double | MZ2, |
| const double | mHp2, | ||
| const double | mHl2 | ||
| ) | const |
\(B_0(mHp2; mHp2, mHl2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | mHp2,squared | charged Higgs mass |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B0_MZ2_MW2_MW2_mHh2 | ( | const double | MZ2, |
| const double | MW2, | ||
| const double | mHh2 | ||
| ) | const |
\(B_0(MW2; MW2, mHh2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | MW2,squared | mass of the Higgs boson |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B0_MZ2_MW2_MW2_mHl2 | ( | const double | MZ2, |
| const double | MW2, | ||
| const double | mHl2 | ||
| ) | const |
\(B_0(MW2; MW2, mHl2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) |
| [in] | MW2,squared | mass of the Higgs boson |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B0_MZ2_MZ2_MZ2_mHh2 | ( | const double | MZ2, |
| const double | mHh2 | ||
| ) | const |
\(B_0(MZ2; MZ2, mHh2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) and the \( p^2 \) and \( m_0^2 \) of \(B_0(p^2; m_0^2, m_1^2)\) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B0_MZ2_MZ2_MZ2_mHl2 | ( | const double | MZ2, |
| const double | mHl2 | ||
| ) | const |
\(B_0(MZ2; MZ2, mHl2)\).
For more details look at \(B_0(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared (the Z boson mass) and the \( p^2 \) and \( m_0^2 \) of \(B_0(p^2; m_0^2, m_1^2)\) |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B0p_MZ2_0_0_mHh2 | ( | const double | MZ2, |
| const double | mHh2 | ||
| ) | const |
\(B_{0p}(0; 0, mHh2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B0p_MZ2_0_0_mHl2 | ( | const double | MZ2, |
| const double | mHl2 | ||
| ) | const |
\(B_{0p}(0; 0, mHl2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B0p_MZ2_0_mA2_mHh2 | ( | const double | MZ2, |
| const double | mA2, | ||
| const double | mHh2 | ||
| ) | const |
\(B_{0p}(0; mA2, mHh2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mA2,squared | CP-odd Higgs mass |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B0p_MZ2_0_mA2_mHl2 | ( | const double | MZ2, |
| const double | mA2, | ||
| const double | mHl2 | ||
| ) | const |
\(B_{0p}(0; mA2, mHl2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mA2,squared | CP-odd Higgs mass |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B0p_MZ2_0_mHp2_mA2 | ( | const double | MZ2, |
| const double | mHp2, | ||
| const double | mA2 | ||
| ) | const |
\(B_{0p}(0; mHp2, mHA2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHp2,squared | charged Higgs mass |
| [in] | mA2,squared | CP-odd Higgs mass |
| gslpp::complex THDMcache::B0p_MZ2_0_mHp2_mHh2 | ( | const double | MZ2, |
| const double | mHp2, | ||
| const double | mHh2 | ||
| ) | const |
\(B_{0p}(0; mHp2, mHh2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHp2,squared | charged Higgs mass |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B0p_MZ2_0_mHp2_mHl2 | ( | const double | MZ2, |
| const double | mHp2, | ||
| const double | mHl2 | ||
| ) | const |
\(B_{0p}(0; mHp2, mHl2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHp2,squared | charged Higgs mass |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B0p_MZ2_mA2_0_mHh2 | ( | const double | MZ2, |
| const double | mA2, | ||
| const double | mHh2 | ||
| ) | const |
\(B_{0p}(mA2; 0, mHh2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mA2,squared | CP-odd Higgs mass |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B0p_MZ2_mA2_0_mHl2 | ( | const double | MZ2, |
| const double | mA2, | ||
| const double | mHl2 | ||
| ) | const |
\(B_{0p}(mA2; 0, mHl2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mA2,squared | CP-odd Higgs mass |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B0p_MZ2_mA2_0_mHp2 | ( | const double | MZ2, |
| const double | mA2, | ||
| const double | mHp2 | ||
| ) | const |
\(B_{0p}(mA2; 0, mHp2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mA2,squared | CP-odd Higgs mass |
| [in] | mHp2,squared | charged Higgs mass |
| gslpp::complex THDMcache::B0p_MZ2_mA2_mA2_mHh2 | ( | const double | MZ2, |
| const double | mA2, | ||
| const double | mHh2 | ||
| ) | const |
\(B_{0p}(mA2; mA2, mHh2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mA2,squared | CP-odd Higgs mass |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B0p_MZ2_mA2_mA2_mHl2 | ( | const double | MZ2, |
| const double | mA2, | ||
| const double | mHl2 | ||
| ) | const |
\(B_{0p}(mA2; mA2, mHl2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mA2,squared | CP-odd Higgs mass |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B0p_MZ2_mHh2_0_0 | ( | const double | MZ2, |
| const double | mHh2 | ||
| ) | const |
\(B_{0p}(mHh2; 0, 0)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B0p_MZ2_mHh2_0_mA2 | ( | const double | MZ2, |
| const double | mHh2, | ||
| const double | mA2 | ||
| ) | const |
\(B_{0p}(mHh2; 0, mA2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| [in] | mA2,squared | CP-odd Higgs mass |
| gslpp::complex THDMcache::B0p_MZ2_mHh2_0_mHp2 | ( | const double | MZ2, |
| const double | mHh2, | ||
| const double | mHp2 | ||
| ) | const |
\(B_{0p}(mHh2; 0, mHp2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| [in] | mHp2,squared | charged Higgs mass |
| gslpp::complex THDMcache::B0p_MZ2_mHh2_mA2_mA2 | ( | const double | MZ2, |
| const double | mHh2, | ||
| const double | mA2 | ||
| ) | const |
\(B_{0p}(mHh2; mA2, mA2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| [in] | mA2,squared | CP-odd Higgs mass |
| gslpp::complex THDMcache::B0p_MZ2_mHh2_mHh2_mHh2 | ( | const double | MZ2, |
| const double | mHh2 | ||
| ) | const |
\(B_{0p}(mHh2; mHh2, mHh2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B0p_MZ2_mHh2_mHh2_mHl2 | ( | const double | MZ2, |
| const double | mHh2, | ||
| const double | mHl2 | ||
| ) | const |
\(B_{0p}(mHh2; mHh2, mHl2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B0p_MZ2_mHh2_mHl2_mHl2 | ( | const double | MZ2, |
| const double | mHh2, | ||
| const double | mHl2 | ||
| ) | const |
\(B_{0p}(mHh2; mHl2, mHl2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B0p_MZ2_mHh2_mHp2_mHp2 | ( | const double | MZ2, |
| const double | mHh2, | ||
| const double | mHp2 | ||
| ) | const |
\(B_{0p}(mHh2; mHp2, mHp2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| [in] | mHp2,squared | charged Higgs mass |
| gslpp::complex THDMcache::B0p_MZ2_mHl2_0_0 | ( | const double | MZ2, |
| const double | mHl2 | ||
| ) | const |
\(B_{0p}(mHl2; 0, 0)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B0p_MZ2_mHl2_0_mA2 | ( | const double | MZ2, |
| const double | mHl2, | ||
| const double | mA2 | ||
| ) | const |
\(B_{0p}(mHl2; 0, mHp2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHl2,squared | mass of the Higgs boson |
| [in] | mA2,squared | CP-odd Higgs mass |
| gslpp::complex THDMcache::B0p_MZ2_mHl2_0_mHp2 | ( | const double | MZ2, |
| const double | mHl2, | ||
| const double | mHp2 | ||
| ) | const |
\(B_{0p}(mHl2; 0, mHp2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHl2,squared | mass of the Higgs boson |
| [in] | mHp2,squared | charged Higgs mass |
| gslpp::complex THDMcache::B0p_MZ2_mHl2_mA2_mA2 | ( | const double | MZ2, |
| const double | mHl2, | ||
| const double | mA2 | ||
| ) | const |
\(B_{0p}(mHl2; mA2, mA2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHl2,squared | mass of the Higgs boson |
| [in] | mA2,squared | CP-odd Higgs mass |
| gslpp::complex THDMcache::B0p_MZ2_mHl2_mHh2_mHh2 | ( | const double | MZ2, |
| const double | mHl2, | ||
| const double | mHh2 | ||
| ) | const |
\(B_{0p}(mHl2; mHh2, mHh2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHl2,squared | mass of the Higgs boson |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B0p_MZ2_mHl2_mHh2_mHl2 | ( | const double | MZ2, |
| const double | mHl2, | ||
| const double | mHh2 | ||
| ) | const |
\(B_{0p}(mHl2; mHh2, mHl2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHl2,squared | mass of the Higgs boson |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B0p_MZ2_mHl2_mHl2_mHl2 | ( | const double | MZ2, |
| const double | mHl2 | ||
| ) | const |
\(B_{0p}(mHl2; mHl2, mHl2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B0p_MZ2_mHl2_mHp2_mHp2 | ( | const double | MZ2, |
| const double | mHl2, | ||
| const double | mHp2 | ||
| ) | const |
\(B_{0p}(mHl2; mHp2, mHp2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHl2,squared | mass of the Higgs boson |
| [in] | mHp2,squared | charged Higgs mass |
| gslpp::complex THDMcache::B0p_MZ2_mHp2_0_mA2 | ( | const double | MZ2, |
| const double | mHp2, | ||
| const double | mA2 | ||
| ) | const |
\(B_{0p}(mHp2; 0, mHA2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHp2,squared | charged Higgs mass |
| [in] | mA2,squared | CP-odd Higgs mass |
| gslpp::complex THDMcache::B0p_MZ2_mHp2_0_mHh2 | ( | const double | MZ2, |
| const double | mHp2, | ||
| const double | mHh2 | ||
| ) | const |
\(B_{0p}(mHp2; 0, mHh2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHp2,squared | charged Higgs mass |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B0p_MZ2_mHp2_0_mHl2 | ( | const double | MZ2, |
| const double | mHp2, | ||
| const double | mHl2 | ||
| ) | const |
\(B_{0p}(mHp2; 0, mHl2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHp2,squared | charged Higgs mass |
| [in] | mHl2,squared | mass of the Higgs boson |
| gslpp::complex THDMcache::B0p_MZ2_mHp2_mHp2_mHh2 | ( | const double | MZ2, |
| const double | mHp2, | ||
| const double | mHh2 | ||
| ) | const |
\(B_{0p}(mHp2; mHp2, mHh2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHp2,squared | charged Higgs mass |
| [in] | mHh2,squared | mass of the "non-125 GeV" neutral scalar Higgs |
| gslpp::complex THDMcache::B0p_MZ2_mHp2_mHp2_mHl2 | ( | const double | MZ2, |
| const double | mHp2, | ||
| const double | mHl2 | ||
| ) | const |
\(B_{0p}(mHp2; mHp2, mHl2)\).
For more details look at \(B_{0p}(p^2; m_0^2, m_1^2)\) in PVfunctions.h
| [in] | MZ2 | the renormalization scale squared for the IR divergence (the Z boson mass) |
| [in] | mHp2,squared | charged Higgs mass |
| [in] | mHl2,squared | mass of the Higgs boson |
| int THDMcache::CacheCheck | ( | const gslpp::complex | cache[][CacheSize], |
| const int | NumPar, | ||
| const double | params[] | ||
| ) | const |
Check whether for the latest set of parameters a value is in the cache.
Takes a complex value.
| int THDMcache::CacheCheckReal | ( | const double | cache[][CacheSize], |
| const int | NumPar, | ||
| const double | params[] | ||
| ) | const |
Check whether for the latest set of parameters a value is in the cache.
Takes a real value.
| void THDMcache::CacheShift | ( | gslpp::complex | cache[][CacheSize], |
| const int | NumPar, | ||
| const double | params[], | ||
| const gslpp::complex | newResult | ||
| ) | const |
Adds a new result and its parameters into the cache.
The new values are added on top. The oldest set on the stack is deleted. Takes a complex value.
| void THDMcache::CacheShiftReal | ( | double | cache[][CacheSize], |
| const int | NumPar, | ||
| const double | params[], | ||
| const double | newResult | ||
| ) | const |
Adds a new result and its parameters into the cache.
The new values are added on top. The oldest set on the stack is deleted. Takes a real value.
| void THDMcache::computeAlimits | ( | ) |
| void THDMcache::computeAquantities | ( | ) |
| void THDMcache::computeHHlimits | ( | ) |
| void THDMcache::computeHHquantities | ( | ) |
| void THDMcache::computeHpquantities | ( | ) |
| void THDMcache::computeSignalStrengthQuantities | ( | ) |
| void THDMcache::computeWFRcombinations | ( | ) |
| double THDMcache::cW2THDM | ( | const double | c02 | ) | const |
|
private |
f function for the gamma gamma coupling to h, H and A
The definition can be found in (2.19) of [134].
|
private |
| double THDMcache::g_HH_HpHm | ( | const double | mHp2, |
| const double | mHh2, | ||
| const double | tanb, | ||
| const double | m12_2, | ||
| const double | bma, | ||
| const double | vev | ||
| ) | const |
|
inline |
Definition at line 81 of file THDMcache.h.
| double THDMcache::ghHpHm | ( | const double | mHp2, |
| const double | tanb, | ||
| const double | m12_2, | ||
| const double | bma, | ||
| const double | mHl2, | ||
| const double | vev | ||
| ) | const |
|
private |
Heaviside \(\Theta\) function.
Gives 1 for \(x\geq 0\) and 0 for \(x<0\).
| gslpp::complex THDMcache::I_A_D | ( | const double | mA2, |
| const double | Ms, | ||
| const double | Mb | ||
| ) | const |
Amplitude for a CP-odd Higgs boson decay to diphotons including the strange and bottom quarks in the loop.
This function can also be used for the gluon fusion production adding the appropriate factor
| gslpp::complex THDMcache::I_A_L | ( | const double | mA2, |
| const double | Mmu, | ||
| const double | Mtau | ||
| ) | const |
Amplitude for a CP-odd Higgs boson decay to diphotons including muons and taus in the loop.
| gslpp::complex THDMcache::I_A_U | ( | const double | mA2, |
| const double | Mc, | ||
| const double | Mt | ||
| ) | const |
Amplitude for a CP-odd Higgs boson decay to diphotons including the charm and top quarks in the loop.
This function can also be used for the gluon fusion production adding the appropriate factor
| gslpp::complex THDMcache::I_h_D | ( | const double | mHl2, |
| const double | Md, | ||
| const double | Ms, | ||
| const double | Mb | ||
| ) | const |
Amplitude for the SM Higgs boson decay to diphotons including the down-type quarks in the loop.
This function can also be used for the gluon fusion production adding the appropriate factor
| gslpp::complex THDMcache::I_H_Hp | ( | const double | mHp2, |
| const double | mH | ||
| ) | const |
Amplitude for a CP-even Higgs boson decay to diphotons including the charged Higgs boson in the loop.
| gslpp::complex THDMcache::I_h_L | ( | const double | mHl2, |
| const double | Me, | ||
| const double | Mmu, | ||
| const double | Mtau | ||
| ) | const |
Amplitude for the SM Higgs boson decay to diphotons including the leptons in the loop.
| gslpp::complex THDMcache::I_h_U | ( | const double | mHl2, |
| const double | Mu, | ||
| const double | Mc, | ||
| const double | Mt | ||
| ) | const |
Amplitude for the SM Higgs boson decay to diphotons including the up-type quarks in the loop.
This function can also be used for the gluon fusion production adding the appropriate factor
| gslpp::complex THDMcache::I_H_W | ( | const double | mH, |
| const double | MW | ||
| ) | const |
Amplitude for a CP-even Higgs boson decay to diphotons including the W boson in the loop.
| gslpp::complex THDMcache::I_HH_D | ( | const double | mHh2, |
| const double | Ms, | ||
| const double | Mb | ||
| ) | const |
Amplitude for a heavy CP-even Higgs boson decay to diphotons including the strange and bottom quarks in the loop.
This function can also be used for the gluon fusion production adding the appropriate factor
| gslpp::complex THDMcache::I_HH_L | ( | const double | mHh2, |
| const double | Mmu, | ||
| const double | Mtau | ||
| ) | const |
Amplitude for a heavy CP-even Higgs boson decay to diphotons including muons and taus in the loop.
| gslpp::complex THDMcache::I_HH_U | ( | const double | mHh2, |
| const double | Mc, | ||
| const double | Mt | ||
| ) | const |
Amplitude for a heavy CP-even Higgs boson decay to diphotons including the charm and top quarks in the loop.
This function can also be used for the gluon fusion production adding the appropriate factor
| double THDMcache::ie1 | ( | double | mass | ) |
| double THDMcache::ie10 | ( | double | mass | ) |
| double THDMcache::ie10e | ( | double | mass | ) |
| double THDMcache::ie11 | ( | double | mass | ) |
| double THDMcache::ie11e | ( | double | mass | ) |
| double THDMcache::ie12 | ( | double | mass | ) |
| double THDMcache::ie12e | ( | double | mass | ) |
| double THDMcache::ie13 | ( | double | mass | ) |
| double THDMcache::ie13e | ( | double | mass | ) |
| double THDMcache::ie14 | ( | double | mass | ) |
| double THDMcache::ie14e | ( | double | mass | ) |
| double THDMcache::ie15 | ( | double | mass | ) |
| double THDMcache::ie15e | ( | double | mass | ) |
| double THDMcache::ie16 | ( | double | mass | ) |
| double THDMcache::ie16e | ( | double | mass | ) |
| double THDMcache::ie17 | ( | double | mass | ) |
| double THDMcache::ie17e | ( | double | mass | ) |
| double THDMcache::ie18 | ( | double | mass | ) |
| double THDMcache::ie18e | ( | double | mass | ) |
| double THDMcache::ie19 | ( | double | mass | ) |
| double THDMcache::ie19e | ( | double | mass | ) |
| double THDMcache::ie1e | ( | double | mass | ) |
| double THDMcache::ie2 | ( | double | mass | ) |
| double THDMcache::ie20 | ( | double | mass | ) |
| double THDMcache::ie20e | ( | double | mass | ) |
| double THDMcache::ie21 | ( | double | mass | ) |
| double THDMcache::ie21e | ( | double | mass | ) |
| double THDMcache::ie22 | ( | double | mass | ) |
| double THDMcache::ie22e | ( | double | mass | ) |
| double THDMcache::ie23 | ( | double | mass | ) |
| double THDMcache::ie23e | ( | double | mass | ) |
| double THDMcache::ie24 | ( | double | mass | ) |
| double THDMcache::ie24e | ( | double | mass | ) |
| double THDMcache::ie25 | ( | double | mass | ) |
| double THDMcache::ie25e | ( | double | mass | ) |
| double THDMcache::ie26 | ( | double | mass | ) |
| double THDMcache::ie26e | ( | double | mass | ) |
| double THDMcache::ie27 | ( | double | mass | ) |
| double THDMcache::ie27e | ( | double | mass | ) |
| double THDMcache::ie28 | ( | double | mass | ) |
| double THDMcache::ie28e | ( | double | mass | ) |
| double THDMcache::ie29 | ( | double | mass | ) |
| double THDMcache::ie29e | ( | double | mass | ) |
| double THDMcache::ie2e | ( | double | mass | ) |
| double THDMcache::ie3 | ( | double | mass | ) |
| double THDMcache::ie30 | ( | double | mass | ) |
| double THDMcache::ie30e | ( | double | mass | ) |
| double THDMcache::ie31 | ( | double | mass | ) |
| double THDMcache::ie31e | ( | double | mass | ) |
| double THDMcache::ie32 | ( | double | mass | ) |
| double THDMcache::ie32e | ( | double | mass | ) |
| double THDMcache::ie33 | ( | double | mass | ) |
| double THDMcache::ie33e | ( | double | mass | ) |
| double THDMcache::ie34 | ( | double | mass | ) |
| double THDMcache::ie34e | ( | double | mass | ) |
| double THDMcache::ie35 | ( | double | mass | ) |
| double THDMcache::ie35e | ( | double | mass | ) |
| double THDMcache::ie36 | ( | double | mass | ) |
| double THDMcache::ie36e | ( | double | mass | ) |
| double THDMcache::ie37 | ( | double | mass | ) |
| double THDMcache::ie37e | ( | double | mass | ) |
| double THDMcache::ie38 | ( | double | mass | ) |
| double THDMcache::ie38e | ( | double | mass | ) |
| double THDMcache::ie39 | ( | double | mass | ) |
| double THDMcache::ie39e | ( | double | mass | ) |
| double THDMcache::ie3e | ( | double | mass | ) |
| double THDMcache::ie4 | ( | double | mass | ) |
| double THDMcache::ie40 | ( | double | mass | ) |
| double THDMcache::ie40e | ( | double | mass | ) |
| double THDMcache::ie4e | ( | double | mass | ) |
| double THDMcache::ie5 | ( | double | mass | ) |
| double THDMcache::ie5e | ( | double | mass | ) |
| double THDMcache::ie6 | ( | double | mass | ) |
| double THDMcache::ie6e | ( | double | mass | ) |
| double THDMcache::ie7 | ( | double | mass | ) |
| double THDMcache::ie7e | ( | double | mass | ) |
| double THDMcache::ie8 | ( | double | mass | ) |
| double THDMcache::ie8e | ( | double | mass | ) |
| double THDMcache::ie9 | ( | double | mass | ) |
| double THDMcache::ie9e | ( | double | mass | ) |
|
private |
\(I_1\) function for Z gamma coupling to h, H and A
The definition can be found in (2.24) of [134].
|
private |
\(I_2\) function for Z gamma coupling to h, H and A
The definition can be found in (2.24) of [134].
| double THDMcache::interpolate | ( | gslpp::matrix< double > | arrayTab, |
| double | x | ||
| ) |
Linearly interpolates a table with one parameter dimension.
| double THDMcache::interpolate2D | ( | gslpp::matrix< double > | arrayTab, |
| double | x, | ||
| double | y | ||
| ) |
Linearly interpolates a table with two parameter dimensions.
