HiggsBounds.h File Reference

C interface to the HiggsBounds subroutines. More...

#include <stddef.h>

Include dependency graph for HiggsBounds.h:

Go to the source code of this file.

Enumerations
enum	HiggsBounds_analyses_flag {   onlyL, onlyH, LandH, onlyP,   list }
	Select which experimental analyses to use with initialize_HiggsBounds() More...
enum	HiggsBounds_collider_id { Tevatron = 2, LHC7 = 7, LHC8 = 8, LHC13 = 13 }
	Select which collider the data refers to. More...
enum	HiggsBounds_likelihood_type { pred = 0, obs = 1 }
	Select the kind of likelihood to return. More...

Functions
void	initialize_HiggsBounds (size_t nHiggsneut, size_t nHiggsplus, int analyses_flag)
	Interface to initialize_higgsbounds_int() More...
void	HiggsBounds_neutral_input_properties (const double Mh[], const double GammaTotal_hj[], const int CP_value[])
	Interface to higgsbounds_neutral_input_properties() More...
void	HiggsBounds_neutral_input_effC (const double ghjss_s[], const double ghjss_p[], const double ghjcc_s[], const double ghjcc_p[], const double ghjbb_s[], const double ghjbb_p[], const double ghjtt_s[], const double ghjtt_p[], const double ghjmumu_s[], const double ghjmumu_p[], const double ghjtautau_s[], const double ghjtautau_p[], const double ghjWW[], const double ghjZZ[], const double ghjZga[], const double ghjgaga[], const double ghjgg[], const double ghjhiZ[])
	Interface to higgsbounds_neutral_input_effc(). More...
void	HiggsBounds_neutral_input_SMBR (const double BR_hjss[], const double BR_hjcc[], const double BR_hjbb[], const double BR_hjtt[], const double BR_hjmumu[], const double BR_hjtautau[], const double BR_hjWW[], const double BR_hjZZ[], const double BR_hjZga[], const double BR_hjgaga[], const double BR_hjgg[])
	Interface to higgsbounds_neutral_input_smbr()
void	HiggsBounds_neutral_input_nonSMBR (const double BR_hjinvisible[], const double BR_hkhjhi[], const double BR_hjhiZ[], const double BR_hjemu[], const double BR_hjetau[], const double BR_hjmutau[], const double BR_hjHpiW[])
	Interface to higgsbounds_neutral_input_nonsmbr() More...
void	HiggsBounds_neutral_input_effC_firstgen (const double ghjuu_s[], const double ghjuu_p[], const double ghjdd_s[], const double ghjdd_p[], const double ghjee_s[], const double ghjee_p[])
	Interface to higgsbounds_neutral_input_effc_firstgen() More...
void	HiggsBounds_neutral_input_effC_FV (const double ghjuc_s[], const double ghjuc_p[], const double ghjut_s[], const double ghjut_p[], const double ghjct_s[], const double ghjct_p[], const double ghjds_s[], const double ghjds_p[], const double ghjdb_s[], const double ghjdb_p[], const double ghjsb_s[], const double ghjsb_p[])
	Interface to higgsbounds_neutral_input_effc_fv() More...
void	HiggsBounds_neutral_input_firstgenBR (const double BR_hjuu[], const double BR_hjdd[], const double BR_hjee[])
	Interface to higgsbounds_neutral_input_firstgenbr() More...
void	HiggsBounds_neutral_input_FVBR (const double BR_hjuc[], const double BR_hjds[], const double BR_hjut[], const double BR_hjdb[], const double BR_hjct[], const double BR_hjsb[])
	Interface to higgsbounds_neutral_input_fvbr() More...
void	HiggsBounds_neutral_input_LEP (const double XS_ee_hjZ_ratio[], const double XS_ee_bbhj_ratio[], const double XS_ee_tautauhj_ratio[], const double XS_ee_hjhi_ratio[])
	Interface to higgsbounds_neutral_input_lep() More...
void	HiggsBounds_neutral_input_hadr (int collider, const double CS_hj_ratio[], const double CS_gg_hj_ratio[], const double CS_bb_hj_ratio[], const double CS_hjW_ratio[], const double CS_hjZ_ratio[], const double CS_vbf_ratio[], const double CS_tthj_ratio[], const double CS_thj_tchan_ratio[], const double CS_thj_schan_ratio[], const double CS_qq_hjZ_ratio[], const double CS_gg_hjZ_ratio[], const double CS_tWhj_ratio[], const double CS_hjhi[])