| double THDMcache::ip_Br_HPtobb | ( | double | mass | ) |
Interpolating function for the SM branching ratio to two bottom quarks.
| double THDMcache::ip_Br_HPtocc | ( | double | mass | ) |
Interpolating function for the SM branching ratio to two charm quarks.
| double THDMcache::ip_Br_HPtomumu | ( | double | mass | ) |
Interpolating function for the SM branching ratio to two muons.
| double THDMcache::ip_Br_HPtotautau | ( | double | mass | ) |
Interpolating function for the SM branching ratio to two tau leptons.
| double THDMcache::ip_Br_HPtott | ( | double | mass | ) |
Interpolating function for the SM branching ratio to two top quarks.
| double THDMcache::ip_Br_HPtoWW | ( | double | mass | ) |
Interpolating function for the SM branching ratio to two \(W\) bosons.
| double THDMcache::ip_Br_HPtoZZ | ( | double | mass | ) |
Interpolating function for the SM branching ratio to two \(Z\) bosons.
| double THDMcache::ip_cs_ggtoA_13 | ( | double | mass | ) |
Interpolating function for the A production cross section via gluon-gluon fusion at 13 TeV.
| double THDMcache::ip_cs_ggtoA_8 | ( | double | mass | ) |
Interpolating function for the A production cross section via gluon-gluon fusion at 8 TeV.
| double THDMcache::ip_cs_ggtoH_13 | ( | double | mass | ) |
Interpolating function for the H production cross section via gluon-gluon fusion at 13 TeV.
| double THDMcache::ip_cs_ggtoH_8 | ( | double | mass | ) |
Interpolating function for the H production cross section via gluon-gluon fusion at 8 TeV.
| double THDMcache::ip_cs_ggtoHp_13 | ( | double | mHp, |
| double | logtb | ||
| ) |
Interpolating function for the H+ production cross section from two gluons at 13 TeV.
| double THDMcache::ip_cs_ggtoHp_8 | ( | double | mHp, |
| double | logtb | ||
| ) |
Interpolating function for the H+ production cross section from two gluons at 8 TeV.
| double THDMcache::ip_cs_pptobbA_13 | ( | double | mass | ) |
Interpolating function for the bottom associated A production cross section at 13 TeV.
| double THDMcache::ip_cs_pptobbA_8 | ( | double | mass | ) |
Interpolating function for the bottom associated A production cross section at 8 TeV.
| double THDMcache::ip_cs_pptobbH_13 | ( | double | mass | ) |
Interpolating function for the bottom associated H production cross section at 13 TeV.
| double THDMcache::ip_cs_pptobbH_8 | ( | double | mass | ) |
Interpolating function for the bottom associated H production cross section at 8 TeV.
| double THDMcache::ip_cs_pptottA_13 | ( | double | mass | ) |
Interpolating function for the top associated A production cross section at 13 TeV.
| double THDMcache::ip_cs_pptottA_8 | ( | double | mass | ) |
Interpolating function for the top associated A production cross section at 8 TeV.
| double THDMcache::ip_cs_pptottH_13 | ( | double | mass | ) |
Interpolating function for the top associated H production cross section at 13 TeV.
| double THDMcache::ip_cs_pptottH_8 | ( | double | mass | ) |
Interpolating function for the top associated H production cross section at 8 TeV.
| double THDMcache::ip_cs_VBFtoH_13 | ( | double | mass | ) |
Interpolating function for the H production cross section via vector boson fusion at 13 TeV.
| double THDMcache::ip_cs_VBFtoH_8 | ( | double | mass | ) |
Interpolating function for the H production cross section via vector boson fusion at 8 TeV.
| double THDMcache::ip_cs_WtoWH_13 | ( | double | mass | ) |
Interpolating function for the W associated H production cross section at 13 TeV.
| double THDMcache::ip_cs_WtoWH_8 | ( | double | mass | ) |
Interpolating function for the W associated H production cross section at 8 TeV.
| double THDMcache::ip_cs_ZtoZH_13 | ( | double | mass | ) |
Interpolating function for the Z associated H production cross section at 13 TeV.
| double THDMcache::ip_cs_ZtoZH_8 | ( | double | mass | ) |
Interpolating function for the Z associated H production cross section at 8 TeV.
| double THDMcache::ip_csr_ggA_b_13 | ( | double | mass | ) |
Interpolating function for the gluon-gluon fusion A cross section ratio of the bottom-loop and the total contribution at 13 TeV.
| double THDMcache::ip_csr_ggA_b_8 | ( | double | mass | ) |
Interpolating function for the gluon-gluon fusion A cross section ratio of the bottom-loop and the total contribution at 8 TeV.
| double THDMcache::ip_csr_ggA_t_13 | ( | double | mass | ) |
Interpolating function for the gluon-gluon fusion A cross section ratio of the top-loop and the total contribution at 13 TeV.
| double THDMcache::ip_csr_ggA_t_8 | ( | double | mass | ) |
Interpolating function for the gluon-gluon fusion A cross section ratio of the top-loop and the total contribution at 8 TeV.
| double THDMcache::ip_csr_ggH_b_13 | ( | double | mass | ) |
Interpolating function for the gluon-gluon fusion H cross section ratio of the bottom-loop and the total contribution at 13 TeV.
| double THDMcache::ip_csr_ggH_b_8 | ( | double | mass | ) |
Interpolating function for the gluon-gluon fusion H cross section ratio of the bottom-loop and the total contribution at 8 TeV.
| double THDMcache::ip_csr_ggH_t_13 | ( | double | mass | ) |
Interpolating function for the gluon-gluon fusion H cross section ratio of the top-loop and the total contribution at 13 TeV.
| double THDMcache::ip_csr_ggH_t_8 | ( | double | mass | ) |
Interpolating function for the gluon-gluon fusion H cross section ratio of the top-loop and the total contribution at 8 TeV.
| double THDMcache::ip_ex_bb_A_Zh_Zbb_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a bb associated pseudoscalar resonance decaying to a \(Z\) and an \(h\) boson, of which the latter further decays to a b quark pair.
Taken from ATLAS-CONF-2017-055, Figure 5b [83].
| double THDMcache::ip_ex_bb_A_Zh_Zbb_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a bb associated pseudoscalar resonance decaying to a \(Z\) and an \(h\) boson, of which the latter further decays to a b quark pair.
Taken from ATLAS-CONF-2017-055, Figure 5b [83].
| double THDMcache::ip_ex_bb_phi_bb_CMS8 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a bottom quark produced scalar resonance decaying to two bottom quarks.
Taken from CMS-HIG-14-017, Figure 6 [151].
| double THDMcache::ip_ex_bb_phi_bb_CMS8_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a bottom quark produced scalar resonance decaying to two bottom quarks.
Taken from CMS-HIG-14-017, Figure 6 [151].
| double THDMcache::ip_ex_bb_phi_tautau_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a bb associated scalar resonance decaying to two tau leptons.
Taken from ATLAS-CONF-2017-050, Figure 6b [102].
| double THDMcache::ip_ex_bb_phi_tautau_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a bb associated scalar resonance decaying to two tau leptons.
Taken from ATLAS-CONF-2017-050, Figure 6b [102].
| double THDMcache::ip_ex_bb_phi_tautau_ATLAS8 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a bottom quark produced scalar resonance decaying to two tau leptons.
Taken from arXiv:1409.6064, Figure 11b [3].
| double THDMcache::ip_ex_bb_phi_tautau_ATLAS8_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a bottom quark produced scalar resonance decaying to two tau leptons.
Taken from arXiv:1409.6064, Figure 11b [3].
| double THDMcache::ip_ex_bb_phi_tautau_CMS13 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a b associated scalar resonance decaying to two tau leptons.
Taken from CMS-PAS-HIG-16-037, Figure 9-b [73].
| double THDMcache::ip_ex_bb_phi_tautau_CMS13_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a b associated scalar resonance decaying to two tau leptons.
Taken from CMS-PAS-HIG-16-037, Figure 9-b [73].
| double THDMcache::ip_ex_bb_phi_tautau_CMS8 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a bottom quark produced scalar resonance decaying to two tau leptons.
Taken from CMS-PAS-HIG-14-029, Figure 10-b [68].
| double THDMcache::ip_ex_bb_phi_tautau_CMS8_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a bottom quark produced scalar resonance decaying to two tau leptons.
Taken from CMS-PAS-HIG-14-029, Figure 10-b [68].
| double THDMcache::ip_ex_bb_phi_tt_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a bb associated scalar resonance decaying to t quarks.
Taken from ATLAS-CONF-2016-104, Figure 21 [83].
| double THDMcache::ip_ex_bb_phi_tt_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a bb associated scalar resonance decaying to t quarks.
Taken from ATLAS-CONF-2016-104, Figure 21 [83].
| double THDMcache::ip_ex_bsgamma | ( | double | logtb, |
| double | logmHp | ||
| ) |
| double THDMcache::ip_ex_gg_A_hZ_bbll_CMS8 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a gluon-gluon produced pseudoscalar resonance decaying to \(hZ\) which further decay to a bottom quark pair and a light lepton pair.
Taken from arXiv:1504.04710, Figure 3 [149].
| double THDMcache::ip_ex_gg_A_hZ_bbll_CMS8_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a gluon-gluon produced pseudoscalar resonance decaying to \(hZ\) which further decay to a bottom quark pair and a light lepton pair.
Taken from arXiv:1504.04710, Figure 3 [149].
| double THDMcache::ip_ex_gg_A_hZ_bbZ_ATLAS8 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced pseudoscalar resonance decaying to \(hZ\) of which the Higgs further decays to a bottom quark pair.
Taken from arXiv:1502.04478, Figure 3b [6].
| double THDMcache::ip_ex_gg_A_hZ_bbZ_ATLAS8_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced pseudoscalar resonance decaying to \(hZ\) of which the Higgs further decays to a bottom quark pair.
Taken from arXiv:1502.04478, Figure 3b [6].
| double THDMcache::ip_ex_gg_A_hZ_tautaull_CMS8 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a gluon-gluon produced pseudoscalar resonance decaying to \(hZ\) which further decay to a \(\tau\) lepton pair and a light lepton pair.
Taken from arXiv:1510.01181, Figure 10, left [146].
| double THDMcache::ip_ex_gg_A_hZ_tautaull_CMS8_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a gluon-gluon produced pseudoscalar resonance decaying to \(hZ\) which further decay to a \(\tau\) lepton pair and a light lepton pair.
Taken from arXiv:1510.01181, Figure 10, left [146].
| double THDMcache::ip_ex_gg_A_hZ_tautauZ_ATLAS8 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced pseudoscalar resonance decaying to \(hZ\) of which the Higgs further decays to a \(\tau\) lepton pair.
Taken from arXiv:1502.04478, Figure 3a [6].
| double THDMcache::ip_ex_gg_A_hZ_tautauZ_ATLAS8_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced pseudoscalar resonance decaying to \(hZ\) of which the Higgs further decays to a \(\tau\) lepton pair.
Taken from arXiv:1502.04478, Figure 3a [6].
| double THDMcache::ip_ex_gg_A_Zh_Zbb_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced pseudoscalar resonance decaying to a \(Z\) and an \(h\) boson, of which the latter further decays to a b quark pair.
Taken from ATLAS-CONF-2017-055, Figure 5a [104].
| double THDMcache::ip_ex_gg_A_Zh_Zbb_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced pseudoscalar resonance decaying to a \(Z\) and an \(h\) boson, of which the latter further decays to a b quark pair.
Taken from ATLAS-CONF-2017-055, Figure 5a [104].
| double THDMcache::ip_ex_gg_H_hh_ATLAS8 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(h\) bosons.
Taken from arXiv:1509.04670, Figure 6 [10].
| double THDMcache::ip_ex_gg_H_hh_ATLAS8_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(h\) bosons.
Taken from arXiv:1509.04670, Figure 6 [10].
| double THDMcache::ip_ex_gg_H_hh_bbtautau_CMS8 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a gluon-gluon produced scalar resonance decaying to two \(h\) bosons which further decay to a bottom quark pair and a \(\tau\) lepton pair.
Taken from arXiv:1510.01181, Figure 8, bottom right [146].
| double THDMcache::ip_ex_gg_H_hh_bbtautau_CMS8_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a gluon-gluon produced scalar resonance decaying to two \(h\) bosons which further decay to a bottom quark pair and a \(\tau\) lepton pair.
Taken from arXiv:1510.01181, Figure 8, bottom right [146].
| double THDMcache::ip_ex_gg_H_WW_ATLAS8 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(W\) bosons.
Taken from arXiv:1509.00389, Figure 13, left [2].
| double THDMcache::ip_ex_gg_H_WW_ATLAS8_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(W\) bosons.
Taken from arXiv:1509.00389, Figure 13, left [2].
| double THDMcache::ip_ex_gg_H_WW_enumunu_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(W\) bosons which further decay to two lepton-neutrino pairs.
Taken from ATLAS-CONF-2016-074, Figure 4a [84].
| double THDMcache::ip_ex_gg_H_WW_enumunu_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(W\) bosons which further decay to two lepton-neutrino pairs.
Taken from ATLAS-CONF-2016-074, Figure 4a [84].
| double THDMcache::ip_ex_gg_H_WW_lnuqq_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(W\) bosons which further decay to a lepton-neutrino pair and a pair of quarks.
Taken from ATLAS-CONF-2017-051, Figure 7c [105].
| double THDMcache::ip_ex_gg_H_WW_lnuqq_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(W\) bosons which further decay to a lepton-neutrino pair and a pair of quarks.
Taken from ATLAS-CONF-2017-051, Figure 7c [105].
| double THDMcache::ip_ex_gg_H_ZZ_ATLAS8 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons.
Taken from arXiv:1507.05930, Figure 12(a) [11].
| double THDMcache::ip_ex_gg_H_ZZ_ATLAS8_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons.
Taken from arXiv:1507.05930, Figure 12(a) [11].
| double THDMcache::ip_ex_gg_H_ZZ_llll_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to four leptons.
Taken from ATLAS-CONF-2016-079, Figure 11a [94].
| double THDMcache::ip_ex_gg_H_ZZ_llll_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to four leptons.
Taken from ATLAS-CONF-2016-079, Figure 11a [94].
| double THDMcache::ip_ex_gg_H_ZZ_llllnunu_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two neutrinos or two leptons.
Taken from ATLAS-CONF-2017-058, Figure 6a [103].
| double THDMcache::ip_ex_gg_H_ZZ_llllnunu_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two neutrinos or two leptons.
Taken from ATLAS-CONF-2017-058, Figure 6a [103].
| double THDMcache::ip_ex_gg_H_ZZ_llnunu_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two neutrinos.
Taken from ATLAS-CONF-2016-056, Figure 7a [90].
| double THDMcache::ip_ex_gg_H_ZZ_llnunu_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two neutrinos.
Taken from ATLAS-CONF-2016-056, Figure 7a [90].
| double THDMcache::ip_ex_gg_H_ZZ_llnunu_CMS13 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two neutrinos.
Taken from CMS-PAS-HIG-16-001, Figure 4a [71].
| double THDMcache::ip_ex_gg_H_ZZ_llnunu_CMS13_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two neutrinos.
Taken from CMS-PAS-HIG-16-001, Figure 4a [71].
| double THDMcache::ip_ex_gg_H_ZZ_llqq_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two quarks.
Taken from ATLAS-CONF-2016-082, Figure 10a [93].
| double THDMcache::ip_ex_gg_H_ZZ_llqq_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two quarks.
Taken from ATLAS-CONF-2016-082, Figure 10a [93].
| double THDMcache::ip_ex_gg_H_ZZ_nunuqq_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to two neutrinos and two quarks.
Taken from ATLAS-CONF-2016-082, Figure 12c [93].
| double THDMcache::ip_ex_gg_H_ZZ_nunuqq_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to two neutrinos and two quarks.
Taken from ATLAS-CONF-2016-082, Figure 12c [93].
| double THDMcache::ip_ex_gg_H_ZZ_qqllnunu_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to two quarks and two neutrinos or two leptons.
Taken from Carminati-EPS2017.
| double THDMcache::ip_ex_gg_H_ZZ_qqllnunu_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(Z\) bosons which further decay to two quarks and two neutrinos or two leptons.
Taken from Carminati-EPS2017.
| double THDMcache::ip_ex_gg_phi_gaga_CMS13 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a gluon-gluon produced scalar resonance decaying to two photons.
Taken from CMS-EXO-PAS-16-027, Figure 7, top [81].
| double THDMcache::ip_ex_gg_phi_gaga_CMS13_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a gluon-gluon produced scalar resonance decaying to two photons.
Taken from CMS-EXO-PAS-16-027, Figure 7, top [81].
| double THDMcache::ip_ex_gg_phi_gaga_CMS8 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a gluon-gluon produced scalar resonance decaying to two photons.
Taken from arXiv:1506.02301, Figure 7, left [150].
| double THDMcache::ip_ex_gg_phi_gaga_CMS8_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a gluon-gluon produced scalar resonance decaying to two photons.
Taken from arXiv:1506.02301, Figure 7, left [150].
| double THDMcache::ip_ex_gg_phi_tautau_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two tau leptons.
Taken from ATLAS-CONF-2017-050, Figure 6a [102].
| double THDMcache::ip_ex_gg_phi_tautau_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two tau leptons.
Taken from ATLAS-CONF-2017-050, Figure 6a [102].
| double THDMcache::ip_ex_gg_phi_tautau_ATLAS8 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two tau leptons.
Taken from arXiv:1409.6064, Figure 11a [3].
| double THDMcache::ip_ex_gg_phi_tautau_ATLAS8_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two tau leptons.
Taken from arXiv:1409.6064, Figure 11a [3].
| double THDMcache::ip_ex_gg_phi_tautau_CMS13 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a gluon-gluon produced scalar resonance decaying to two tau leptons.
Taken from CMS-PAS-HIG-16-037, Figure 9-a [73].
| double THDMcache::ip_ex_gg_phi_tautau_CMS13_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a gluon-gluon produced scalar resonance decaying to two tau leptons.
Taken from CMS-PAS-HIG-16-037, Figure 9-a [73].
| double THDMcache::ip_ex_gg_phi_tautau_CMS8 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a gluon-gluon produced scalar resonance decaying to two tau leptons.
Taken from CMS-PAS-HIG-14-029, Figure 10-a [68].
| double THDMcache::ip_ex_gg_phi_tautau_CMS8_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a gluon-gluon produced scalar resonance decaying to two tau leptons.
Taken from CMS-PAS-HIG-14-029, Figure 10-a [68].
| double THDMcache::ip_ex_gg_phi_tt_ATLAS8 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to a top quark pair.
Taken from arXiv:1505.07018, Figure 11d [5].
| double THDMcache::ip_ex_gg_phi_tt_ATLAS8_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to a top quark pair.
Taken from arXiv:1505.07018, Figure 11d [5].
| double THDMcache::ip_ex_gg_phi_Zga_llga_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to a \(Z\) boson and a photon, of which the \(Z\) further decays to two leptons.
Taken from Carminati-EPS2017.
| double THDMcache::ip_ex_gg_phi_Zga_llga_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to a \(Z\) boson and a photon, of which the \(Z\) further decays to two leptons.
Taken from Carminati-EPS2017.
| double THDMcache::ip_ex_ggF_H_hh_bbbb_CMS13 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to four b quarks.
Taken from CMS-PAS-B2G-16-026, Figure 9 left [96].
| double THDMcache::ip_ex_ggF_H_hh_bbbb_CMS13_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to four b quarks.
Taken from CMS-PAS-B2G-16-026, Figure 9 left [96].
| double THDMcache::ip_ex_ggF_phi_Zga_CMS13 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a gluon-gluon produced scalar resonance decaying to a \(Z\) boson and a photon.
Taken from CMS-PAS-EXO-17-005, Figure 7 left [98].
| double THDMcache::ip_ex_ggF_phi_Zga_CMS13_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a gluon-gluon produced scalar resonance decaying to a \(Z\) boson and a photon.
Taken from CMS-PAS-EXO-17-005, Figure 7 left [98].
| double THDMcache::ip_ex_ggVV_H_WW_lnulnu_CMS13 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a gluon-gluon or vector boson fusion produced scalar resonance decaying to two \(W\) bosons which further decay to two lepton-neutrino pairs.
Taken from CMS-PAS-HIG-16-023, Figure 5-a [75].
| double THDMcache::ip_ex_ggVV_H_WW_lnulnu_CMS13_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a gluon-gluon or vector boson fusion produced scalar resonance decaying to two \(W\) bosons which further decay to two lepton-neutrino pairs.
Taken from CMS-PAS-HIG-16-023, Figure 5-a [75].
| double THDMcache::ip_ex_mu_pp_H_VV_CMS8 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two massive vector bosons.
Taken from arXiv:1504.00936, Figure 7, bottom right [148].
| double THDMcache::ip_ex_mu_pp_H_VV_CMS8_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two massive vector bosons.
Taken from arXiv:1504.00936, Figure 7, bottom right [148].
| double THDMcache::ip_ex_pp_A_HZ_bbll_CMS8 | ( | double | mA, |
| double | mH | ||
| ) |
Interpolating function for the observed CMS upper limit on a pseudoscalar resonance decaying to \(HZ\) which further decay to a \(b\) quark pair and a light lepton pair.
Taken from arXiv:1603.02991, Figure 1, lower right triangle [153].
| double THDMcache::ip_ex_pp_A_HZ_tautaull_CMS8 | ( | double | mA, |
| double | mH | ||
| ) |
Interpolating function for the observed CMS upper limit on a pseudoscalar resonance decaying to \(HZ\) which further decay to a \(\tau\) lepton pair and a light lepton pair.
Taken from arXiv:1603.02991, Figure 4, lower right triangle [153].
| double THDMcache::ip_ex_pp_A_Zga_llga_CMS8 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a pseudoscalar resonance decaying to a Z boson and a photon which further decay into two leptons and a photon.
Taken from CMS-PAS-HIG-16-014, Figure 2 [82].
| double THDMcache::ip_ex_pp_A_Zga_llga_CMS8_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a pseudoscalar resonance decaying to a Z boson and a photon which further decay into two leptons and a photon.
Taken from CMS-PAS-HIG-16-014, Figure 2 [82].
| double THDMcache::ip_ex_pp_H_AZ_bbll_CMS8 | ( | double | mA, |
| double | mH | ||
| ) |
Interpolating function for the observed CMS upper limit on a scalar resonance decaying to \(AZ\) which further decay to a \(b\) quark pair and a light lepton pair.
Taken from arXiv:1603.02991, Figure 1, upper left triangle [153].
| double THDMcache::ip_ex_pp_H_AZ_tautaull_CMS8 | ( | double | mA, |
| double | mH | ||
| ) |
Interpolating function for the observed CMS upper limit on a scalar resonance decaying to \(AZ\) which further decay to a \(\tau\) lepton pair and a light lepton pair.
Taken from arXiv:1603.02991, Figure 4, upper left triangle [153].
| double THDMcache::ip_ex_pp_H_hh_bbbb_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a spin-2 resonance decaying to two \(h\) bosons which further decay to four b quarks.
Taken from ATLAS-CONF-2016-049, Figure 11 [92].
| double THDMcache::ip_ex_pp_H_hh_bbbb_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a spin-2 resonance decaying to two \(h\) bosons which further decay to four b quarks.
Taken from ATLAS-CONF-2016-049, Figure 11 [92].
| double THDMcache::ip_ex_pp_H_hh_bbbb_CMS13 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to four b quarks.
Taken from CMS-PAS-HIG-16-002, Figure 7 [80].
| double THDMcache::ip_ex_pp_H_hh_bbbb_CMS13_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to four b quarks.
Taken from CMS-PAS-HIG-16-002, Figure 7 [80].
| double THDMcache::ip_ex_pp_H_hh_bblnulnu_CMS13 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to a b quark pair and two lepton-neutrino pairs.
Taken from CMS-PAS-HIG-16-011, Figure 5-a [79].
| double THDMcache::ip_ex_pp_H_hh_bblnulnu_CMS13_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to a b quark pair and two lepton-neutrino pairs.
Taken from CMS-PAS-HIG-16-011, Figure 5-a [79].
| double THDMcache::ip_ex_pp_H_hh_bbtautau1_CMS13 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to a b quark pair and two tau leptons.
Taken from CMS-PAS-HIG-17-002, Figure 5-a [100].
| double THDMcache::ip_ex_pp_H_hh_bbtautau1_CMS13_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to a b quark pair and two tau leptons.
Taken from CMS-PAS-HIG-17-002, Figure 5-a [100].
| double THDMcache::ip_ex_pp_H_hh_bbtautau_CMS13 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to a b quark pair and two tau leptons.
Taken from CMS-PAS-HIG-16-029, Figure 3 [78].
| double THDMcache::ip_ex_pp_H_hh_bbtautau_CMS13_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to a b quark pair and two tau leptons.
Taken from CMS-PAS-HIG-16-029, Figure 3 [78].
| double THDMcache::ip_ex_pp_H_hh_bbVV_CMS13 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to a b quark pair, two leptons and two neutrinos.
Taken from CMS-PAS-HIG-17-006, Figure 6-a [101].
| double THDMcache::ip_ex_pp_H_hh_bbVV_CMS13_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to a b quark pair, two leptons and two neutrinos.
Taken from CMS-PAS-HIG-17-006, Figure 6-a [101].
| double THDMcache::ip_ex_pp_H_hh_CMS8 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(h\) bosons.
Taken from CMS-PAS-HIG-15-013, Figure 5a [70].
| double THDMcache::ip_ex_pp_H_hh_CMS8_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(h\) bosons.
Taken from CMS-PAS-HIG-15-013, Figure 5a [70].
| double THDMcache::ip_ex_pp_H_hh_gagabb_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to two photons and a b quark pair.
Taken from ATLAS-CONF-2016-004, Figure 6a [88].
| double THDMcache::ip_ex_pp_H_hh_gagabb_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to two photons and a b quark pair.
Taken from ATLAS-CONF-2016-004, Figure 6a [88].
| double THDMcache::ip_ex_pp_H_hh_gagabb_CMS13 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to two photons and a b quark pair.
Taken from CMS-PAS-HIG-17-008, Figure 11 left [97].
| double THDMcache::ip_ex_pp_H_hh_gagabb_CMS13_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to two photons and a b quark pair.
Taken from CMS-PAS-HIG-17-008, Figure 11 left [97].
| double THDMcache::ip_ex_pp_H_hh_gagaWW_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(h\) bosons which further decay to two photons and two \(W\) bosons.
Taken from ATLAS-CONF-2016-071, Figure 3a [87].
| double THDMcache::ip_ex_pp_H_hh_gagaWW_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a gluon-gluon produced scalar resonance decaying to two \(h\) bosons which further decay to two photons and two \(W\) bosons.
Taken from ATLAS-CONF-2016-071, Figure 3a [87].
| double THDMcache::ip_ex_pp_H_VV_qqqq_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a scalar resonance decaying to two \(W\) or \(Z\) bosons which further decay hadronically.
Taken from Carminati-EPS2017.
| double THDMcache::ip_ex_pp_H_VV_qqqq_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a scalar resonance decaying to two \(W\) or \(Z\) bosons which further decay hadronically.
Taken from Carminati-EPS2017.
| double THDMcache::ip_ex_pp_H_ZZ_llll_CMS13 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(Z\) bosons which further decay to four leptons.
Taken from CMS-PAS-HIG-16-033, Figure 16-a [69].
| double THDMcache::ip_ex_pp_H_ZZ_llll_CMS13_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(Z\) bosons which further decay to four leptons.
Taken from CMS-PAS-HIG-16-033, Figure 16-a [69].
| double THDMcache::ip_ex_pp_H_ZZ_llnunu_CMS13 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two neutrinos.
Taken from CMS-PAS-B2G-16-023, Figure 5 [95].
| double THDMcache::ip_ex_pp_H_ZZ_llnunu_CMS13_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two neutrinos.
Taken from CMS-PAS-B2G-16-023, Figure 5 [95].
| double THDMcache::ip_ex_pp_H_ZZ_llqq_CMS13 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two quarks.
Taken from CMS-PAS-HIG-16-034, Figure 4-a [99].
| double THDMcache::ip_ex_pp_H_ZZ_llqq_CMS13_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two quarks.
Taken from CMS-PAS-HIG-16-034, Figure 4-a [99].
| double THDMcache::ip_ex_pp_Hp_taunu_CMS8 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a singly charged scalar resonance decaying to a \(\tau\) lepton and a neutrino.
Taken from arXiv:1508.07774, Table 10 bottom [147].
| double THDMcache::ip_ex_pp_Hp_taunu_CMS8_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a singly charged scalar resonance decaying to a \(\tau\) lepton and a neutrino.
Taken from arXiv:1508.07774, Table 10 bottom [147].
| double THDMcache::ip_ex_pp_Hp_tb_ATLAS13_1 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a singly charged scalar resonance decaying to a \(t\) quark and a \(b\) quark.
Taken from ATLAS-CONF-2016-089, Figure 12 [86].
| double THDMcache::ip_ex_pp_Hp_tb_ATLAS13_1_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a singly charged scalar resonance decaying to a \(t\) quark and a \(b\) quark.
Taken from ATLAS-CONF-2016-089, Figure 12 [86].
| double THDMcache::ip_ex_pp_Hp_tb_ATLAS13_2 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a singly charged scalar resonance decaying to a \(t\) quark and a \(b\) quark.
Taken from ATLAS-CONF-2016-104, Figure 23 [89].
| double THDMcache::ip_ex_pp_Hp_tb_ATLAS13_2_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a singly charged scalar resonance decaying to a \(t\) quark and a \(b\) quark.
Taken from ATLAS-CONF-2016-104, Figure 23 [89].
| double THDMcache::ip_ex_pp_Hp_tb_CMS8 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a singly charged scalar resonance decaying to a \(t\) quark and a \(b\) quark.
Taken from arXiv:1508.07774, Table 11 [147].
| double THDMcache::ip_ex_pp_Hp_tb_CMS8_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a singly charged scalar resonance decaying to a \(t\) quark and a \(b\) quark.
Taken from arXiv:1508.07774, Table 11 [147].
| double THDMcache::ip_ex_pp_Hpm_taunu_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a singly charged scalar resonance decaying to a \(\tau\) lepton and a neutrino.
Taken from ATLAS-CONF-2016-088, Figure 6 [85].
| double THDMcache::ip_ex_pp_Hpm_taunu_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a singly charged scalar resonance decaying to a \(\tau\) lepton and a neutrino.
Taken from ATLAS-CONF-2016-088, Figure 6 [85].
| double THDMcache::ip_ex_pp_Hpm_taunu_ATLAS8 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a singly charged scalar resonance decaying to a \(\tau\) lepton and a neutrino.
Taken from arXiv:1412.6663, Figure 7-b [7].
| double THDMcache::ip_ex_pp_Hpm_taunu_ATLAS8_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a singly charged scalar resonance decaying to a \(\tau\) lepton and a neutrino.
Taken from arXiv:1412.6663, Figure 7-b [7].
| double THDMcache::ip_ex_pp_Hpm_taunu_CMS13 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a singly charged scalar resonance decaying to a \(\tau\) lepton and a neutrino.
Taken from CMS-PAS-HIG-16-031, Figure 6 right [74].
| double THDMcache::ip_ex_pp_Hpm_taunu_CMS13_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a singly charged scalar resonance decaying to a \(\tau\) lepton and a neutrino.
Taken from CMS-PAS-HIG-16-031, Figure 6 right [74].
| double THDMcache::ip_ex_pp_Hpm_tb_ATLAS8 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a singly charged scalar resonance decaying to a \(t\) quark and a \(b\) quark.
Taken from arXiv:1512.03704, Figure 6 [8].
| double THDMcache::ip_ex_pp_Hpm_tb_ATLAS8_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a singly charged scalar resonance decaying to a \(t\) quark and a \(b\) quark.
Taken from arXiv:1512.03704, Figure 6 [8].
| double THDMcache::ip_ex_pp_phi_bb_CMS13 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a scalar resonance decaying to a b quark pair.
Taken from CMS-PAS-HIG-16-025, Figure 5 [72].
| double THDMcache::ip_ex_pp_phi_bb_CMS13_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a scalar resonance decaying to a b quark pair.
Taken from CMS-PAS-HIG-16-025, Figure 5 [72].
| double THDMcache::ip_ex_pp_phi_gaga_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a scalar resonance decaying to two photons.
Taken from 1707.04147, Figure ? [1].
| double THDMcache::ip_ex_pp_phi_gaga_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a scalar resonance decaying to two photons.
Taken from 1707.04147, Figure ? [1].
| double THDMcache::ip_ex_pp_phi_gaga_ATLAS8 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a scalar resonance decaying to two photons.
Taken from arXiv:1407.6583, Figure 4 [9].
| double THDMcache::ip_ex_pp_phi_gaga_ATLAS8_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a scalar resonance decaying to two photons.
Taken from arXiv:1407.6583, Figure 4 [9].
| double THDMcache::ip_ex_pp_phi_hh_bbbb_CMS8 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to two bottom quark pairs.
Taken from arXiv:1503.04114, Figure 5, left [152].
| double THDMcache::ip_ex_pp_phi_hh_bbbb_CMS8_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to two bottom quark pairs.
Taken from arXiv:1503.04114, Figure 5, left [152].
| double THDMcache::ip_ex_pp_phi_hh_gagabb_CMS8 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to a photon pair and a bottom quark pair.
Taken from CMS-PAS-HIG-13-032, Figure 8 [67].
| double THDMcache::ip_ex_pp_phi_hh_gagabb_CMS8_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a scalar resonance decaying to two \(h\) bosons which further decay to a photon pair and a bottom quark pair.
Taken from CMS-PAS-HIG-13-032, Figure 8 [67].
| double THDMcache::ip_ex_pp_phi_Zga_llga_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a scalar resonance decaying to a \(Z\) boson and a photon, of which the \(Z\) further decays to two leptons.
Taken from ATLAS-CONF-2016-044, Figure 6 [91].
| double THDMcache::ip_ex_pp_phi_Zga_llga_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a scalar resonance decaying to a \(Z\) boson and a photon, of which the \(Z\) further decays to two leptons.
Taken from ATLAS-CONF-2016-044, Figure 6 [91].
| double THDMcache::ip_ex_pp_phi_Zga_llga_ATLAS8 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a pseudoscalar resonance decaying to a Z boson and a photon which further decay into two leptons and a photon.
Taken from arXiv:1407.8150, Figure 3c [4].
| double THDMcache::ip_ex_pp_phi_Zga_llga_ATLAS8_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a pseudoscalar resonance decaying to a Z boson and a photon which further decay into two leptons and a photon.
Taken from arXiv:1407.8150, Figure 3c [4].
| double THDMcache::ip_ex_pp_phi_Zga_llga_CMS13 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a scalar resonance decaying to a \(Z\) boson and a photon, of which the \(Z\) further decays to two leptons.
Taken from CMS-EXO-PAS-16-034, Figure 4 [77].
| double THDMcache::ip_ex_pp_phi_Zga_llga_CMS13_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a scalar resonance decaying to a \(Z\) boson and a photon, of which the \(Z\) further decays to two leptons.
Taken from CMS-EXO-PAS-16-034, Figure 4 [77].
| double THDMcache::ip_ex_pp_phi_Zga_qqga_CMS13 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a scalar resonance decaying to a \(Z\) boson and a photon, of which the \(Z\) further decays to two quarks.
Taken from CMS-EXO-PAS-16-035, Figure 5-a [76].
| double THDMcache::ip_ex_pp_phi_Zga_qqga_CMS13_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a scalar resonance decaying to a \(Z\) boson and a photon, of which the \(Z\) further decays to two quarks.
Taken from CMS-EXO-PAS-16-035, Figure 5-a [76].
| double THDMcache::ip_ex_tt_phi_tt_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a tt associated scalar resonance decaying to t quarks.
Taken from ATLAS-CONF-2016-104, Figure 22 [83].
| double THDMcache::ip_ex_tt_phi_tt_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a tt associated scalar resonance decaying to t quarks.
Taken from ATLAS-CONF-2016-104, Figure 22 [83].
| double THDMcache::ip_ex_VBF_H_WW_ATLAS8 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a vector boson fusion produced scalar resonance decaying to two \(W\) bosons.
Taken from arXiv:1509.00389, Figure 13, right [2].
| double THDMcache::ip_ex_VBF_H_WW_ATLAS8_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a vector boson fusion produced scalar resonance decaying to two \(W\) bosons.
Taken from arXiv:1509.00389, Figure 13, right [2].
| double THDMcache::ip_ex_VBF_H_WW_enumunu_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a vector boson fusion produced scalar resonance decaying to two \(W\) bosons which further decay to two lepton-neutrino pairs.
Taken from ATLAS-CONF-2016-074, Figure 4b [84].
| double THDMcache::ip_ex_VBF_H_WW_enumunu_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a vector boson fusion produced scalar resonance decaying to two \(W\) bosons which further decay to two lepton-neutrino pairs.
Taken from ATLAS-CONF-2016-074, Figure 4b [84].
| double THDMcache::ip_ex_VBF_H_WW_lnuqq_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a VBF produced scalar resonance decaying to two \(W\) bosons which further decay to a lepton-neutrino pair and a pair of quarks.
Taken from ATLAS-CONF-2017-051, Figure 6c [105].
| double THDMcache::ip_ex_VBF_H_WW_lnuqq_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a VBF produced scalar resonance decaying to two \(W\) bosons which further decay to a lepton-neutrino pair and a pair of quarks.
Taken from ATLAS-CONF-2017-051, Figure 6c [105].
| double THDMcache::ip_ex_VBF_H_ZZ_ATLAS8 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a vector boson fusion produced scalar resonance decaying to two \(Z\) bosons.
Taken from arXiv:1507.05930, Figure 12(b) [11].
| double THDMcache::ip_ex_VBF_H_ZZ_ATLAS8_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a vector boson fusion produced scalar resonance decaying to two \(Z\) bosons.
Taken from arXiv:1507.05930, Figure 12(b) [11].
| double THDMcache::ip_ex_VBF_H_ZZ_llll_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a vector boson fusion produced scalar resonance decaying to two \(Z\) bosons which further decay to four leptons.
Taken from ATLAS-CONF-2016-079, Figure 11b [94].
| double THDMcache::ip_ex_VBF_H_ZZ_llll_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a vector boson fusion produced scalar resonance decaying to two \(Z\) bosons which further decay to four leptons.
Taken from ATLAS-CONF-2016-079, Figure 11b [94].
| double THDMcache::ip_ex_VBF_H_ZZ_llllnunu_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a VBF produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two neutrinos or two leptons.
Taken from ATLAS-CONF-2017-058, Figure 6b [103].
| double THDMcache::ip_ex_VBF_H_ZZ_llllnunu_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a VBF produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two neutrinos or two leptons.
Taken from ATLAS-CONF-2017-058, Figure 6b [103].
| double THDMcache::ip_ex_VBF_H_ZZ_llnunu_CMS13 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a VBF produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two neutrinos.
Taken from CMS-PAS-HIG-16-001, Figure 4b [71].
| double THDMcache::ip_ex_VBF_H_ZZ_llnunu_CMS13_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a VBF produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two neutrinos.
Taken from CMS-PAS-HIG-16-001, Figure 4b [71].
| double THDMcache::ip_ex_VBF_H_ZZ_llqq_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a vector boson fusion produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two quarks.
Taken from ATLAS-CONF-2016-082, Figure 10b [93].
| double THDMcache::ip_ex_VBF_H_ZZ_llqq_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a vector boson fusion produced scalar resonance decaying to two \(Z\) bosons which further decay to two leptons and two quarks.
Taken from ATLAS-CONF-2016-082, Figure 10b [93].
| double THDMcache::ip_ex_VBF_H_ZZ_qqllnunu_ATLAS13 | ( | double | mass | ) |
Interpolating function for the observed ATLAS upper limit on a VBF produced scalar resonance decaying to two \(Z\) bosons which further decay to two quarks and two neutrinos or two leptons.
Taken from Carminati-EPS2017.
| double THDMcache::ip_ex_VBF_H_ZZ_qqllnunu_ATLAS13_e | ( | double | mass | ) |
Interpolating function for the expected ATLAS upper limit on a VBF produced scalar resonance decaying to two \(Z\) bosons which further decay to two quarks and two neutrinos or two leptons.
Taken from Carminati-EPS2017.
| double THDMcache::ip_ex_VBF_VH_H_ZZ_llll_CMS13 | ( | double | mass | ) |
Interpolating function for the observed CMS upper limit on a vector boson fusion produced scalar resonance decaying to two \(Z\) bosons which further decay to four leptons.
Taken from CMS-PAS-HIG-16-033, Figure 16-b [69].
| double THDMcache::ip_ex_VBF_VH_H_ZZ_llll_CMS13_e | ( | double | mass | ) |
Interpolating function for the expected CMS upper limit on a vector boson fusion produced scalar resonance decaying to two \(Z\) bosons which further decay to four leptons.
Taken from CMS-PAS-HIG-16-033, Figure 16-b [69].
| double THDMcache::ip_GammaHPtotSM | ( | double | mass | ) |
Interpolating function for the total SM Higgs decay width.
| double THDMcache::KaellenFunction | ( | const double | a2, |
| const double | b2, | ||
| const double | c2 | ||
| ) | const |
Kaellen function.
| double THDMcache::MWTHDM | ( | const double | MW | ) | const |
| void THDMcache::read | ( | ) |
Fills all required arrays with the values read from the tables.
| gslpp::matrix<double> THDMcache::readTable | ( | std::string | filename, |
| int | rowN, | ||
| int | colN | ||
| ) |
This function reads values from a table and returns them as an array.
| void THDMcache::runTHDMparameters | ( | ) |
| double THDMcache::updateCache | ( | ) |
|
mutableprivate |
Definition at line 3871 of file THDMcache.h.
|
mutableprivate |
Definition at line 3874 of file THDMcache.h.
|
mutableprivate |
Definition at line 3868 of file THDMcache.h.
|
mutableprivate |
Definition at line 3869 of file THDMcache.h.
|
mutableprivate |
Definition at line 3876 of file THDMcache.h.
|
mutableprivate |
Definition at line 3872 of file THDMcache.h.
|
mutableprivate |
Definition at line 3866 of file THDMcache.h.
|
mutableprivate |
Definition at line 3875 of file THDMcache.h.
|
mutableprivate |
Definition at line 3870 of file THDMcache.h.
|
mutableprivate |
Definition at line 3873 of file THDMcache.h.
|
mutableprivate |
Definition at line 3867 of file THDMcache.h.
|
private |
Definition at line 3446 of file THDMcache.h.
|
private |
Definition at line 3447 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::arraybsgamma |
\(b\to s \gamma\) table, depending on logtb and the logarithm of the charged Higgs mass.
Definition at line 195 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_bb_A_Zh_Zbb |
ATLAS observed \(95\%\) upper cross section limits at 13 TeV, depending on the Higgs mass.
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_bb_A_Zh_Zbb_e |
ATLAS expected \(95\%\) upper cross section limits at 13 TeV, depending on the Higgs mass.