	Interface to higgsbounds_neutral_input_hadr() More...
void	HiggsBounds_charged_input (const double Mhplus[], const double GammaTotal_Hpj[], const double CS_ee_HpjHmj_ratio[], double BR_tWpb, const double BR_tHpjb[], const double BR_Hpjcs[], const double BR_Hpjcb[], const double BR_Hpjtaunu[], const double BR_Hpjtb[], const double BR_HpjWZ[], const double BR_HpjhiW[])
	Interface to higgsbounds_charged_input() More...
void	HiggsBounds_charged_input_firstgenBR (const double BR_Hpjud[], const double BR_Hpjus[], const double BR_Hpjcd[], const double BR_Hpjub[], const double BR_Hpjenu[], const double BR_Hpjmunu[])
	Interface to higgsbounds_charged_input_firstgenbr() More...
void	HiggsBounds_charged_input_hadr (int collider, const double CS_Hpmjtb[], const double CS_Hpmjcb[], const double CS_Hpmjbjet[], const double CS_Hpmjcjet[], const double CS_Hpmjjetjet[], const double CS_HpmjW[], const double CS_HpmjZ[], const double CS_vbf_Hpmj[], const double CS_HpjHmj[], const double CS_Hpmjhi[])
	Interface to higgsbounds_charged_input_hadr() More...
void	HiggsBounds_charged_input_effC_fermions (const double hcjud_L[], const double hcjud_R[], const double hcjcs_L[], const double hcjcs_R[], const double hcjtb_L[], const double hcjtb_R[], const double hcjus_L[], const double hcjus_R[], const double hcjub_L[], const double hcjub_R[], const double hcjcd_L[], const double hcjcd_R[], const double hcjcb_L[], const double hcjcb_R[], const double hcjtd_L[], const double hcjtd_R[], const double hcjts_L[], const double hcjts_R[])
	Interface to higgsbounds_charged_input_effc_fermions() More...
void	HiggsBounds_charged_input_exoticBR (const double BR_Hpjud[], const double BR_Hpjus[], const double BR_Hpjcd[], const double BR_Hpjub[], const double BR_Hpjenu[], const double BR_Hpjmunu[])
	Interface to higgsbounds_charged_input_exoticbr() More...
void	HiggsBounds_get_neutral_hadr_CS (int i, int collider, double *singleH, double *ggH, double *bbH, double *VBF, double *WH, double *ZH, double *ttH, double *tH_tchan, double *tH_schan, double *qqZH, double *ggZH)
	Interface to higgsbounds_get_neutral_hadr_cs() More...
void	HiggsBounds_get_neutral_BR (int i, double *BR_hjss, double *BR_hjcc, double *BR_hjbb, double *BR_hjtt, double *BR_hjmumu, double *BR_hjtautau, double *BR_hjWW, double *BR_hjZZ, double *BR_hjZga, double *BR_hjgaga, double *BR_hjgg)
	Interface to higgsbounds_get_neutral_br() More...
void	HiggsBounds_set_mass_uncertainties (const double dMhneut[], const double dMhch[])
	Interface to higgsbounds_set_mass_uncertainties() More...
void	run_HiggsBounds (int *HBresult, int *chan, double *obsratio, int *ncombined)
	Interface to run_higgsbounds() More...
void	run_HiggsBounds_single (int h, int *HBresult, int *chan, double *obsratio, int *ncombined)
	Interface to run_higgsbounds_single() More...
void	run_HiggsBounds_full (int HBresult[], int chan[], double obsratio[], int ncombined[])
	Interface to run_higgsbounds_full() More...
void	run_HiggsBounds_classic (int *HBresult, int *chan, double *obsratio, int *ncombined)
	Interface to run_higgsbounds_classic() More...
void	HiggsBounds_get_most_sensitive_channels_per_Higgs (int nH, int pos, int *HBresult, int *chan, double *obsratio, double *predratio, int *ncombined)
	Interface to higgsbounds_get_most_sensitive_channels_per_higgs() More...
void	HiggsBounds_get_most_sensitive_channels (int pos, int *HBresult, int *chan, double *obsratio, double *predratio, int *ncombined)
	Interface to higgsbounds_get_most_sensitive_channels() More...
void	HiggsBounds_get_likelihood (int analysisID, int *Hindex, int *nc, int *cbin, double *M, double *llh, int obspred)
	Interface to higgsbounds_get_likelihood() More...
void	HiggsBounds_get_likelihood_for_Higgs (int analysisID, int cbin_in, int Hindex, int *nc, int *cbin, double *M, double *llh, int obspred)