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_bb_phi_tautau |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_bb_phi_tautau_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_bb_phi_tt |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_bb_phi_tt_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_gg_A_Zh_Zbb |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_gg_A_Zh_Zbb_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_gg_H_WW_enumumu |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_gg_H_WW_enumumu_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_gg_H_WW_lnuqq |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_gg_H_WW_lnuqq_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_gg_H_ZZ_llll |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_gg_H_ZZ_llll_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_gg_H_ZZ_llllnunu |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_gg_H_ZZ_llllnunu_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_gg_H_ZZ_llnunu |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_gg_H_ZZ_llnunu_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_gg_H_ZZ_llqq |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_gg_H_ZZ_llqq_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_gg_H_ZZ_nunuqq |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_gg_H_ZZ_nunuqq_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_gg_H_ZZ_qqllnunu |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_gg_H_ZZ_qqllnunu_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_gg_phi_tautau |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_gg_phi_tautau_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_gg_phi_Zga_llga |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_gg_phi_Zga_llga_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_pp_H_hh_bbbb |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_pp_H_hh_bbbb_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_pp_H_hh_gagabb |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_pp_H_hh_gagabb_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_pp_H_hh_gagaWW |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_pp_H_hh_gagaWW_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_pp_H_VV_qqqq |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_pp_H_VV_qqqq_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_pp_Hp_tb1 |
Definition at line 187 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_pp_Hp_tb1_e |
Definition at line 189 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_pp_Hp_tb2 |
ATLAS observed \(95\%\) upper cross section limits at 13 TeV, depending on the charged Higgs mass.
Definition at line 187 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_pp_Hp_tb2_e |
ATLAS expected \(95\%\) upper cross section limits at 13 TeV, depending on the charged Higgs mass.
Definition at line 189 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_pp_Hpm_taunu |
Definition at line 187 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_pp_Hpm_taunu_e |
Definition at line 189 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_pp_phi_gaga |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_pp_phi_gaga_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_pp_phi_Zga |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_pp_phi_Zga_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_tt_phi_tt |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_tt_phi_tt_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_VBF_H_WW_enumumu |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_VBF_H_WW_enumumu_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_VBF_H_WW_lnuqq |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_VBF_H_WW_lnuqq_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_VBF_H_ZZ_llll |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_VBF_H_ZZ_llll_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_VBF_H_ZZ_llllnunu |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_VBF_H_ZZ_llllnunu_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_VBF_H_ZZ_llqq |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_VBF_H_ZZ_llqq_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_VBF_H_ZZ_qqllnunu |
Definition at line 150 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS13_VBF_H_ZZ_qqllnunu_e |
Definition at line 156 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_bb_phi_tautau |
Definition at line 136 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_bb_phi_tautau_e |
Definition at line 138 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_gg_A_hZ_bbZ |
Definition at line 136 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_gg_A_hZ_bbZ_e |
Definition at line 138 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_gg_A_hZ_tautauZ |
Definition at line 136 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_gg_A_hZ_tautauZ_e |
Definition at line 138 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_gg_H_hh |
ATLAS observed \(95\%\) upper cross section limits at 8 TeV, depending on the Higgs mass.
Definition at line 136 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_gg_H_hh_e |
ATLAS expected \(95\%\) upper cross section limits at 8 TeV, depending on the Higgs mass.
Definition at line 138 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_gg_H_WW |
Definition at line 136 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_gg_H_WW_e |
Definition at line 138 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_gg_H_ZZ |
Definition at line 136 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_gg_H_ZZ_e |
Definition at line 138 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_gg_phi_tautau |
Definition at line 136 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_gg_phi_tautau_e |
Definition at line 138 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_gg_phi_tt |
Definition at line 136 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_gg_phi_tt_e |
Definition at line 138 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_pp_Hpm_taunu |
Definition at line 179 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_pp_Hpm_taunu_e |
Definition at line 181 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_pp_Hpm_tb |
ATLAS observed \(95\%\) upper cross section limits at 8 TeV, depending on the charged Higgs mass.
Definition at line 179 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_pp_Hpm_tb_e |
ATLAS expected \(95\%\) upper cross section limits at 8 TeV, depending on the charged Higgs mass.
Definition at line 181 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_pp_phi_gaga |
Definition at line 136 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_pp_phi_gaga_e |
Definition at line 138 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_pp_phi_Zga_llga |
Definition at line 136 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_pp_phi_Zga_llga_e |
Definition at line 138 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_VBF_H_WW |
Definition at line 136 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_VBF_H_WW_e |
Definition at line 138 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_VBF_H_ZZ |
Definition at line 136 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::ATLAS8_VBF_H_ZZ_e |
Definition at line 138 of file THDMcache.h.
|
mutableprivate |
Definition at line 3541 of file THDMcache.h.
|
mutableprivate |
Definition at line 3542 of file THDMcache.h.
|
mutableprivate |
Definition at line 3543 of file THDMcache.h.
|
mutableprivate |
Definition at line 3544 of file THDMcache.h.
|
mutableprivate |
Definition at line 3545 of file THDMcache.h.
|
mutableprivate |
Definition at line 3546 of file THDMcache.h.
|
mutableprivate |
Definition at line 3547 of file THDMcache.h.
|
mutableprivate |
Definition at line 3548 of file THDMcache.h.
|
mutableprivate |
Definition at line 3549 of file THDMcache.h.
|
mutableprivate |
Definition at line 3550 of file THDMcache.h.
|
mutableprivate |
Definition at line 3551 of file THDMcache.h.
|
mutableprivate |
Definition at line 3552 of file THDMcache.h.
|
mutableprivate |
Definition at line 3553 of file THDMcache.h.
|
mutableprivate |
Definition at line 3554 of file THDMcache.h.
|
mutableprivate |
Definition at line 3555 of file THDMcache.h.
|
mutableprivate |
Definition at line 3556 of file THDMcache.h.
|
mutableprivate |
Definition at line 3557 of file THDMcache.h.
|
mutableprivate |
Definition at line 3558 of file THDMcache.h.
|
mutableprivate |
Definition at line 3559 of file THDMcache.h.
|
mutableprivate |
Definition at line 3560 of file THDMcache.h.
|
mutableprivate |
Definition at line 3561 of file THDMcache.h.
|
mutableprivate |
Definition at line 3477 of file THDMcache.h.
|
mutableprivate |
Definition at line 3476 of file THDMcache.h.
|
mutableprivate |
Definition at line 3481 of file THDMcache.h.
|
mutableprivate |
Definition at line 3480 of file THDMcache.h.
|
mutableprivate |
Definition at line 3479 of file THDMcache.h.
|
mutableprivate |
Definition at line 3478 of file THDMcache.h.
|
mutableprivate |
Definition at line 3467 of file THDMcache.h.
|
mutableprivate |
Definition at line 3468 of file THDMcache.h.
|
mutableprivate |
Definition at line 3469 of file THDMcache.h.
|
mutableprivate |
Definition at line 3470 of file THDMcache.h.
|
mutableprivate |
Definition at line 3503 of file THDMcache.h.
|
mutableprivate |
Definition at line 3502 of file THDMcache.h.
|
mutableprivate |
Definition at line 3505 of file THDMcache.h.
|
mutableprivate |
Definition at line 3504 of file THDMcache.h.
|
mutableprivate |
Definition at line 3490 of file THDMcache.h.
|
mutableprivate |
Definition at line 3492 of file THDMcache.h.
|
mutableprivate |
Definition at line 3491 of file THDMcache.h.
|
mutableprivate |
Definition at line 3497 of file THDMcache.h.
|
mutableprivate |
Definition at line 3495 of file THDMcache.h.
|
mutableprivate |
Definition at line 3494 of file THDMcache.h.
|
mutableprivate |
Definition at line 3493 of file THDMcache.h.
|
mutableprivate |
Definition at line 3496 of file THDMcache.h.
|
mutableprivate |
Definition at line 3482 of file THDMcache.h.
|
mutableprivate |
Definition at line 3484 of file THDMcache.h.
|
mutableprivate |
Definition at line 3483 of file THDMcache.h.
|
mutableprivate |
Definition at line 3489 of file THDMcache.h.
|
mutableprivate |
Definition at line 3487 of file THDMcache.h.
|
mutableprivate |
Definition at line 3486 of file THDMcache.h.
|
mutableprivate |
Definition at line 3485 of file THDMcache.h.
|
mutableprivate |
Definition at line 3488 of file THDMcache.h.
|
mutableprivate |
Definition at line 3499 of file THDMcache.h.
|
mutableprivate |
Definition at line 3498 of file THDMcache.h.
|
mutableprivate |
Definition at line 3501 of file THDMcache.h.
|
mutableprivate |
Definition at line 3500 of file THDMcache.h.
|
mutableprivate |
Definition at line 3471 of file THDMcache.h.
|
mutableprivate |
Definition at line 3472 of file THDMcache.h.
|
mutableprivate |
Definition at line 3473 of file THDMcache.h.
|
mutableprivate |
Definition at line 3474 of file THDMcache.h.
|
mutableprivate |
Definition at line 3508 of file THDMcache.h.
|
mutableprivate |
Definition at line 3507 of file THDMcache.h.
|
mutableprivate |
Definition at line 3513 of file THDMcache.h.
|
mutableprivate |
Definition at line 3512 of file THDMcache.h.
|
mutableprivate |
Definition at line 3511 of file THDMcache.h.
|
mutableprivate |
Definition at line 3510 of file THDMcache.h.
|
mutableprivate |
Definition at line 3509 of file THDMcache.h.
|
mutableprivate |
Definition at line 3536 of file THDMcache.h.
|
mutableprivate |
Definition at line 3535 of file THDMcache.h.
|
mutableprivate |
Definition at line 3537 of file THDMcache.h.
|
mutableprivate |
Definition at line 3539 of file THDMcache.h.
|
mutableprivate |
Definition at line 3538 of file THDMcache.h.
|
mutableprivate |
Definition at line 3522 of file THDMcache.h.
|
mutableprivate |
Definition at line 3524 of file THDMcache.h.
|
mutableprivate |
Definition at line 3523 of file THDMcache.h.
|
mutableprivate |
Definition at line 3529 of file THDMcache.h.
|
mutableprivate |
Definition at line 3527 of file THDMcache.h.
|
mutableprivate |
Definition at line 3526 of file THDMcache.h.
|
mutableprivate |
Definition at line 3525 of file THDMcache.h.
|
mutableprivate |
Definition at line 3528 of file THDMcache.h.
|
mutableprivate |
Definition at line 3514 of file THDMcache.h.
|
mutableprivate |
Definition at line 3516 of file THDMcache.h.
|
mutableprivate |
Definition at line 3515 of file THDMcache.h.
|
mutableprivate |
Definition at line 3521 of file THDMcache.h.
|
mutableprivate |
Definition at line 3519 of file THDMcache.h.
|
mutableprivate |
Definition at line 3518 of file THDMcache.h.
|
mutableprivate |
Definition at line 3517 of file THDMcache.h.
|
mutableprivate |
Definition at line 3520 of file THDMcache.h.
|
mutableprivate |
Definition at line 3532 of file THDMcache.h.
|
mutableprivate |
Definition at line 3531 of file THDMcache.h.
|
mutableprivate |
Definition at line 3530 of file THDMcache.h.
|
mutableprivate |
Definition at line 3534 of file THDMcache.h.
|
mutableprivate |
Definition at line 3533 of file THDMcache.h.
| double THDMcache::bbF_A_bb_TH8 |
Cross section times branching ratio for the process \(b\bar b\to A\to b\bar b\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{b\bar b\to A}\cdot BR^{\text{THDM}}(A\to b\bar b)\)
Definition at line 3244 of file THDMcache.h.
| double THDMcache::bbF_A_hZ_bbZ_TH13 |
Cross section times branching ratio for the process \(b\bar b\to A\to hZ\to b\bar b Z\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{b\bar b\to A}\cdot BR^{\text{THDM}}(A\to hZ\to b\bar b Z)\)
Definition at line 3264 of file THDMcache.h.
| double THDMcache::bbF_A_tautau_TH13 |
Cross section times branching ratio for the process \(b\bar b\to A\to \tau \tauZ\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{b\bar b\to A}\cdot BR^{\text{THDM}}(A\to \tau \tau)\)
Definition at line 3252 of file THDMcache.h.
| double THDMcache::bbF_A_tautau_TH8 |
Cross section times branching ratio for the process \(b\bar b\to A\to \tau\tau\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{b\bar b\to A}\cdot BR^{\text{THDM}}(A\to \tau\tau)\)
Definition at line 3224 of file THDMcache.h.
| double THDMcache::bbF_A_tt_TH13 |
Cross section times branching ratio for the process \(b\bar b\to A\to t\bar t\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{b\bar b\to A}\cdot BR^{\text{THDM}}(A\to t\bar t)\)
Definition at line 3268 of file THDMcache.h.
| double THDMcache::bbF_H_bb_TH8 |
Cross section times branching ratio for the process \(b\bar b\to H\to b\bar b\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{b\bar b\to H}\cdot BR^{\text{THDM}}(H\to b\bar b)\)
Definition at line 2974 of file THDMcache.h.
| double THDMcache::bbF_H_tautau_TH13 |
Cross section times branching ratio for the process \(b\bar b\to H\to \tau\tau\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{b\bar b\to H}\cdot BR^{\text{THDM}}(H\to \tau\tau)\)
Definition at line 2982 of file THDMcache.h.
| double THDMcache::bbF_H_tautau_TH8 |
Cross section times branching ratio for the process \(b\bar b\to H\to \tau\tau\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{b\bar b\to H}\cdot BR^{\text{THDM}}(H\to \tau\tau)\)
Definition at line 2944 of file THDMcache.h.
| double THDMcache::bbF_H_tt_TH13 |
Cross section times branching ratio for the process \(b\bar b\to H\to t\bar t\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{b\bar b\to H}\cdot BR^{\text{THDM}}(H\to t\bar t)\)
Definition at line 3032 of file THDMcache.h.
|
private |
Definition at line 3436 of file THDMcache.h.
|
private |
Definition at line 3437 of file THDMcache.h.
|
private |
Definition at line 3435 of file THDMcache.h.
|
private |
Definition at line 3433 of file THDMcache.h.
|
private |
Definition at line 3434 of file THDMcache.h.
|
private |
Definition at line 3432 of file THDMcache.h.
|
private |
Definition at line 3428 of file THDMcache.h.
| double THDMcache::Br_Atobb |
Definition at line 3218 of file THDMcache.h.
| double THDMcache::Br_Atogaga |
Definition at line 3216 of file THDMcache.h.
| double THDMcache::Br_AtoHpW |
\(A\) branching ratio to a charged Higgs and a \(W^\mp\) boson.
Definition at line 3286 of file THDMcache.h.
| double THDMcache::Br_AtoHZ |
\(A\) branching ratio to an \(H\) and a \(Z\) boson. This is \(BR(A\to HZ)\)
Definition at line 3278 of file THDMcache.h.
| double THDMcache::Br_AtohZ |
\(A\) branching ratio to an \(h\) and a \(Z\) boson. This is \(BR(A\to hZ)\)
Definition at line 3280 of file THDMcache.h.
| double THDMcache::Br_Atotautau |
Definition at line 3215 of file THDMcache.h.
| double THDMcache::Br_Atott |
Definition at line 3217 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::br_bb |
Definition at line 108 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::br_cc |
Definition at line 108 of file THDMcache.h.
| double THDMcache::Br_HtoAA |
\(H\) branching ratio to two CP-odd Higgs bosons. This is \(BR(H\to AA)\)
Definition at line 3047 of file THDMcache.h.
| double THDMcache::Br_HtoAZ |
\(H\) branching ratio to two light Higgs bosons. This is \(BR(H\to hh)\)
Definition at line 3051 of file THDMcache.h.
| double THDMcache::Br_Htobb |
Definition at line 2939 of file THDMcache.h.
| double THDMcache::Br_Htogaga |
Definition at line 2934 of file THDMcache.h.
| double THDMcache::Br_Htohh |
\(H\) branching ratio to two light Higgs bosons. This is \(BR(H\to hh)\)
Definition at line 3045 of file THDMcache.h.
| double THDMcache::Br_HtoHpHm |
\(H\) branching ratio to two charged Higgs bosons. This is \(BR(H\to H^\pm H^\mp)\)
Definition at line 3049 of file THDMcache.h.
| double THDMcache::Br_HtoHpW |
\(H\) branching ratio to two light Higgs bosons. This is \(BR(H\to hh)\)
Definition at line 3053 of file THDMcache.h.
| double THDMcache::Br_Htotautau |
Definition at line 2933 of file THDMcache.h.
| double THDMcache::Br_Htott |
Definition at line 2938 of file THDMcache.h.
| double THDMcache::Br_HtoWW |
Definition at line 2937 of file THDMcache.h.
| double THDMcache::Br_HtoZga |
Definition at line 2935 of file THDMcache.h.
| double THDMcache::Br_HtoZZ |
Definition at line 2936 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::br_mumu |
Definition at line 108 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::br_tautau |
Definition at line 108 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::br_tt |
Definition at line 108 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::br_WW |
SM Higgs branching ratio tables (obtained with HDECAY 6.10), depending on the Higgs mass.
Definition at line 108 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::br_ZZ |
Definition at line 108 of file THDMcache.h.
| double THDMcache::BrSM_htobb |
SM branching ratio of \(h\to b \bar b\). This is \(BR{\text SM}(h\to b \bar b)\)
Definition at line 2876 of file THDMcache.h.
| double THDMcache::BrSM_htogaga |
SM branching ratio of \(h\to \gamma \gamma\). This is \(BR{\text SM}(h\to \gamma \gamma)\)
Definition at line 2878 of file THDMcache.h.
| double THDMcache::BrSM_htotautau |
SM branching ratio of \(h\to \tau \tau\). This is \(BR{\text SM}(h\to \tau \tau)\)
Definition at line 2880 of file THDMcache.h.
|
static |
Cache size.
Determines the size of the cache. If it is set to 5, the cache will remember the last five function calls and store their results.
Definition at line 48 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_bb_phi_tautau |
Definition at line 162 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_bb_phi_tautau_e |
Definition at line 166 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_gg_H_ZZ_llnunu |
Definition at line 162 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_gg_H_ZZ_llnunu_e |
Definition at line 166 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_gg_phi_gaga |
Definition at line 162 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_gg_phi_gaga_e |
Definition at line 166 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_gg_phi_tautau |
Definition at line 162 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_gg_phi_tautau_e |
Definition at line 166 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_ggF_H_hh_bbbb |
Definition at line 162 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_ggF_H_hh_bbbb_e |
Definition at line 166 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_ggF_phi_Zga |
Definition at line 162 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_ggF_phi_Zga_e |
Definition at line 166 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_ggFVBF_H_WW_lnulnu |
Definition at line 162 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_ggFVBF_H_WW_lnulnu_e |
Definition at line 166 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_H_hh_bbbb |
Definition at line 162 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_H_hh_bbbb_e |
Definition at line 166 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_H_hh_bblnulnu |
Definition at line 162 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_H_hh_bblnulnu_e |
Definition at line 166 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_H_hh_bbtautau |
Definition at line 162 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_H_hh_bbtautau1 |
Definition at line 162 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_H_hh_bbtautau1_e |
Definition at line 166 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_H_hh_bbtautau_e |
Definition at line 166 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_H_hh_bbVV |
CMS observed \(95\%\) upper cross section limits at 13 TeV, depending on the Higgs mass.
Definition at line 162 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_H_hh_bbVV_e |
ATLAS expected \(95\%\) upper cross section limits at 13 TeV, depending on the Higgs mass.
Definition at line 166 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_H_hh_gagabb |
Definition at line 162 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_H_hh_gagabb_e |
Definition at line 166 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_H_ZZ_llll |
Definition at line 162 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_H_ZZ_llll_e |
Definition at line 166 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_H_ZZ_llnunu |
Definition at line 162 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_H_ZZ_llnunu_e |
Definition at line 166 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_H_ZZ_llqq |
Definition at line 162 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_H_ZZ_llqq_e |
Definition at line 166 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_Hpm_taunu |
CMS observed \(95\%\) upper cross section limits at 13 TeV, depending on the charged Higgs mass.
Definition at line 191 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_Hpm_taunu_e |
CMS expected \(95\%\) upper cross section limits at 13 TeV, depending on the charged Higgs mass.
Definition at line 193 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_phi_bb |
Definition at line 162 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_phi_bb_e |
Definition at line 166 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_phi_Zga_llga |
Definition at line 162 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_phi_Zga_llga_e |
Definition at line 166 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_phi_Zga_qqga |
Definition at line 162 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_pp_phi_Zga_qqga_e |
Definition at line 166 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_VBF_H_ZZ_llnunu |
Definition at line 162 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_VBF_H_ZZ_llnunu_e |
Definition at line 166 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_VBFVH_H_ZZ_llll |
Definition at line 162 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS13_VBFVH_H_ZZ_llll_e |
Definition at line 166 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_bb_phi_bb |
Definition at line 144 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_bb_phi_bb_e |
Definition at line 146 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_bb_phi_tautau |
Definition at line 144 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_bb_phi_tautau_e |
Definition at line 146 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_gg_A_hZ_bbll |
Definition at line 144 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_gg_A_hZ_bbll_e |
Definition at line 146 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_gg_A_hZ_tautaull |
Definition at line 144 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_gg_A_hZ_tautaull_e |
CMS expected \(95\%\) upper cross section limits at 8 TeV, depending on the Higgs mass.
Definition at line 146 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_gg_H_hh_bbtautau |
Definition at line 144 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_gg_H_hh_bbtautau_e |
Definition at line 146 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_gg_phi_gaga |
Definition at line 144 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_gg_phi_gaga_e |
Definition at line 146 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_gg_phi_tautau |
Definition at line 144 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_gg_phi_tautau_e |
Definition at line 146 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_mu_pp_H_VV |
CMS observed \(95\%\) upper signal strength limits at 8 TeV, depending on the Higgs mass.
Definition at line 140 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_mu_pp_H_VV_e |
CMS expected \(95\%\) upper signal strength limits at 8 TeV, depending on the Higgs mass.
Definition at line 142 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_pp_A_HZ_bbll |
Definition at line 144 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_pp_A_HZ_tautaull |
Definition at line 144 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_pp_A_Zga_llga |
Definition at line 144 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_pp_A_Zga_llga_e |
Definition at line 146 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_pp_H_AZ_bbll |
Definition at line 144 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_pp_H_AZ_tautaull |
CMS observed \(95\%\) upper cross section limits at 8 TeV, depending on the Higgs mass.
Definition at line 144 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_pp_H_hh |
Definition at line 144 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_pp_H_hh_bbbb |
Definition at line 144 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_pp_H_hh_bbbb_e |
Definition at line 146 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_pp_H_hh_e |
Definition at line 146 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_pp_H_hh_gagabb |
Definition at line 144 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_pp_H_hh_gagabb_e |
Definition at line 146 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_pp_Hp_taunu |
Definition at line 183 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_pp_Hp_taunu_e |
Definition at line 185 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_pp_Hp_tb |
CMS observed \(95\%\) upper cross section limits at 8 TeV, depending on the charged Higgs mass.
Definition at line 183 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_pp_Hp_tb_e |
CMS expected \(95\%\) upper cross section limits at 8 TeV, depending on the charged Higgs mass.
Definition at line 185 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::CMS8_pp_phi_Zga |
Definition at line 144 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::csrA_bottom_13 |
Production cross section ratio tables at 13 TeV obtained with HIGLU 4.34, depending on the Higgs mass.
Definition at line 134 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::csrA_bottom_8 |
Production cross section ratio tables at 8 TeV obtained with HIGLU 4.34, depending on the Higgs mass.
Definition at line 132 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::csrA_top_13 |
Definition at line 134 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::csrA_top_8 |
Definition at line 132 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::csrH_bottom_13 |
Definition at line 134 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::csrH_bottom_8 |
Definition at line 132 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::csrH_top_13 |
Definition at line 134 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::csrH_top_8 |
Definition at line 132 of file THDMcache.h.
|
private |
Definition at line 3444 of file THDMcache.h.
| double THDMcache::g1_at_Q |
Definition at line 3392 of file THDMcache.h.
| double THDMcache::g2_at_Q |
Definition at line 3393 of file THDMcache.h.
| double THDMcache::g3_at_Q |
Definition at line 3394 of file THDMcache.h.
|
mutableprivate |
Definition at line 3852 of file THDMcache.h.
| double THDMcache::Gamma_AZga |
Definition at line 3219 of file THDMcache.h.
| double THDMcache::Gamma_h |
Total h decay rate in the THDM. This is \(\Gamma_h\)
Definition at line 2904 of file THDMcache.h.
| double THDMcache::GammaAtot |
Total decay width of the CP-odd Higgs \(A\). This is \(\Gamma_A\)
Definition at line 3272 of file THDMcache.h.
| double THDMcache::GammaHptot |
Total decay width of the charged Higgs \(H^+\).
Definition at line 3389 of file THDMcache.h.
| double THDMcache::GammaHtot |
Total decay width of the heavy CP-even Higgs \(H\). This is \(\Gamma_H\)
Definition at line 3036 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::GammaHtot_SM |
Total SM decay width (obtained with HDECAY 6.10), depending on the Higgs mass.
Definition at line 110 of file THDMcache.h.
| double THDMcache::GammaHtotSM |
Definition at line 2940 of file THDMcache.h.
| double THDMcache::ggF_A_gaga_TH13 |
Cross section times branching ratio for the process \(gg\to A\to \gamma \gamma\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{gg\to A}\cdot BR^{\text{THDM}}(A\to \gamma \gamma)\)
Definition at line 3256 of file THDMcache.h.
| double THDMcache::ggF_A_gaga_TH8 |
Cross section times branching ratio for the process \(gg\to A\to \gamma\gamma\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{gg\to A}\cdot BR^{\text{THDM}}(A\to \gamma\gamma)\)
Definition at line 3228 of file THDMcache.h.
| double THDMcache::ggF_A_hZ_bbll_TH8 |
Cross section times branching ratio for the process \(gg\to A\to hZ \to b\bar b \ell \ell\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{gg\to A}\cdot BR^{\text{THDM}}(A\to hZ \to b\bar b \ell \ell)\)
Definition at line 3234 of file THDMcache.h.
| double THDMcache::ggF_A_hZ_bbZ_TH13 |
Cross section times branching ratio for the process \(gg\to A\to hZ\to b\bar b Z\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{gg\to A}\cdot BR^{\text{THDM}}(A\to hZ\to b\bar b Z)\)
Definition at line 3262 of file THDMcache.h.
| double THDMcache::ggF_A_hZ_bbZ_TH8 |
Cross section times branching ratio for the process \(gg\to A\to hZ \to b\bar b Z\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{gg\to A}\cdot BR^{\text{THDM}}(A\to hZ \to b\bar b Z)\)
Definition at line 3236 of file THDMcache.h.
| double THDMcache::ggF_A_hZ_tautaull_TH8 |
Cross section times branching ratio for the process \(gg\to A\to hZ \to \tau \tau \ell \ell\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{gg\to A}\cdot BR^{\text{THDM}}(A\to hZ \to \tau \tau \ell \ell)\)
Definition at line 3238 of file THDMcache.h.
| double THDMcache::ggF_A_hZ_tautauZ_TH8 |
Cross section times branching ratio for the process \(gg\to A\to hZ \to \tau \tau Z\) at the LHC with 8 TeV. This is
Definition at line 3240 of file THDMcache.h.
| double THDMcache::ggF_A_hZ_TH8 |
Cross section times branching ratio for the process \(gg\to A\to hZ\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{gg\to A}\cdot BR^{\text{THDM}}(A\to hZ)\)
Definition at line 3232 of file THDMcache.h.
| double THDMcache::ggF_A_tautau_TH13 |
Cross section times branching ratio for the process \(gg\to A\to \tau \tauZ\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{gg\to A}\cdot BR^{\text{THDM}}(A\to \tau \tau)\)
Definition at line 3250 of file THDMcache.h.
| double THDMcache::ggF_A_tautau_TH8 |
Cross section times branching ratio for the process \(gg\to A\to \tau\tau\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{gg\to A}\cdot BR^{\text{THDM}}(A\to \tau\tau)\)
Definition at line 3222 of file THDMcache.h.
| double THDMcache::ggF_A_tt_TH8 |
Cross section times branching ratio for the process \(gg\to A\to t\bar t\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{gg\to A}\cdot BR^{\text{THDM}}(A\to t\bar t)\)
Definition at line 3242 of file THDMcache.h.
| double THDMcache::ggF_A_Zga_TH13 |
Cross section times branching ratio for the process \(gg\to A\to Z\gamma\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{gg\to A}\cdot BR^{\text{THDM}}(A\to Z\gamma)\)
Definition at line 3260 of file THDMcache.h.
| double THDMcache::ggF_H_gaga_TH13 |
Cross section times branching ratio for the process \(gg\to H\to \gamma\gamma\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{gg\to H}\cdot BR^{\text{THDM}}(H\to \gamma\gamma)\)
Definition at line 2986 of file THDMcache.h.
| double THDMcache::ggF_H_gaga_TH8 |
Cross section times branching ratio for the process \(gg\to H\to \gamma\gamma\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{gg\to H}\cdot BR^{\text{THDM}}(H\to \gamma\gamma)\)
Definition at line 2948 of file THDMcache.h.
| double THDMcache::ggF_H_hh_bbbb_TH13 |
Cross section times branching ratio for the process \(gg\to H\to hh\to b\bar b b\bar b\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{gg\to H}\cdot BR^{\text{THDM}}(H\to hh\to b\bar b b\bar b)\)
Definition at line 3020 of file THDMcache.h.
| double THDMcache::ggF_H_hh_bbtautau_TH8 |
Cross section times branching ratio for the process \(gg\to H\to hh\to b\bar b \tau\tau\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{gg\to H}\cdot BR^{\text{THDM}}(H\to hh\to b\bar b \tau\tau)\)
Definition at line 2966 of file THDMcache.h.
| double THDMcache::ggF_H_hh_TH13 |
Cross section times branching ratio for the process \(gg\to H\to hh\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{gg\to H}\cdot BR^{\text{THDM}}(H\to hh)\)
Definition at line 3014 of file THDMcache.h.
| double THDMcache::ggF_H_hh_TH8 |
Cross section times branching ratio for the process \(gg\to H\to hh\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{gg\to H}\cdot BR^{\text{THDM}}(H\to hh)\)
Definition at line 2962 of file THDMcache.h.
| double THDMcache::ggF_H_tautau_TH13 |
Cross section times branching ratio for the process \(gg\to H\to \tau\tau\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{gg\to H}\cdot BR^{\text{THDM}}(H\to \tau\tau)\)
Definition at line 2980 of file THDMcache.h.
| double THDMcache::ggF_H_tautau_TH8 |
Cross section times branching ratio for the process \(gg\to H\to \tau\tau\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{gg\to H}\cdot BR^{\text{THDM}}(H\to \tau\tau)\)
Definition at line 2942 of file THDMcache.h.
| double THDMcache::ggF_H_tt_TH8 |
Cross section times branching ratio for the process \(gg\to H\to t\bar t\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{gg\to H}\cdot BR^{\text{THDM}}(H\to t\bar t)\)
Definition at line 2972 of file THDMcache.h.
| double THDMcache::ggF_H_WW_TH13 |
Cross section times branching ratio for the process \(gg\to H\to WW\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{gg\to H}\cdot BR^{\text{THDM}}(H\to WW)\)
Definition at line 3006 of file THDMcache.h.
| double THDMcache::ggF_H_WW_TH8 |
Cross section times branching ratio for the process \(gg\to H\to WW\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{gg\to H}\cdot BR^{\text{THDM}}(H\to WW)\)
Definition at line 2958 of file THDMcache.h.
| double THDMcache::ggF_H_Zga_TH13 |
Cross section times branching ratio for the process \(gg\to H\to Z\gamma\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{gg\to H}\cdot BR^{\text{THDM}}(H\to Z\gamma)\)
Definition at line 2990 of file THDMcache.h.
| double THDMcache::ggF_H_ZZ_llll_TH13 |
Cross section times branching ratio for the process \(gg\to H\to ZZ\to 4\ell\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{gg\to H}\cdot BR^{\text{THDM}}(H\to ZZ\to 4\ell)\)
Definition at line 2998 of file THDMcache.h.
| double THDMcache::ggF_H_ZZ_TH13 |
Cross section times branching ratio for the process \(gg\to H\to ZZ\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{gg\to H}\cdot BR^{\text{THDM}}(H\to ZZ)\)
Definition at line 2994 of file THDMcache.h.
| double THDMcache::ggF_H_ZZ_TH8 |
Cross section times branching ratio for the process \(gg\to H\to ZZ\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{gg\to H}\cdot BR^{\text{THDM}}(H\to ZZ)\)
Definition at line 2954 of file THDMcache.h.
| double THDMcache::ggF_tth13 |
Ratio of THDM and SM cross sections for ggF and tth production of h at 13 TeV. This is \(\sigma^{\text THDM}_{\text ggF+tth}/\sigma^{\text SM}_{\text ggF+tth}\)
Definition at line 2896 of file THDMcache.h.
| double THDMcache::ggF_tth8 |
Ratio of THDM and SM cross sections for ggF and tth production of h at 8 TeV. This is \(\sigma^{\text THDM}_{\text ggF+tth}/\sigma^{\text SM}_{\text ggF+tth}\)
Definition at line 2894 of file THDMcache.h.
| double THDMcache::ggF_VBF_H_WW_lnulnu_TH13 |
Cross section times branching ratio for the process \((gg+VV)\to H\to WW\to \ell \nu \ell \nu\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{(gg+VV)\to H}\cdot BR^{\text{THDM}}(H\to WW\to \ell \nu \ell \nu)\)
Definition at line 3010 of file THDMcache.h.
|
mutableprivate |
Definition at line 3851 of file THDMcache.h.
|
mutableprivate |
Definition at line 3859 of file THDMcache.h.
|
mutableprivate |
Definition at line 3862 of file THDMcache.h.
|
mutableprivate |
Definition at line 3856 of file THDMcache.h.
|
mutableprivate |
Definition at line 3857 of file THDMcache.h.
|
mutableprivate |
Definition at line 3864 of file THDMcache.h.
|
mutableprivate |
Definition at line 3860 of file THDMcache.h.
|
mutableprivate |
Definition at line 3854 of file THDMcache.h.
|
mutableprivate |
Definition at line 3863 of file THDMcache.h.
|
mutableprivate |
Definition at line 3858 of file THDMcache.h.
|
mutableprivate |
Definition at line 3861 of file THDMcache.h.
|
mutableprivate |
Definition at line 3855 of file THDMcache.h.
|
mutableprivate |
Definition at line 3769 of file THDMcache.h.
|
mutableprivate |
Definition at line 3770 of file THDMcache.h.
|
mutableprivate |
Definition at line 3771 of file THDMcache.h.
|
mutableprivate |
Definition at line 3772 of file THDMcache.h.
|
mutableprivate |
Definition at line 3773 of file THDMcache.h.
|
mutableprivate |
Definition at line 3774 of file THDMcache.h.
|
mutableprivate |
Definition at line 3775 of file THDMcache.h.
|
mutableprivate |
Definition at line 3776 of file THDMcache.h.
|
mutableprivate |
Definition at line 3777 of file THDMcache.h.
|
mutableprivate |
Definition at line 3778 of file THDMcache.h.
|
mutableprivate |
Definition at line 3779 of file THDMcache.h.
|
mutableprivate |
Definition at line 3780 of file THDMcache.h.
|
mutableprivate |
Definition at line 3781 of file THDMcache.h.
|
mutableprivate |
Definition at line 3782 of file THDMcache.h.
|
mutableprivate |
Definition at line 3783 of file THDMcache.h.
|
mutableprivate |
Definition at line 3784 of file THDMcache.h.
|
mutableprivate |
Definition at line 3785 of file THDMcache.h.
|
mutableprivate |
Definition at line 3786 of file THDMcache.h.
|
mutableprivate |
Definition at line 3787 of file THDMcache.h.
|
mutableprivate |
Definition at line 3788 of file THDMcache.h.
|
mutableprivate |
Definition at line 3751 of file THDMcache.h.
|
mutableprivate |
Definition at line 3752 of file THDMcache.h.
|
mutableprivate |
Definition at line 3789 of file THDMcache.h.
|
mutableprivate |
Definition at line 3790 of file THDMcache.h.
|
mutableprivate |
Definition at line 3791 of file THDMcache.h.
|
mutableprivate |
Definition at line 3792 of file THDMcache.h.
|
mutableprivate |
Definition at line 3793 of file THDMcache.h.
|
mutableprivate |
Definition at line 3794 of file THDMcache.h.
|
mutableprivate |
Definition at line 3795 of file THDMcache.h.
|
mutableprivate |
Definition at line 3796 of file THDMcache.h.
|
mutableprivate |
Definition at line 3797 of file THDMcache.h.
|
mutableprivate |
Definition at line 3798 of file THDMcache.h.
|
mutableprivate |
Definition at line 3799 of file THDMcache.h.
|
mutableprivate |
Definition at line 3800 of file THDMcache.h.
|
mutableprivate |
Definition at line 3801 of file THDMcache.h.
|
mutableprivate |
Definition at line 3802 of file THDMcache.h.
|
mutableprivate |
Definition at line 3803 of file THDMcache.h.
|
mutableprivate |
Definition at line 3804 of file THDMcache.h.
|
mutableprivate |
Definition at line 3805 of file THDMcache.h.
|
mutableprivate |
Definition at line 3806 of file THDMcache.h.
|
mutableprivate |
Definition at line 3807 of file THDMcache.h.
|
mutableprivate |
Definition at line 3808 of file THDMcache.h.
|
mutableprivate |
Definition at line 3753 of file THDMcache.h.
|
mutableprivate |
Definition at line 3754 of file THDMcache.h.
|
mutableprivate |
Definition at line 3809 of file THDMcache.h.
|
mutableprivate |
Definition at line 3810 of file THDMcache.h.
|
mutableprivate |
Definition at line 3811 of file THDMcache.h.
|
mutableprivate |
Definition at line 3812 of file THDMcache.h.
|
mutableprivate |
Definition at line 3813 of file THDMcache.h.
|
mutableprivate |
Definition at line 3814 of file THDMcache.h.
|
mutableprivate |
Definition at line 3815 of file THDMcache.h.
|
mutableprivate |
Definition at line 3816 of file THDMcache.h.
|
mutableprivate |
Definition at line 3817 of file THDMcache.h.
|
mutableprivate |
Definition at line 3818 of file THDMcache.h.
|
mutableprivate |
Definition at line 3819 of file THDMcache.h.
|
mutableprivate |
Definition at line 3820 of file THDMcache.h.
|
mutableprivate |
Definition at line 3821 of file THDMcache.h.
|
mutableprivate |
Definition at line 3822 of file THDMcache.h.
|
mutableprivate |
Definition at line 3823 of file THDMcache.h.
|
mutableprivate |
Definition at line 3824 of file THDMcache.h.
|
mutableprivate |
Definition at line 3825 of file THDMcache.h.
|
mutableprivate |
Definition at line 3826 of file THDMcache.h.
|
mutableprivate |
Definition at line 3827 of file THDMcache.h.
|
mutableprivate |
Definition at line 3828 of file THDMcache.h.
|
mutableprivate |
Definition at line 3755 of file THDMcache.h.
|
mutableprivate |
Definition at line 3756 of file THDMcache.h.
|
mutableprivate |
Definition at line 3829 of file THDMcache.h.
|
mutableprivate |
Definition at line 3830 of file THDMcache.h.
|
mutableprivate |
Definition at line 3757 of file THDMcache.h.
|
mutableprivate |
Definition at line 3758 of file THDMcache.h.
|
mutableprivate |
Definition at line 3759 of file THDMcache.h.
|
mutableprivate |
Definition at line 3760 of file THDMcache.h.
|
mutableprivate |
Definition at line 3761 of file THDMcache.h.
|
mutableprivate |
Definition at line 3762 of file THDMcache.h.
|
mutableprivate |
Definition at line 3763 of file THDMcache.h.
|
mutableprivate |
Definition at line 3764 of file THDMcache.h.
|
mutableprivate |
Definition at line 3765 of file THDMcache.h.
|
mutableprivate |
Definition at line 3766 of file THDMcache.h.
|
mutableprivate |
Definition at line 3767 of file THDMcache.h.
|
mutableprivate |
Definition at line 3768 of file THDMcache.h.
|
mutableprivate |
Definition at line 3564 of file THDMcache.h.
|
mutableprivate |
Definition at line 3566 of file THDMcache.h.
|
mutableprivate |
Definition at line 3567 of file THDMcache.h.
|
mutableprivate |
Definition at line 3565 of file THDMcache.h.
|
mutableprivate |
Definition at line 3563 of file THDMcache.h.
|
mutableprivate |
Definition at line 3569 of file THDMcache.h.
|
mutableprivate |
Definition at line 3568 of file THDMcache.h.
|
mutableprivate |
Definition at line 3584 of file THDMcache.h.
|
mutableprivate |
Definition at line 3583 of file THDMcache.h.
|
mutableprivate |
Definition at line 3572 of file THDMcache.h.
|
mutableprivate |
Definition at line 3571 of file THDMcache.h.
|
mutableprivate |
Definition at line 3590 of file THDMcache.h.
|
mutableprivate |
Definition at line 3589 of file THDMcache.h.
|
mutableprivate |
Definition at line 3588 of file THDMcache.h.
|
mutableprivate |
Definition at line 3587 of file THDMcache.h.
|
mutableprivate |
Definition at line 3582 of file THDMcache.h.
|
mutableprivate |
Definition at line 3581 of file THDMcache.h.
|
mutableprivate |
Definition at line 3586 of file THDMcache.h.
|
mutableprivate |
Definition at line 3585 of file THDMcache.h.
|
mutableprivate |
Definition at line 3580 of file THDMcache.h.
|
mutableprivate |
Definition at line 3579 of file THDMcache.h.
|
mutableprivate |
Definition at line 3574 of file THDMcache.h.
|
mutableprivate |
Definition at line 3573 of file THDMcache.h.
|
mutableprivate |
Definition at line 3576 of file THDMcache.h.
|
mutableprivate |
Definition at line 3575 of file THDMcache.h.
|
mutableprivate |
Definition at line 3578 of file THDMcache.h.
|
mutableprivate |
Definition at line 3577 of file THDMcache.h.
|
mutableprivate |
Definition at line 3598 of file THDMcache.h.
|
mutableprivate |
Definition at line 3597 of file THDMcache.h.
|
mutableprivate |
Definition at line 3596 of file THDMcache.h.
|
mutableprivate |
Definition at line 3595 of file THDMcache.h.
|
mutableprivate |
Definition at line 3594 of file THDMcache.h.
|
mutableprivate |
Definition at line 3593 of file THDMcache.h.
|
mutableprivate |
Definition at line 3592 of file THDMcache.h.
|
mutableprivate |
Definition at line 3591 of file THDMcache.h.
|
mutableprivate |
Definition at line 3706 of file THDMcache.h.
|
mutableprivate |
Definition at line 3707 of file THDMcache.h.
|
mutableprivate |
Definition at line 3633 of file THDMcache.h.
|
mutableprivate |
Definition at line 3634 of file THDMcache.h.
|
mutableprivate |
Definition at line 3660 of file THDMcache.h.
|
mutableprivate |
Definition at line 3661 of file THDMcache.h.
|
mutableprivate |
Definition at line 3605 of file THDMcache.h.
|
mutableprivate |
Definition at line 3606 of file THDMcache.h.
|
mutableprivate |
Definition at line 3712 of file THDMcache.h.
|
mutableprivate |
Definition at line 3713 of file THDMcache.h.
|
mutableprivate |
Definition at line 3637 of file THDMcache.h.
|
mutableprivate |
Definition at line 3638 of file THDMcache.h.
|
mutableprivate |
Definition at line 3654 of file THDMcache.h.
|
mutableprivate |
Definition at line 3655 of file THDMcache.h.
|
mutableprivate |
Definition at line 3849 of file THDMcache.h.
|
mutableprivate |
Definition at line 3625 of file THDMcache.h.
|
mutableprivate |
Definition at line 3626 of file THDMcache.h.
|
mutableprivate |
Definition at line 3609 of file THDMcache.h.
|
mutableprivate |
Definition at line 3610 of file THDMcache.h.
|
mutableprivate |
Definition at line 3647 of file THDMcache.h.
|
mutableprivate |
Definition at line 3648 of file THDMcache.h.
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mutableprivate |
Definition at line 3607 of file THDMcache.h.
|
mutableprivate |
Definition at line 3608 of file THDMcache.h.
|
mutableprivate |
Definition at line 3704 of file THDMcache.h.
|
mutableprivate |
Definition at line 3705 of file THDMcache.h.
|
mutableprivate |
Definition at line 3621 of file THDMcache.h.
|
mutableprivate |
Definition at line 3622 of file THDMcache.h.
|
mutableprivate |
Definition at line 3645 of file THDMcache.h.
|
mutableprivate |
Definition at line 3646 of file THDMcache.h.
|
mutableprivate |
Definition at line 3613 of file THDMcache.h.
|
mutableprivate |
Definition at line 3614 of file THDMcache.h.
|
mutableprivate |
Definition at line 3688 of file THDMcache.h.
|
mutableprivate |
Definition at line 3689 of file THDMcache.h.
|
mutableprivate |
Definition at line 3692 of file THDMcache.h.
|
mutableprivate |
Definition at line 3693 of file THDMcache.h.
|
mutableprivate |
Definition at line 3617 of file THDMcache.h.
|
mutableprivate |
Definition at line 3618 of file THDMcache.h.
|
mutableprivate |
Definition at line 3678 of file THDMcache.h.
|
mutableprivate |
Definition at line 3679 of file THDMcache.h.
|
mutableprivate |
Definition at line 3668 of file THDMcache.h.
|
mutableprivate |
Definition at line 3669 of file THDMcache.h.
|
mutableprivate |
Definition at line 3676 of file THDMcache.h.
|
mutableprivate |
Definition at line 3677 of file THDMcache.h.
|
mutableprivate |
Definition at line 3724 of file THDMcache.h.
|
mutableprivate |
Definition at line 3725 of file THDMcache.h.
|
mutableprivate |
Definition at line 3682 of file THDMcache.h.
|
mutableprivate |
Definition at line 3683 of file THDMcache.h.
|
mutableprivate |
Definition at line 3686 of file THDMcache.h.
|
mutableprivate |
Definition at line 3687 of file THDMcache.h.
|
mutableprivate |
Definition at line 3672 of file THDMcache.h.
|
mutableprivate |
Definition at line 3673 of file THDMcache.h.
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Definition at line 3714 of file THDMcache.h.
|
mutableprivate |
Definition at line 3715 of file THDMcache.h.
|
mutableprivate |
Definition at line 3639 of file THDMcache.h.
|
mutableprivate |
Definition at line 3640 of file THDMcache.h.
|
mutableprivate |
Definition at line 3658 of file THDMcache.h.
|
mutableprivate |
Definition at line 3659 of file THDMcache.h.
|
mutableprivate |
Definition at line 3603 of file THDMcache.h.
|
mutableprivate |
Definition at line 3604 of file THDMcache.h.
|
mutableprivate |
Definition at line 3710 of file THDMcache.h.
|
mutableprivate |
Definition at line 3711 of file THDMcache.h.
|
mutableprivate |
Definition at line 3635 of file THDMcache.h.
|
mutableprivate |
Definition at line 3636 of file THDMcache.h.
|
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Definition at line 3611 of file THDMcache.h.
|
mutableprivate |
Definition at line 3612 of file THDMcache.h.
|
mutableprivate |
Definition at line 3666 of file THDMcache.h.
|
mutableprivate |
Definition at line 3667 of file THDMcache.h.
|
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Definition at line 3738 of file THDMcache.h.
|
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Definition at line 3739 of file THDMcache.h.
|
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Definition at line 3720 of file THDMcache.h.
|
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Definition at line 3721 of file THDMcache.h.
|
mutableprivate |
Definition at line 3734 of file THDMcache.h.
|
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Definition at line 3735 of file THDMcache.h.
|
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Definition at line 3623 of file THDMcache.h.
|
mutableprivate |
Definition at line 3624 of file THDMcache.h.
|
mutableprivate |
Definition at line 3649 of file THDMcache.h.
|
mutableprivate |
Definition at line 3651 of file THDMcache.h.
|
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Definition at line 3643 of file THDMcache.h.
|
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Definition at line 3644 of file THDMcache.h.
|
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Definition at line 3650 of file THDMcache.h.
|
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Definition at line 3652 of file THDMcache.h.
|
mutableprivate |
Definition at line 3698 of file THDMcache.h.
|
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Definition at line 3699 of file THDMcache.h.
|
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Definition at line 3736 of file THDMcache.h.
|
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Definition at line 3737 of file THDMcache.h.
|
mutableprivate |
Definition at line 3746 of file THDMcache.h.
|
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Definition at line 3747 of file THDMcache.h.
|
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Definition at line 3744 of file THDMcache.h.
|
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Definition at line 3745 of file THDMcache.h.
|
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Definition at line 3742 of file THDMcache.h.
|
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Definition at line 3743 of file THDMcache.h.
|
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Definition at line 3748 of file THDMcache.h.
|
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Definition at line 3749 of file THDMcache.h.
|
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Definition at line 3627 of file THDMcache.h.
|
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Definition at line 3628 of file THDMcache.h.
|
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Definition at line 3700 of file THDMcache.h.
|
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Definition at line 3701 of file THDMcache.h.
|
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Definition at line 3740 of file THDMcache.h.
|
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Definition at line 3741 of file THDMcache.h.
|
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Definition at line 3702 of file THDMcache.h.
|
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Definition at line 3703 of file THDMcache.h.
|
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Definition at line 3696 of file THDMcache.h.
|
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Definition at line 3697 of file THDMcache.h.
|
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Definition at line 3728 of file THDMcache.h.
|
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Definition at line 3729 of file THDMcache.h.
|
mutableprivate |
Definition at line 3722 of file THDMcache.h.
|
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Definition at line 3723 of file THDMcache.h.
|
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Definition at line 3732 of file THDMcache.h.
|
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Definition at line 3733 of file THDMcache.h.
|
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Definition at line 3834 of file THDMcache.h.
|
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Definition at line 3835 of file THDMcache.h.
|
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Definition at line 3844 of file THDMcache.h.
|
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Definition at line 3845 of file THDMcache.h.
|
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Definition at line 3846 of file THDMcache.h.
|
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Definition at line 3847 of file THDMcache.h.
|
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Definition at line 3838 of file THDMcache.h.
|
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Definition at line 3839 of file THDMcache.h.
|
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Definition at line 3840 of file THDMcache.h.
|
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Definition at line 3841 of file THDMcache.h.
|
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Definition at line 3832 of file THDMcache.h.
|
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Definition at line 3833 of file THDMcache.h.
|
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Definition at line 3842 of file THDMcache.h.
|
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Definition at line 3843 of file THDMcache.h.
|
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Definition at line 3836 of file THDMcache.h.
|
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Definition at line 3837 of file THDMcache.h.
|
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Definition at line 3708 of file THDMcache.h.
|
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Definition at line 3709 of file THDMcache.h.
|
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Definition at line 3662 of file THDMcache.h.
|
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Definition at line 3663 of file THDMcache.h.
|
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Definition at line 3599 of file THDMcache.h.
|
mutableprivate |
Definition at line 3600 of file THDMcache.h.
|
mutableprivate |
Definition at line 3631 of file THDMcache.h.
|
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Definition at line 3632 of file THDMcache.h.
|
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Definition at line 3629 of file THDMcache.h.
|
mutableprivate |
Definition at line 3630 of file THDMcache.h.
|
mutableprivate |
Definition at line 3664 of file THDMcache.h.
|
mutableprivate |
Definition at line 3665 of file THDMcache.h.
|
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Definition at line 3601 of file THDMcache.h.
|
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Definition at line 3602 of file THDMcache.h.
|
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Definition at line 3716 of file THDMcache.h.
|
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Definition at line 3717 of file THDMcache.h.
|
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Definition at line 3718 of file THDMcache.h.
|
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Definition at line 3719 of file THDMcache.h.
|
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Definition at line 3656 of file THDMcache.h.
|
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Definition at line 3657 of file THDMcache.h.
|
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Definition at line 3615 of file THDMcache.h.
|
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Definition at line 3616 of file THDMcache.h.
|
mutableprivate |
Definition at line 3690 of file THDMcache.h.
|
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Definition at line 3691 of file THDMcache.h.
|
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Definition at line 3694 of file THDMcache.h.
|
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Definition at line 3695 of file THDMcache.h.
|
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Definition at line 3619 of file THDMcache.h.
|
mutableprivate |
Definition at line 3620 of file THDMcache.h.
|
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Definition at line 3680 of file THDMcache.h.
|
mutableprivate |
Definition at line 3681 of file THDMcache.h.
|
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Definition at line 3670 of file THDMcache.h.
|
mutableprivate |
Definition at line 3671 of file THDMcache.h.
|
mutableprivate |
Definition at line 3726 of file THDMcache.h.
|
mutableprivate |
Definition at line 3727 of file THDMcache.h.
|
mutableprivate |
Definition at line 3684 of file THDMcache.h.
|
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Definition at line 3685 of file THDMcache.h.
|
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Definition at line 3674 of file THDMcache.h.
|
mutableprivate |
Definition at line 3675 of file THDMcache.h.
|
mutableprivate |
Definition at line 3730 of file THDMcache.h.
|
mutableprivate |
Definition at line 3731 of file THDMcache.h.
|
mutableprivate |
Definition at line 3570 of file THDMcache.h.
|
mutableprivate |
Definition at line 3878 of file THDMcache.h.
| double THDMcache::lambda1_at_Q |
Definition at line 3403 of file THDMcache.h.
| double THDMcache::lambda2_at_Q |
Definition at line 3404 of file THDMcache.h.
| double THDMcache::lambda3_at_Q |
Definition at line 3405 of file THDMcache.h.
| double THDMcache::lambda4_at_Q |
Definition at line 3406 of file THDMcache.h.
| double THDMcache::lambda5_at_Q |
Definition at line 3407 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::log_cs_bbA_13 |
CP-odd Higgs production cross section tables at 13 TeV obtained with HIGLU 4.34, depending on the Higgs mass.
Definition at line 126 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::log_cs_bbA_8 |
CP-odd Higgs production cross section tables at 8 TeV obtained with HIGLU 4.34, depending on the Higgs mass.
Definition at line 124 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::log_cs_bbH_13 |
SM Higgs production cross section table at 13 TeV obtained with SusHi 1.5, depending on the Higgs mass.
Definition at line 122 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::log_cs_bbH_8 |
SM Higgs production cross section table at 8 TeV obtained with SusHi 1.5, depending on the Higgs mass.
Definition at line 120 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::log_cs_ggA_13 |
Definition at line 126 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::log_cs_ggA_8 |
Definition at line 124 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::log_cs_ggH_13 |
Definition at line 114 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::log_cs_ggH_8 |
Definition at line 112 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::log_cs_ggHp_13 |
Charged Higgs production cross section table at 13 TeV from LHCHXSWGMSSMCharged, depending on the charged Higgs mass and logtb.
Definition at line 130 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::log_cs_ggHp_8 |
Charged Higgs production cross section table at 8 TeV from LHCHXSWGMSSMCharged, depending on the charged Higgs mass and logtb.
Definition at line 128 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::log_cs_ttA_13 |
Definition at line 126 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::log_cs_ttA_8 |
Definition at line 124 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::log_cs_ttH_13 |
SM Higgs production cross section table at 13 TeV obtained with MadGraph 5, depending on the Higgs mass.
Definition at line 118 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::log_cs_ttH_8 |
SM Higgs production cross section table at 8 TeV obtained with MadGraph 5, depending on the Higgs mass.
Definition at line 116 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::log_cs_VBF_13 |
Definition at line 114 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::log_cs_VBF_8 |
Definition at line 112 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::log_cs_WH_13 |
Definition at line 114 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::log_cs_WH_8 |
Definition at line 112 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::log_cs_ZH_13 |
SM Higgs production cross section tables at 13 TeV from the LHC Higgs Cross Section Working Group, depending on the Higgs mass.
Definition at line 114 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::log_cs_ZH_8 |
SM Higgs production cross section tables at 8 TeV from the LHC Higgs Cross Section Working Group, depending on the Higgs mass.
Definition at line 112 of file THDMcache.h.
|
private |
Definition at line 3429 of file THDMcache.h.
| double THDMcache::m11_2_at_Q |
Definition at line 3400 of file THDMcache.h.
|
private |
Definition at line 3431 of file THDMcache.h.
| double THDMcache::m12_2_at_Q |
Definition at line 3402 of file THDMcache.h.
| double THDMcache::m22_2_at_Q |
Definition at line 3401 of file THDMcache.h.
|
private |
Definition at line 3441 of file THDMcache.h.
|
private |
Definition at line 3449 of file THDMcache.h.
|
private |
Definition at line 3451 of file THDMcache.h.
|
private |
Definition at line 3455 of file THDMcache.h.
|
private |
Definition at line 3456 of file THDMcache.h.
|
private |
Definition at line 3440 of file THDMcache.h.
|
private |
Definition at line 3438 of file THDMcache.h.
|
private |
Definition at line 3439 of file THDMcache.h.
|
private |
Definition at line 3442 of file THDMcache.h.
|
private |
Definition at line 3453 of file THDMcache.h.
|
private |
Definition at line 3458 of file THDMcache.h.
|
private |
Definition at line 3452 of file THDMcache.h.
|
private |
Definition at line 3448 of file THDMcache.h.
|
private |
Definition at line 3450 of file THDMcache.h.
|
private |
Definition at line 3454 of file THDMcache.h.
| double THDMcache::mu_pp_H_VV_TH8 |
Signal strength for the process \(pp\to H\to VV\) with $VV=WW,ZZ$ at the LHC with 8 TeV. This is \(\mu_H^{\text{THDM}}(H\to VV)=[\sigma^{\text{THDM}}_{pp\to H}\cdot BR^{\text{THDM}}(H\to VV)] / [\sigma^{\text{SM}}_{pp\to H}\cdot BR^{\text{SM}}(H\to VV)]\)
Definition at line 2952 of file THDMcache.h.
|
private |
Definition at line 3443 of file THDMcache.h.
|
private |
Definition at line 3420 of file THDMcache.h.
|
private |
Definition at line 3421 of file THDMcache.h.
|
private |
Definition at line 3422 of file THDMcache.h.
|
private |
Definition at line 3423 of file THDMcache.h.
|
private |
Definition at line 3424 of file THDMcache.h.
|
private |
Definition at line 3418 of file THDMcache.h.
|
private |
Definition at line 3419 of file THDMcache.h.
|
private |
Definition at line 3425 of file THDMcache.h.
|
private |
Definition at line 3416 of file THDMcache.h.
|
private |
Definition at line 3457 of file THDMcache.h.
| double THDMcache::pp_A_bb_TH13 |
Cross section times branching ratio for the process \(pp\to A\to b\bar b\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{pp\to A}\cdot BR^{\text{THDM}}(A\to b\bar b)\)
Definition at line 3270 of file THDMcache.h.
| double THDMcache::pp_A_gaga_TH13 |
Cross section times branching ratio for the process \(pp\to A\to \gamma \gamma\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{pp\to A}\cdot BR^{\text{THDM}}(A\to \gamma \gamma)\)
Definition at line 3254 of file THDMcache.h.
| double THDMcache::pp_A_gaga_TH8 |
Cross section times branching ratio for the process \(pp\to A\to \gamma\gamma\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{pp\to A}\cdot BR^{\text{THDM}}(A\to \gamma\gamma)\)
Definition at line 3226 of file THDMcache.h.
| double THDMcache::pp_A_HZ_bbll_TH8 |
Cross section times branching ratio for the process \(pp\to A\to HZ\to b\bar b \ell \ell\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{pp\to A}\cdot BR^{\text{THDM}}(A\to HZ\to b\bar b \ell \ell)\)
Definition at line 3246 of file THDMcache.h.
| double THDMcache::pp_A_HZ_tautaull_TH8 |
Cross section times branching ratio for the process \(pp\to A\to HZ\to \tau\tau \ell \ell\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{pp\to A}\cdot BR^{\text{THDM}}(A\to HZ\to \tau\tau \ell \ell)\)
Definition at line 3248 of file THDMcache.h.
| double THDMcache::pp_A_Zga_llga_TH8 |
Cross section times branching ratio for the process \(pp\to A\to Z\gamma \to \ell \ell \gamma\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{pp\to A}\cdot BR^{\text{THDM}}(A\to Z\gamma \to \ell \ell \gamma)\)
Definition at line 3230 of file THDMcache.h.
| double THDMcache::pp_A_Zga_TH13 |
Cross section times branching ratio for the process \(pp\to A\to Z\gamma\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{pp\to A}\cdot BR^{\text{THDM}}(A\to Z\gamma)\)
Definition at line 3258 of file THDMcache.h.
| double THDMcache::pp_H_AZ_bbll_TH8 |
Cross section times branching ratio for the process \(pp\to H\to AZ\to b\bar b \ell \ell\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{pp\to H}\cdot BR^{\text{THDM}}(H\to AZ\to b\bar b \ell \ell)\)
Definition at line 2976 of file THDMcache.h.
| double THDMcache::pp_H_AZ_tautaull_TH8 |
Cross section times branching ratio for the process \(pp\to H\to AZ\to \tau\tau \ell \ell\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{pp\to H}\cdot BR^{\text{THDM}}(H\to AZ\to \tau\tau \ell \ell)\)
Definition at line 2978 of file THDMcache.h.
| double THDMcache::pp_H_bb_TH13 |
Cross section times branching ratio for the process \(pp\to H\to b\bar b\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{pp\to H}\cdot BR^{\text{THDM}}(H\to b\bar b)\)
Definition at line 3034 of file THDMcache.h.
| double THDMcache::pp_H_gaga_TH13 |
Cross section times branching ratio for the process \(pp\to H\to \gamma\gamma\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{pp\to H}\cdot BR^{\text{THDM}}(H\to \gamma\gamma)\)
Definition at line 2984 of file THDMcache.h.
| double THDMcache::pp_H_gaga_TH8 |
Cross section times branching ratio for the process \(pp\to H\to \gamma\gamma\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{pp\to H}\cdot BR^{\text{THDM}}(H\to \gamma\gamma)\)
Definition at line 2946 of file THDMcache.h.
| double THDMcache::pp_H_hh_bbbb_TH13 |
Cross section times branching ratio for the process \(pp\to H\to hh\to b\bar b b\bar b\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{pp\to H}\cdot BR^{\text{THDM}}(H\to hh\to b\bar b b\bar b)\)
Definition at line 3018 of file THDMcache.h.
| double THDMcache::pp_H_hh_bbbb_TH8 |
Cross section times branching ratio for the process \(pp\to H\to hh\to b\bar b b\bar b\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{pp\to H}\cdot BR^{\text{THDM}}(H\to hh\to b\bar b b\bar b)\)
Definition at line 2968 of file THDMcache.h.
| double THDMcache::pp_H_hh_bblnulnu_TH13 |
Cross section times branching ratio for the process \(pp\to H\to hh\to b\bar b WW\to b\bar b \ell \nu \ell \nu\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{pp\to H}\cdot BR^{\text{THDM}}(H\to hh\to b\bar b WW\to b\bar b \ell \nu \ell \nu)\)
Definition at line 3026 of file THDMcache.h.
| double THDMcache::pp_H_hh_bbtautau_TH13 |
Cross section times branching ratio for the process \(pp\to H\to hh\to b\bar b \tau\tau\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{pp\to H}\cdot BR^{\text{THDM}}(H\to hh\to b\bar b \tau\tau)\)
Definition at line 3024 of file THDMcache.h.
| double THDMcache::pp_H_hh_bbVV_TH13 |
Cross section times branching ratio for the process \(pp\to H\to hh\to b\bar b VV(\ell\ell \nu\nu)\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{pp\to H}\cdot BR^{\text{THDM}}[H\to hh\to b\bar b VV(\ell\ell \nu\nu)]\)
Definition at line 3028 of file THDMcache.h.
| double THDMcache::pp_H_hh_gagabb_TH13 |
Cross section times branching ratio for the process \(pp\to H\to hh\to \gamma\gamma b\bar b\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{pp\to H}\cdot BR^{\text{THDM}}(H\to hh\to \gamma\gamma b\bar b)\)
Definition at line 3022 of file THDMcache.h.
| double THDMcache::pp_H_hh_gagabb_TH8 |
Cross section times branching ratio for the process \(pp\to H\to hh\to \gamma\gamma b\bar b\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{pp\to H}\cdot BR^{\text{THDM}}(H\to hh\to \gamma\gamma b\bar b)\)
Definition at line 2970 of file THDMcache.h.
| double THDMcache::pp_H_hh_TH13 |
Cross section times branching ratio for the process \(pp\to H\to hh\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{pp\to H}\cdot BR^{\text{THDM}}(H\to hh)\)
Definition at line 3016 of file THDMcache.h.
| double THDMcache::pp_H_hh_TH8 |
Cross section times branching ratio for the process \(pp\to H\to hh\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{pp\to H}\cdot BR^{\text{THDM}}(H\to hh)\)
Definition at line 2964 of file THDMcache.h.
| double THDMcache::pp_H_VV_TH13 |
Cross section times branching ratio for the process \(pp\to H\to (WW+ZZ)\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{pp\to H}\cdot [BR^{\text{THDM}}(H\to WW)+BR^{\text{THDM}}(H\to ZZ)]\)
Definition at line 3012 of file THDMcache.h.
| double THDMcache::pp_H_Zga_llga_TH8 |
Cross section times branching ratio for the process \(pp\to H\to Z\gamma \to \ell \ell \gamma\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{pp\to H}\cdot BR^{\text{THDM}}(H\to Z\gamma \to \ell \ell \gamma)\)
Definition at line 2950 of file THDMcache.h.
| double THDMcache::pp_H_Zga_TH13 |
Cross section times branching ratio for the process \(pp\to H\to Z\gamma\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{pp\to H}\cdot BR^{\text{THDM}}(H\to Z\gamma)\)
Definition at line 2988 of file THDMcache.h.
| double THDMcache::pp_H_ZZ_llll_TH13 |
Cross section times branching ratio for the process \(pp\to H\to ZZ\to 4\ell\) at the LHC with 13 TeV. This is
Definition at line 3002 of file THDMcache.h.
| double THDMcache::pp_H_ZZ_TH13 |
Cross section times branching ratio for the process \(pp\to H\to ZZ\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{pp\to H}\cdot BR^{\text{THDM}}(H\to ZZ)\)
Definition at line 2992 of file THDMcache.h.
| double THDMcache::pp_Hp_taunu_TH8 |
Cross section for the process \(pp\to H^+\to \tau^+ \nu\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{pp\to H^+\to \tau^+ \nu}\)
Definition at line 3356 of file THDMcache.h.
| double THDMcache::pp_Hp_tb_TH13 |
Cross section times branching ratio for the process \(pp\to H^+\to t\bar b\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{pp\to H^+}\cdot BR^{\text{THDM}}(H^+\to t\bar b)\)
Definition at line 3364 of file THDMcache.h.
| double THDMcache::pp_Hp_tb_TH8 |
Cross section times branching ratio for the process \(pp\to H^+\to t\bar b\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{pp\to H^+}\cdot BR^{\text{THDM}}(H^+\to t\bar b)\)
Definition at line 3360 of file THDMcache.h.
| double THDMcache::pp_Hpm_taunu_TH13 |
Cross section times branching ratio for the process \(pp\to H^\pm\to \tau^\pm \nu\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{pp\to H^\pm}\cdot BR^{\text{THDM}}(H^\pm\to \tau^\pm \nu)\)
Definition at line 3362 of file THDMcache.h.
| double THDMcache::pp_Hpm_taunu_TH8 |
Cross section times branching ratio for the process \(pp\to H^\pm\to \tau^\pm \nu\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{pp\to H^\pm}\cdot BR^{\text{THDM}}(H^\pm\to \tau^\pm \nu)\)
Definition at line 3354 of file THDMcache.h.
| double THDMcache::pp_Hpm_tb_TH8 |
Cross section times branching ratio for the process \(pp\to H^\pm\to t b\) at the LHC with 8 TeV. This is \(2 \sigma^{\text{THDM}}_{pp\to H^+}\cdot BR^{\text{THDM}}(H^+\to t\bar b)\)
Definition at line 3358 of file THDMcache.h.
| double THDMcache::pph13 |
Ratio of THDM and SM cross sections for the production of h at 13 TeV. This is \(\sigma^{\text THDM}_{\text ggF+VBF+Vh+tth}/\sigma^{\text SM}_{\text ggF+VBF+Vh+tth}\)
Definition at line 2898 of file THDMcache.h.
|
private |
Definition at line 3417 of file THDMcache.h.
| double THDMcache::Q_cutoff |
Definition at line 3391 of file THDMcache.h.
|
private |
Definition at line 3427 of file THDMcache.h.
| double THDMcache::R_bbF_A_bb_CMS8 |
Definition at line 3315 of file THDMcache.h.
| double THDMcache::R_bbF_A_hZ_bbZ_ATLAS13 |
Definition at line 3346 of file THDMcache.h.
| double THDMcache::R_bbF_A_tautau_ATLAS13 |
Definition at line 3324 of file THDMcache.h.
| double THDMcache::R_bbF_A_tautau_ATLAS8 |
Definition at line 3293 of file THDMcache.h.
| double THDMcache::R_bbF_A_tautau_CMS13 |
Definition at line 3328 of file THDMcache.h.
| double THDMcache::R_bbF_A_tautau_CMS8 |
Definition at line 3295 of file THDMcache.h.
| double THDMcache::R_bbF_A_tt_ATLAS13 |
Definition at line 3320 of file THDMcache.h.
| double THDMcache::R_bbF_H_bb_CMS8 |
Definition at line 3109 of file THDMcache.h.
| double THDMcache::R_bbF_H_tautau_ATLAS13 |
Definition at line 3122 of file THDMcache.h.
| double THDMcache::R_bbF_H_tautau_ATLAS8 |
Definition at line 3065 of file THDMcache.h.
| double THDMcache::R_bbF_H_tautau_CMS13 |
Definition at line 3126 of file THDMcache.h.
| double THDMcache::R_bbF_H_tautau_CMS8 |
Definition at line 3069 of file THDMcache.h.
| double THDMcache::R_bbF_H_tt_ATLAS13 |
Definition at line 3118 of file THDMcache.h.
| double THDMcache::R_ggF_A_gaga_CMS13 |
Definition at line 3332 of file THDMcache.h.
| double THDMcache::R_ggF_A_gaga_CMS8 |
Definition at line 3299 of file THDMcache.h.
| double THDMcache::R_ggF_A_hZ_bbll_CMS8 |
Definition at line 3305 of file THDMcache.h.
| double THDMcache::R_ggF_A_hZ_bbZ_ATLAS13 |
Definition at line 3344 of file THDMcache.h.
| double THDMcache::R_ggF_A_hZ_bbZ_ATLAS8 |
Definition at line 3307 of file THDMcache.h.
| double THDMcache::R_ggF_A_hZ_tautaull_CMS8 |
Definition at line 3309 of file THDMcache.h.
| double THDMcache::R_ggF_A_hZ_tautauZ_ATLAS8 |
Definition at line 3311 of file THDMcache.h.
| double THDMcache::R_ggF_A_tautau_ATLAS13 |
Definition at line 3322 of file THDMcache.h.
| double THDMcache::R_ggF_A_tautau_ATLAS8 |
Definition at line 3289 of file THDMcache.h.
| double THDMcache::R_ggF_A_tautau_CMS13 |
Definition at line 3326 of file THDMcache.h.
| double THDMcache::R_ggF_A_tautau_CMS8 |
Definition at line 3291 of file THDMcache.h.
| double THDMcache::R_ggF_A_tt_ATLAS8 |
Definition at line 3313 of file THDMcache.h.
| double THDMcache::R_ggF_A_Zga_CMS13 |
Definition at line 3342 of file THDMcache.h.
| double THDMcache::R_ggF_A_Zga_llga_ATLAS13 |
Definition at line 3334 of file THDMcache.h.
| double THDMcache::R_ggF_H_gaga_CMS13 |
Definition at line 3130 of file THDMcache.h.
| double THDMcache::R_ggF_H_gaga_CMS8 |
Definition at line 3077 of file THDMcache.h.
| double THDMcache::R_ggF_H_hh_ATLAS8 |
Definition at line 3097 of file THDMcache.h.
| double THDMcache::R_ggF_H_hh_bbbb_CMS13 |
Definition at line 3194 of file THDMcache.h.
| double THDMcache::R_ggF_H_hh_bbtautau_CMS8 |
Definition at line 3101 of file THDMcache.h.
| double THDMcache::R_ggF_H_hh_gagaWW_ATLAS13 |
Definition at line 3196 of file THDMcache.h.
| double THDMcache::R_ggF_H_tautau_ATLAS13 |
Definition at line 3120 of file THDMcache.h.
| double THDMcache::R_ggF_H_tautau_ATLAS8 |
Definition at line 3057 of file THDMcache.h.
| double THDMcache::R_ggF_H_tautau_CMS13 |
Definition at line 3124 of file THDMcache.h.
| double THDMcache::R_ggF_H_tautau_CMS8 |
Definition at line 3061 of file THDMcache.h.
| double THDMcache::R_ggF_H_tt_ATLAS8 |
Definition at line 3107 of file THDMcache.h.
| double THDMcache::R_ggF_H_WW_ATLAS8 |
Definition at line 3089 of file THDMcache.h.
| double THDMcache::R_ggF_H_WW_enumunu_ATLAS13 |
Definition at line 3178 of file THDMcache.h.
| double THDMcache::R_ggF_H_WW_lnuqq_ATLAS13 |
Definition at line 3174 of file THDMcache.h.
| double THDMcache::R_ggF_H_Zga_CMS13 |
Definition at line 3140 of file THDMcache.h.
| double THDMcache::R_ggF_H_Zga_llga_ATLAS13 |
Definition at line 3134 of file THDMcache.h.
| double THDMcache::R_ggF_H_ZZ_ATLAS8 |
Definition at line 3093 of file THDMcache.h.
| double THDMcache::R_ggF_H_ZZ_llll_ATLAS13 |
Definition at line 3154 of file THDMcache.h.
| double THDMcache::R_ggF_H_ZZ_llllnunu_ATLAS13 |
Definition at line 3142 of file THDMcache.h.
| double THDMcache::R_ggF_H_ZZ_llnunu_ATLAS13 |
Definition at line 3146 of file THDMcache.h.
| double THDMcache::R_ggF_H_ZZ_llnunu_CMS13 |
Definition at line 3150 of file THDMcache.h.
| double THDMcache::R_ggF_H_ZZ_llqq_ATLAS13 |
Definition at line 3166 of file THDMcache.h.
| double THDMcache::R_ggF_H_ZZ_nunuqq_ATLAS13 |
Definition at line 3170 of file THDMcache.h.
| double THDMcache::R_ggF_H_ZZ_qqllnunu_ATLAS13 |
Definition at line 3162 of file THDMcache.h.
| double THDMcache::R_ggF_VBF_H_WW_lnulnu_CMS13 |
Definition at line 3182 of file THDMcache.h.
| double THDMcache::R_mu_pp_H_VV_CMS8 |
Definition at line 3087 of file THDMcache.h.
| double THDMcache::R_pp_A_bb_CMS13 |
Definition at line 3348 of file THDMcache.h.
| double THDMcache::R_pp_A_gaga_ATLAS13 |
Definition at line 3330 of file THDMcache.h.
| double THDMcache::R_pp_A_gaga_ATLAS8 |
Definition at line 3297 of file THDMcache.h.
| double THDMcache::R_pp_A_HZ_bbll_CMS8 |
Definition at line 3350 of file THDMcache.h.
| double THDMcache::R_pp_A_HZ_tautaull_CMS8 |
Definition at line 3352 of file THDMcache.h.
| double THDMcache::R_pp_A_Zga_llga_ATLAS13 |
Definition at line 3336 of file THDMcache.h.
| double THDMcache::R_pp_A_Zga_llga_ATLAS8 |
Definition at line 3303 of file THDMcache.h.
| double THDMcache::R_pp_A_Zga_llga_CMS13 |
Definition at line 3338 of file THDMcache.h.
| double THDMcache::R_pp_A_Zga_llga_CMS8 |
Definition at line 3301 of file THDMcache.h.
| double THDMcache::R_pp_A_Zga_qqga_CMS13 |
Definition at line 3340 of file THDMcache.h.
| double THDMcache::R_pp_H_AZ_bbll_CMS8 |
Definition at line 3111 of file THDMcache.h.
| double THDMcache::R_pp_H_AZ_tautaull_CMS8 |
Definition at line 3113 of file THDMcache.h.
| double THDMcache::R_pp_H_bb_CMS13 |
Definition at line 3206 of file THDMcache.h.
| double THDMcache::R_pp_H_gaga_ATLAS13 |
Definition at line 3128 of file THDMcache.h.
| double THDMcache::R_pp_H_gaga_ATLAS8 |
Definition at line 3073 of file THDMcache.h.
| double THDMcache::R_pp_H_hh_bbbb_ATLAS13 |
Definition at line 3190 of file THDMcache.h.
| double THDMcache::R_pp_H_hh_bbbb_CMS13 |
Definition at line 3192 of file THDMcache.h.
| double THDMcache::R_pp_H_hh_bbbb_CMS8 |
Definition at line 3103 of file THDMcache.h.
| double THDMcache::R_pp_H_hh_bbgaga_ATLAS13 |
Definition at line 3186 of file THDMcache.h.
| double THDMcache::R_pp_H_hh_bbgaga_CMS13 |
Definition at line 3188 of file THDMcache.h.
| double THDMcache::R_pp_H_hh_bblnulnu_CMS13 |
Definition at line 3202 of file THDMcache.h.
| double THDMcache::R_pp_H_hh_bbtautau1_CMS13 |
Definition at line 3200 of file THDMcache.h.
| double THDMcache::R_pp_H_hh_bbtautau_CMS13 |
Definition at line 3198 of file THDMcache.h.
| double THDMcache::R_pp_H_hh_bbVV_CMS13 |
Definition at line 3204 of file THDMcache.h.
| double THDMcache::R_pp_H_hh_CMS8 |
Definition at line 3099 of file THDMcache.h.
| double THDMcache::R_pp_H_hh_gagabb_CMS8 |
Definition at line 3105 of file THDMcache.h.
| double THDMcache::R_pp_H_VV_qqqq_ATLAS13 |
Definition at line 3184 of file THDMcache.h.
| double THDMcache::R_pp_H_Zga_ATLAS13 |
Definition at line 3132 of file THDMcache.h.
| double THDMcache::R_pp_H_Zga_llga_ATLAS8 |
Definition at line 3085 of file THDMcache.h.
| double THDMcache::R_pp_H_Zga_llga_CMS13 |
Definition at line 3136 of file THDMcache.h.
| double THDMcache::R_pp_H_Zga_llga_CMS8 |
Definition at line 3083 of file THDMcache.h.
| double THDMcache::R_pp_H_Zga_qqga_CMS13 |
Definition at line 3138 of file THDMcache.h.
| double THDMcache::R_pp_H_ZZ_llll_CMS13 |
Definition at line 3158 of file THDMcache.h.
| double THDMcache::R_pp_H_ZZ_llnunu_CMS13 |
Definition at line 3148 of file THDMcache.h.
| double THDMcache::R_pp_H_ZZ_llqq_CMS13 |
Definition at line 3172 of file THDMcache.h.
| double THDMcache::R_pp_Hp_taunu_CMS8 |
Definition at line 3369 of file THDMcache.h.
| double THDMcache::R_pp_Hp_tb_ATLAS13 |
Definition at line 3383 of file THDMcache.h.
| double THDMcache::R_pp_Hp_tb_ATLAS13_1 |
Definition at line 3379 of file THDMcache.h.
| double THDMcache::R_pp_Hp_tb_ATLAS13_2 |
Definition at line 3381 of file THDMcache.h.
| double THDMcache::R_pp_Hp_tb_CMS8 |
Definition at line 3373 of file THDMcache.h.
| double THDMcache::R_pp_Hpm_taunu_ATLAS13 |
Definition at line 3375 of file THDMcache.h.
| double THDMcache::R_pp_Hpm_taunu_ATLAS8 |
Definition at line 3367 of file THDMcache.h.
| double THDMcache::R_pp_Hpm_taunu_CMS13 |
Definition at line 3377 of file THDMcache.h.
| double THDMcache::R_pp_Hpm_tb_ATLAS8 |
Definition at line 3371 of file THDMcache.h.
| double THDMcache::R_ttF_A_tt_ATLAS13 |
Definition at line 3318 of file THDMcache.h.
| double THDMcache::R_ttF_H_tt_ATLAS13 |
Definition at line 3116 of file THDMcache.h.
| double THDMcache::R_VBF_H_WW_ATLAS8 |
Definition at line 3091 of file THDMcache.h.
| double THDMcache::R_VBF_H_WW_enumunu_ATLAS13 |
Definition at line 3180 of file THDMcache.h.
| double THDMcache::R_VBF_H_WW_lnuqq_ATLAS13 |
Definition at line 3176 of file THDMcache.h.
| double THDMcache::R_VBF_H_ZZ_ATLAS8 |
Definition at line 3095 of file THDMcache.h.
| double THDMcache::R_VBF_H_ZZ_llll_ATLAS13 |
Definition at line 3156 of file THDMcache.h.
| double THDMcache::R_VBF_H_ZZ_llllnunu_ATLAS13 |
Definition at line 3144 of file THDMcache.h.
| double THDMcache::R_VBF_H_ZZ_llnunu_CMS13 |
Definition at line 3152 of file THDMcache.h.
| double THDMcache::R_VBF_H_ZZ_llqq_ATLAS13 |
Definition at line 3168 of file THDMcache.h.
| double THDMcache::R_VBF_H_ZZ_qqllnunu_ATLAS13 |
Definition at line 3164 of file THDMcache.h.
| double THDMcache::R_VBF_VH_H_ZZ_llll_CMS13 |
Definition at line 3160 of file THDMcache.h.
| double THDMcache::rA_gg |
Squared relative coupling of \(A\) to two gluons. This is \(r^{(A)}_{gg}\). Note that this depends on the type of \(Z_2\) symmetry.
Definition at line 3276 of file THDMcache.h.
| double THDMcache::rh_gaga |
Squared relative coupling of \(h\) to two photons. This is \(r^{(h)}_{\gamma \gamma}\). Note that this depends on the type of \(Z_2\) symmetry.
Definition at line 2888 of file THDMcache.h.
| double THDMcache::rh_gg |
Squared relative coupling of \(h\) to two gluons. This is \(r^{(h)}_{gg}\). Note that this depends on the type of \(Z_2\) symmetry.
Definition at line 2892 of file THDMcache.h.
| double THDMcache::rh_ll |
Squared relative coupling of \(h\) to two charged leptons. This is \(r^{(h)}_{\ell \ell}\). Note that this depends on the type of \(Z_2\) symmetry.
Definition at line 2886 of file THDMcache.h.
| double THDMcache::rh_QdQd |
quared relative coupling of \(h\) to two down type quarks. This is \(r^{(h)}_{Q_dQ_d}\). Note that this depends on the type of \(Z_2\) symmetry.
Definition at line 2882 of file THDMcache.h.
| double THDMcache::rh_QuQu |
Squared relative coupling of \(h\) to two up type quarks. This is \(r^{(h)}_{Q_uQ_u}\)
Definition at line 2906 of file THDMcache.h.
| double THDMcache::rh_VV |
Squared relative coupling of \(h\) to two massive vector bosons. This is \(r^{(h)}_{WW}=r^{(h)}_{ZZ}\)
Definition at line 2884 of file THDMcache.h.
| double THDMcache::rh_Zga |
Squared relative coupling of \(h\) to a \(Z\) boson and a photon. This is \(r^{(h)}_{Z\gamma}\). Note that this depends on the type of \(Z_2\) symmetry.
Definition at line 2890 of file THDMcache.h.
| double THDMcache::rHH_gg |
Squared relative coupling of \(H\) to two gluons. This is \(r^{(H)}_{gg}\). Note that this depends on the type of \(Z_2\) symmetry.
Definition at line 3041 of file THDMcache.h.
| double THDMcache::rHH_VV |
Squared relative coupling of \(H\) to two massive vector bosons. This is \(r^{(H)}_{VV}\)
Definition at line 3043 of file THDMcache.h.
| double THDMcache::Rpeps |
Definition at line 3412 of file THDMcache.h.
| double THDMcache::SigmabbF_A13 |
Definition at line 3212 of file THDMcache.h.
| double THDMcache::SigmabbF_A8 |
Definition at line 3209 of file THDMcache.h.
| double THDMcache::SigmabbF_H13 |
Definition at line 2930 of file THDMcache.h.
| double THDMcache::SigmabbF_H8 |
Definition at line 2925 of file THDMcache.h.
| double THDMcache::SigmaggF_A13 |
Definition at line 3211 of file THDMcache.h.
| double THDMcache::SigmaggF_A8 |
Definition at line 3208 of file THDMcache.h.
| double THDMcache::SigmaggF_H13 |
Definition at line 2928 of file THDMcache.h.
| double THDMcache::SigmaggF_H8 |
Definition at line 2924 of file THDMcache.h.
| double THDMcache::SigmaSumA13 |
Definition at line 3214 of file THDMcache.h.
| double THDMcache::SigmaSumA8 |
Definition at line 3210 of file THDMcache.h.
| double THDMcache::SigmaSumH13 |
Definition at line 2927 of file THDMcache.h.
| double THDMcache::SigmaSumH8 |
Definition at line 2922 of file THDMcache.h.
| double THDMcache::SigmaTotSM_H8 |
Definition at line 2923 of file THDMcache.h.
| double THDMcache::SigmattF_A13 |
Definition at line 3213 of file THDMcache.h.
| double THDMcache::SigmattF_H13 |
Definition at line 2929 of file THDMcache.h.
| double THDMcache::SigmaVBF_H13 |
Definition at line 2931 of file THDMcache.h.
| double THDMcache::SigmaVBF_H8 |
Definition at line 2926 of file THDMcache.h.
| double THDMcache::SigmaVH_H13 |
Definition at line 2932 of file THDMcache.h.
| double THDMcache::sumModBRs |
Sum of the modified branching ratios. This is \(\sum _i r^{(h)}_{i} BR^{\text SM}(h\to i)\)
Definition at line 2902 of file THDMcache.h.
|
private |
Definition at line 3430 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp1 |
Definition at line 170 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp10 |
data templates
Definition at line 170 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp10e |
data templates
Definition at line 174 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp11 |
Definition at line 171 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp11e |
Definition at line 175 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp12 |
Definition at line 171 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp12e |
Definition at line 175 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp13 |
Definition at line 171 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp13e |
Definition at line 175 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp14 |
Definition at line 171 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp14e |
Definition at line 175 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp15 |
Definition at line 171 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp15e |
Definition at line 175 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp16 |
Definition at line 171 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp16e |
Definition at line 175 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp17 |
Definition at line 171 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp17e |
Definition at line 175 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp18 |
Definition at line 171 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp18e |
Definition at line 175 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp19 |
Definition at line 171 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp19e |
Definition at line 175 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp1e |
Definition at line 174 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp2 |
Definition at line 170 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp20 |
data templates
Definition at line 171 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp20e |
data templates
Definition at line 175 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp21 |
Definition at line 172 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp21e |
Definition at line 176 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp22 |
Definition at line 172 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp22e |
Definition at line 176 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp23 |
Definition at line 172 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp23e |
Definition at line 176 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp24 |
Definition at line 172 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp24e |
Definition at line 176 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp25 |
Definition at line 172 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp25e |
Definition at line 176 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp26 |
Definition at line 172 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp26e |
Definition at line 176 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp27 |
Definition at line 172 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp27e |
Definition at line 176 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp28 |
Definition at line 172 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp28e |
Definition at line 176 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp29 |
Definition at line 172 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp29e |
Definition at line 176 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp2e |
Definition at line 174 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp3 |
Definition at line 170 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp30 |
data templates
Definition at line 172 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp30e |
data templates
Definition at line 176 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp31 |
Definition at line 173 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp31e |
Definition at line 177 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp32 |
Definition at line 173 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp32e |
Definition at line 177 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp33 |
Definition at line 173 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp33e |
Definition at line 177 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp34 |
Definition at line 173 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp34e |
Definition at line 177 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp35 |
Definition at line 173 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp35e |
Definition at line 177 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp36 |
Definition at line 173 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp36e |
Definition at line 177 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp37 |
Definition at line 173 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp37e |
Definition at line 177 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp38 |
Definition at line 173 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp38e |
Definition at line 177 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp39 |
Definition at line 173 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp39e |
Definition at line 177 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp3e |
Definition at line 174 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp4 |
Definition at line 170 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp40 |
data templates
Definition at line 173 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp40e |
data templates
Definition at line 177 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp4e |
Definition at line 174 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp5 |
Definition at line 170 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp5e |
Definition at line 174 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp6 |
Definition at line 170 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp6e |
Definition at line 174 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp7 |
Definition at line 170 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp7e |
Definition at line 174 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp8 |
Definition at line 170 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp8e |
Definition at line 174 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp9 |
Definition at line 170 of file THDMcache.h.
| gslpp::matrix<double> THDMcache::temp9e |
Definition at line 174 of file THDMcache.h.
| double THDMcache::THDM_BR_h_bb |
\(h\) branching ratio to two \(b\) quarks in the THDM. This is \(BR^{\text{THDM}}(h\to b \bar b)\)
Definition at line 2908 of file THDMcache.h.
| double THDMcache::THDM_BR_h_cc |
\(h\) branching ratio to two \(c\) quarks in the THDM. This is \(BR^{\text{THDM}}(h\to c\bar c)\)
Definition at line 2920 of file THDMcache.h.
| double THDMcache::THDM_BR_h_gaga |
branching ratio to two photons in the THDM. This is \(BR^{\text{THDM}}(h\to \gamma \gamma)\)
Definition at line 2910 of file THDMcache.h.
| double THDMcache::THDM_BR_h_gg |
\(h\) branching ratio to two gluons in the THDM. This is \(BR^{\text{THDM}}(h\to gg)\)
Definition at line 2918 of file THDMcache.h.
| double THDMcache::THDM_BR_h_tautau |
\(h\) branching ratio to two \(\tau\) leptons in the THDM. This is \(BR^{\text{THDM}}(h\to \tau\tau )\)
Definition at line 2912 of file THDMcache.h.
| double THDMcache::THDM_BR_h_WW |
\(h\) branching ratio to two \(W\) bosons in the THDM. This is \(BR^{\text{THDM}}(h\to WW)\)
Definition at line 2914 of file THDMcache.h.
| double THDMcache::THDM_BR_h_ZZ |
\(h\) branching ratio to two \(Z\) bosons in the THDM. This is \(BR^{\text{THDM}}(h\to ZZ)\)
Definition at line 2916 of file THDMcache.h.
| double THDMcache::THoEX_bbF_A_bb_CMS8 |
Definition at line 3314 of file THDMcache.h.
| double THDMcache::THoEX_bbF_A_hZ_bbZ_ATLAS13 |
Definition at line 3345 of file THDMcache.h.
| double THDMcache::THoEX_bbF_A_tautau_ATLAS13 |
Definition at line 3323 of file THDMcache.h.
| double THDMcache::THoEX_bbF_A_tautau_ATLAS8 |
Definition at line 3292 of file THDMcache.h.
| double THDMcache::THoEX_bbF_A_tautau_CMS13 |
Definition at line 3327 of file THDMcache.h.
| double THDMcache::THoEX_bbF_A_tautau_CMS8 |
Definition at line 3294 of file THDMcache.h.
| double THDMcache::THoEX_bbF_A_tt_ATLAS13 |
Definition at line 3319 of file THDMcache.h.
| double THDMcache::THoEX_bbF_H_bb_CMS8 |
Definition at line 3108 of file THDMcache.h.
| double THDMcache::THoEX_bbF_H_tautau_ATLAS13 |
Definition at line 3121 of file THDMcache.h.
| double THDMcache::THoEX_bbF_H_tautau_ATLAS8 |
Definition at line 3063 of file THDMcache.h.
| double THDMcache::THoEX_bbF_H_tautau_CMS13 |
Definition at line 3125 of file THDMcache.h.
| double THDMcache::THoEX_bbF_H_tautau_CMS8 |
Definition at line 3067 of file THDMcache.h.
| double THDMcache::THoEX_bbF_H_tt_ATLAS13 |
Definition at line 3117 of file THDMcache.h.
| double THDMcache::THoEX_ggF_A_gaga_CMS13 |
Definition at line 3331 of file THDMcache.h.
| double THDMcache::THoEX_ggF_A_gaga_CMS8 |
Definition at line 3298 of file THDMcache.h.
| double THDMcache::THoEX_ggF_A_hZ_bbll_CMS8 |
Definition at line 3304 of file THDMcache.h.
| double THDMcache::THoEX_ggF_A_hZ_bbZ_ATLAS13 |
Definition at line 3343 of file THDMcache.h.
| double THDMcache::THoEX_ggF_A_hZ_bbZ_ATLAS8 |
Definition at line 3306 of file THDMcache.h.
| double THDMcache::THoEX_ggF_A_hZ_tautaull_CMS8 |
Definition at line 3308 of file THDMcache.h.
| double THDMcache::THoEX_ggF_A_hZ_tautauZ_ATLAS8 |
Definition at line 3310 of file THDMcache.h.
| double THDMcache::THoEX_ggF_A_tautau_ATLAS13 |
Definition at line 3321 of file THDMcache.h.
| double THDMcache::THoEX_ggF_A_tautau_ATLAS8 |
Definition at line 3288 of file THDMcache.h.
| double THDMcache::THoEX_ggF_A_tautau_CMS13 |
Definition at line 3325 of file THDMcache.h.
| double THDMcache::THoEX_ggF_A_tautau_CMS8 |
Definition at line 3290 of file THDMcache.h.
| double THDMcache::THoEX_ggF_A_tt_ATLAS8 |
Definition at line 3312 of file THDMcache.h.
| double THDMcache::THoEX_ggF_A_Zga_CMS13 |
Definition at line 3341 of file THDMcache.h.
| double THDMcache::THoEX_ggF_A_Zga_llga_ATLAS13 |
Definition at line 3333 of file THDMcache.h.
| double THDMcache::THoEX_ggF_H_gaga_CMS13 |
Definition at line 3129 of file THDMcache.h.
| double THDMcache::THoEX_ggF_H_gaga_CMS8 |
Definition at line 3075 of file THDMcache.h.
| double THDMcache::THoEX_ggF_H_hh_ATLAS8 |
Definition at line 3096 of file THDMcache.h.
| double THDMcache::THoEX_ggF_H_hh_bbbb_CMS13 |
Definition at line 3193 of file THDMcache.h.
| double THDMcache::THoEX_ggF_H_hh_bbtautau_CMS8 |
Definition at line 3100 of file THDMcache.h.
| double THDMcache::THoEX_ggF_H_hh_gagaWW_ATLAS13 |
Definition at line 3195 of file THDMcache.h.
| double THDMcache::THoEX_ggF_H_tautau_ATLAS13 |
Definition at line 3119 of file THDMcache.h.
| double THDMcache::THoEX_ggF_H_tautau_ATLAS8 |
Ratio between the theoretical prediction and the experimental upper limit for the process \(gg\to H\to \tau\tau\) at 8 TeV. This is \(\frac{\sigma^{\text{THDM}}_{\text{theo}}(gg\to H)BR^{\text{THDM}}_{\text{theo}}(H\to \tau\tau)}{\sigma^{\text{THDM}}_{\text{exp}}(gg\to H)BR^{\text{THDM}}_{\text{exp}}(H\to \tau\tau)}\).
Definition at line 3055 of file THDMcache.h.
| double THDMcache::THoEX_ggF_H_tautau_CMS13 |
Definition at line 3123 of file THDMcache.h.
| double THDMcache::THoEX_ggF_H_tautau_CMS8 |
Definition at line 3059 of file THDMcache.h.
| double THDMcache::THoEX_ggF_H_tt_ATLAS8 |
Definition at line 3106 of file THDMcache.h.
| double THDMcache::THoEX_ggF_H_WW_ATLAS8 |
Definition at line 3088 of file THDMcache.h.
| double THDMcache::THoEX_ggF_H_WW_enumunu_ATLAS13 |
Definition at line 3177 of file THDMcache.h.
| double THDMcache::THoEX_ggF_H_WW_lnuqq_ATLAS13 |
Definition at line 3173 of file THDMcache.h.
| double THDMcache::THoEX_ggF_H_Zga_CMS13 |
Definition at line 3139 of file THDMcache.h.
| double THDMcache::THoEX_ggF_H_Zga_llga_ATLAS13 |
Definition at line 3133 of file THDMcache.h.
| double THDMcache::THoEX_ggF_H_ZZ_ATLAS8 |
Definition at line 3092 of file THDMcache.h.
| double THDMcache::THoEX_ggF_H_ZZ_llll_ATLAS13 |
Definition at line 3153 of file THDMcache.h.
| double THDMcache::THoEX_ggF_H_ZZ_llllnunu_ATLAS13 |
Definition at line 3141 of file THDMcache.h.
| double THDMcache::THoEX_ggF_H_ZZ_llnunu_ATLAS13 |
Definition at line 3145 of file THDMcache.h.
| double THDMcache::THoEX_ggF_H_ZZ_llnunu_CMS13 |
Definition at line 3149 of file THDMcache.h.
| double THDMcache::THoEX_ggF_H_ZZ_llqq_ATLAS13 |
Definition at line 3165 of file THDMcache.h.
| double THDMcache::THoEX_ggF_H_ZZ_nunuqq_ATLAS13 |
Definition at line 3169 of file THDMcache.h.
| double THDMcache::THoEX_ggF_H_ZZ_qqllnunu_ATLAS13 |
Definition at line 3161 of file THDMcache.h.
| double THDMcache::THoEX_ggF_VBF_H_WW_lnulnu_CMS13 |
Definition at line 3181 of file THDMcache.h.
| double THDMcache::THoEX_mu_pp_H_VV_CMS8 |
Definition at line 3086 of file THDMcache.h.
| double THDMcache::THoEX_pp_A_bb_CMS13 |
Definition at line 3347 of file THDMcache.h.
| double THDMcache::THoEX_pp_A_gaga_ATLAS13 |
Definition at line 3329 of file THDMcache.h.
| double THDMcache::THoEX_pp_A_gaga_ATLAS8 |
Definition at line 3296 of file THDMcache.h.
| double THDMcache::THoEX_pp_A_HZ_bbll_CMS8 |
Definition at line 3349 of file THDMcache.h.
| double THDMcache::THoEX_pp_A_HZ_tautaull_CMS8 |
Definition at line 3351 of file THDMcache.h.
| double THDMcache::THoEX_pp_A_Zga_llga_ATLAS13 |
Definition at line 3335 of file THDMcache.h.
| double THDMcache::THoEX_pp_A_Zga_llga_ATLAS8 |
Definition at line 3302 of file THDMcache.h.
| double THDMcache::THoEX_pp_A_Zga_llga_CMS13 |
Definition at line 3337 of file THDMcache.h.
| double THDMcache::THoEX_pp_A_Zga_llga_CMS8 |
Definition at line 3300 of file THDMcache.h.
| double THDMcache::THoEX_pp_A_Zga_qqga_CMS13 |
Definition at line 3339 of file THDMcache.h.
| double THDMcache::THoEX_pp_H_AZ_bbll_CMS8 |
Definition at line 3110 of file THDMcache.h.
| double THDMcache::THoEX_pp_H_AZ_tautaull_CMS8 |
Definition at line 3112 of file THDMcache.h.
| double THDMcache::THoEX_pp_H_bb_CMS13 |
Definition at line 3205 of file THDMcache.h.
| double THDMcache::THoEX_pp_H_gaga_ATLAS13 |
Definition at line 3127 of file THDMcache.h.
| double THDMcache::THoEX_pp_H_gaga_ATLAS8 |
Definition at line 3071 of file THDMcache.h.
| double THDMcache::THoEX_pp_H_hh_bbbb_ATLAS13 |
Definition at line 3189 of file THDMcache.h.
| double THDMcache::THoEX_pp_H_hh_bbbb_CMS13 |
Definition at line 3191 of file THDMcache.h.
| double THDMcache::THoEX_pp_H_hh_bbbb_CMS8 |
Definition at line 3102 of file THDMcache.h.
| double THDMcache::THoEX_pp_H_hh_bbgaga_ATLAS13 |
Definition at line 3185 of file THDMcache.h.
| double THDMcache::THoEX_pp_H_hh_bbgaga_CMS13 |
Definition at line 3187 of file THDMcache.h.
| double THDMcache::THoEX_pp_H_hh_bblnulnu_CMS13 |
Definition at line 3201 of file THDMcache.h.
| double THDMcache::THoEX_pp_H_hh_bbtautau1_CMS13 |
Definition at line 3199 of file THDMcache.h.
| double THDMcache::THoEX_pp_H_hh_bbtautau_CMS13 |
Definition at line 3197 of file THDMcache.h.
| double THDMcache::THoEX_pp_H_hh_bbVV_CMS13 |
Definition at line 3203 of file THDMcache.h.
| double THDMcache::THoEX_pp_H_hh_CMS8 |
Definition at line 3098 of file THDMcache.h.
| double THDMcache::THoEX_pp_H_hh_gagabb_CMS8 |
Definition at line 3104 of file THDMcache.h.
| double THDMcache::THoEX_pp_H_VV_qqqq_ATLAS13 |
Definition at line 3183 of file THDMcache.h.
| double THDMcache::THoEX_pp_H_Zga_ATLAS13 |
Definition at line 3131 of file THDMcache.h.
| double THDMcache::THoEX_pp_H_Zga_llga_ATLAS8 |
Definition at line 3084 of file THDMcache.h.
| double THDMcache::THoEX_pp_H_Zga_llga_CMS13 |
Definition at line 3135 of file THDMcache.h.
| double THDMcache::THoEX_pp_H_Zga_llga_CMS8 |
Definition at line 3082 of file THDMcache.h.
| double THDMcache::THoEX_pp_H_Zga_qqga_CMS13 |
Definition at line 3137 of file THDMcache.h.
| double THDMcache::THoEX_pp_H_ZZ_llll_CMS13 |
Definition at line 3157 of file THDMcache.h.
| double THDMcache::THoEX_pp_H_ZZ_llnunu_CMS13 |
Definition at line 3147 of file THDMcache.h.
| double THDMcache::THoEX_pp_H_ZZ_llqq_CMS13 |
Definition at line 3171 of file THDMcache.h.
| double THDMcache::THoEX_pp_Hp_taunu_CMS8 |
Definition at line 3368 of file THDMcache.h.
| double THDMcache::THoEX_pp_Hp_tb_ATLAS13 |
Definition at line 3382 of file THDMcache.h.
| double THDMcache::THoEX_pp_Hp_tb_ATLAS13_1 |
Definition at line 3378 of file THDMcache.h.
| double THDMcache::THoEX_pp_Hp_tb_ATLAS13_2 |
Definition at line 3380 of file THDMcache.h.
| double THDMcache::THoEX_pp_Hp_tb_CMS8 |
Definition at line 3372 of file THDMcache.h.
| double THDMcache::THoEX_pp_Hpm_taunu_ATLAS13 |
Definition at line 3374 of file THDMcache.h.
| double THDMcache::THoEX_pp_Hpm_taunu_ATLAS8 |
Definition at line 3366 of file THDMcache.h.
| double THDMcache::THoEX_pp_Hpm_taunu_CMS13 |
Definition at line 3376 of file THDMcache.h.
| double THDMcache::THoEX_pp_Hpm_tb_ATLAS8 |
Definition at line 3370 of file THDMcache.h.
| double THDMcache::THoEX_ttF_A_tt_ATLAS13 |
Definition at line 3317 of file THDMcache.h.
| double THDMcache::THoEX_ttF_H_tt_ATLAS13 |
Definition at line 3115 of file THDMcache.h.
| double THDMcache::THoEX_VBF_H_WW_ATLAS8 |
Definition at line 3090 of file THDMcache.h.
| double THDMcache::THoEX_VBF_H_WW_enumunu_ATLAS13 |
Definition at line 3179 of file THDMcache.h.
| double THDMcache::THoEX_VBF_H_WW_lnuqq_ATLAS13 |
Definition at line 3175 of file THDMcache.h.
| double THDMcache::THoEX_VBF_H_ZZ_ATLAS8 |
Definition at line 3094 of file THDMcache.h.
| double THDMcache::THoEX_VBF_H_ZZ_llll_ATLAS13 |
Definition at line 3155 of file THDMcache.h.
| double THDMcache::THoEX_VBF_H_ZZ_llllnunu_ATLAS13 |
Definition at line 3143 of file THDMcache.h.
| double THDMcache::THoEX_VBF_H_ZZ_llnunu_CMS13 |
Definition at line 3151 of file THDMcache.h.
| double THDMcache::THoEX_VBF_H_ZZ_llqq_ATLAS13 |
Definition at line 3167 of file THDMcache.h.
| double THDMcache::THoEX_VBF_H_ZZ_qqllnunu_ATLAS13 |
Definition at line 3163 of file THDMcache.h.
| double THDMcache::THoEX_VBF_VH_H_ZZ_llll_CMS13 |
Definition at line 3159 of file THDMcache.h.
| double THDMcache::ttF_A_tt_TH13 |
Cross section times branching ratio for the process \(t\bar t\to A\to t\bar t\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{t\bar t\to A}\cdot BR^{\text{THDM}}(A\to t\bar t)\)
Definition at line 3266 of file THDMcache.h.
| double THDMcache::ttF_H_tt_TH13 |
Cross section times branching ratio for the process \(t\bar t\to H\to t\bar t\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{t\bar t\to H}\cdot BR^{\text{THDM}}(H\to t\bar t)\)
Definition at line 3030 of file THDMcache.h.
|
private |
Definition at line 3460 of file THDMcache.h.
| double THDMcache::VBF_H_WW_TH13 |
Cross section times branching ratio for the process \(VV\to H\to WW\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{VV\to H}\cdot BR^{\text{THDM}}(H\to WW)\)
Definition at line 3008 of file THDMcache.h.
| double THDMcache::VBF_H_WW_TH8 |
Cross section times branching ratio for the process \(VV\to H\to WW\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{VV\to H}\cdot BR^{\text{THDM}}(H\to WW)\)
Definition at line 2960 of file THDMcache.h.
| double THDMcache::VBF_H_ZZ_llll_TH13 |
Cross section times branching ratio for the process \(VV\to H\to ZZ\to 4\ell\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{VV\to H}\cdot BR^{\text{THDM}}(H\to ZZ\to 4\ell)\)
Definition at line 3000 of file THDMcache.h.
| double THDMcache::VBF_H_ZZ_TH13 |
Cross section times branching ratio for the process \(VV\to H\to ZZ\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{VV\to H}\cdot BR^{\text{THDM}}(H\to ZZ)\)
Definition at line 2996 of file THDMcache.h.
| double THDMcache::VBF_H_ZZ_TH8 |
Cross section times branching ratio for the process \(VV\to H\to ZZ\) at the LHC with 8 TeV. This is \(\sigma^{\text{THDM}}_{VV\to H}\cdot BR^{\text{THDM}}(H\to ZZ)\)
Definition at line 2956 of file THDMcache.h.
| double THDMcache::VBF_Vh |
Ratio of THDM and SM cross sections for VBF and Vh production of h. This is \(\sigma^{\text THDM}_{\text VBF+Vh}/\sigma^{\text SM}_{\text VBF+Vh}\)
Definition at line 2900 of file THDMcache.h.
| double THDMcache::VBF_VH_H_ZZ_llll_TH13 |
Cross section times branching ratio for the process \(VV+VH\to H\to ZZ\to 4\ell\) at the LHC with 13 TeV. This is \(\sigma^{\text{THDM}}_{VV+VH\to H}\cdot BR^{\text{THDM}}(H\to ZZ\to 4\ell)\)
Definition at line 3004 of file THDMcache.h.
|
private |
Definition at line 3445 of file THDMcache.h.
| double THDMcache::WFRcomb1 |
Definition at line 3408 of file THDMcache.h.
| double THDMcache::WFRcomb2 |
Definition at line 3409 of file THDMcache.h.
| double THDMcache::WFRcomb3 |
Definition at line 3410 of file THDMcache.h.
| double THDMcache::WFRcomb4 |
Definition at line 3411 of file THDMcache.h.
|
private |
Definition at line 3459 of file THDMcache.h.
| double THDMcache::Ybottom1_at_Q |
Definition at line 3396 of file THDMcache.h.
| double THDMcache::Ybottom2_at_Q |
Definition at line 3397 of file THDMcache.h.
| double THDMcache::Ytau1_at_Q |
Definition at line 3398 of file THDMcache.h.
| double THDMcache::Ytau2_at_Q |
Definition at line 3399 of file THDMcache.h.
| double THDMcache::Ytop_at_Q |
Definition at line 3395 of file THDMcache.h.
1.8.16