	Interface to higgsbounds_get_likelihood_for_higgs() More...
void	HiggsBounds_get_likelihood_for_comb (int analysisID, int cbin_in, int Hindex, int *nc, int *cbin, double *M, double *llh, int obspred)
	Interface to higgsbounds_get_likelihood_for_comb() More...
void	initialize_HiggsBounds_chisqtables ()
	Interface to initialize_higgsbounds_chisqtables() More...
void	HiggsBounds_get_LEPChisq (double theory_uncertainty_1s, double *chisq_withouttheory, double *chisq_withtheory, int *channel)
	Interface to higgsbounds_get_lepchisq() More...
void	finish_HiggsBounds_chisqtables ()
	Interface to finish_higgsbounds_chisqtables() More...
void	finish_HiggsBounds ()
	Interface to finish_higgsbounds() More...
void	HiggsBounds_neutral_input_hadr_channelrates_single (int collider, int nHiggs, int p, int d, double val)
	Interface to higgsbounds_neutral_input_hadr_channelrates_single() More...
void	HiggsBounds_neutral_input_hadr_channelrates_clean ()
	Interface to higgsbounds_neutral_input_hadr_channelrates_clean() More...
double	SMBR_HWW (double Mh)
	Interface to smbr_hww() More...
double	SMBR_HZZ (double Mh)
	Interface to smbr_hzz() More...
double	SMBR_Hbb (double Mh)
	Interface to smbr_hbb() More...
double	SMBR_Htautau (double Mh)
	Interface to smbr_htautau() More...
double	SMBR_Hgamgam (double Mh)
	Interface to smbr_hgamgam() More...
double	SMBR_Hgg (double Mh)
	Interface to smbr_hgg() More...
double	SMBR_Htoptop (double Mh)
	Interface to smbr_htoptop() More...
double	SMBR_Hcc (double Mh)
	Interface to smbr_hcc() More...
double	SMBR_Hss (double Mh)
	Interface to smbr_hss() More...
double	SMBR_Hmumu (double Mh)
	Interface to smbr_hmumu() More...
double	SMBR_HZgam (double Mh)
	Interface to smbr_hzgam() More...
double	SMGamma_H (double Mh)
	Interface to smgamma_h() More...
double	SMGamma_tWpb (double mt)
	Interface to smgamma_twpb() More...
double	SMCS_tev_HW (double Mh)
	Interface to smcs_tev_hw() More...
double	SMCS_tev_HZ (double Mh)
	Interface to smcs_tev_hz() More...
double	SMCS_tev_gg_H (double Mh)
	Interface to smcs_tev_gg_h() More...
double	SMCS_tev_bb_H (double Mh)
	Interface to smcs_tev_bb_h() More...
double	SMCS_tev_vbf_H (double Mh)
	Interface to smcs_tev_vbf_h() More...
double	SMCS_tev_bg_Hb (double Mh)
	Interface to smcs_tev_bg_hb() More...
double	SMCS_tev_ttH (double Mh)
	Interface to smcs_tev_tth() More...
double	SMCS_lhc7_HW (double Mh)
	Interface to smcs_lhc7_hw() More...
double	SMCS_lhc7_HZ (double Mh)
	Interface to smcs_lhc7_hz() More...
double	SMCS_lhc7_gg_H (double Mh)
	Interface to smcs_lhc7_gg_h() More...
double	SMCS_lhc7_bb_H (double Mh)
	Interface to smcs_lhc7_bb_h() More...
double	SMCS_lhc7_vbf_H (double Mh)
	Interface to smcs_lhc7_vbf_h() More...
double	SMCS_lhc7_ttH (double Mh)
	Interface to smcs_lhc7_tth() More...
double	SMCS_lhc8_HW (double Mh)
	Interface to smcs_lhc8_hw() More...
double	SMCS_lhc8_HZ (double Mh)
	Interface to smcs_lhc8_hz() More...
double	SMCS_lhc8_gg_H (double Mh)
	Interface to smcs_lhc8_gg_h() More...
double	SMCS_lhc8_bb_H (double Mh)
	Interface to smcs_lhc8_bb_h() More...
double	SMCS_lhc8_vbf_H (double Mh)
	Interface to smcs_lhc8_vbf_h() More...
double	SMCS_lhc8_ttH (double Mh)
	Interface to smcs_lhc8_tth() More...
double	SMCS_lhc13_HW (double Mh)
	Interface to smcs_lhc13_hw() More...
double	SMCS_lhc13_HZ (double Mh)
	Interface to smcs_lhc13_hz() More...
double	SMCS_lhc13_gg_H (double Mh)
	Interface to smcs_lhc13_gg_h() More...
double	SMCS_lhc13_bb_H (double Mh)
	Interface to smcs_lhc13_bb_h() More...
double	SMCS_lhc13_vbf_H (double Mh)
	Interface to smcs_lhc13_vbf_h() More...
double	SMCS_lhc13_ttH (double Mh)
	Interface to smcs_lhc13_tth() More...
double	SMCS_effC_HZ (double Mh, int collider, double ghZZ, double ghtt_s, double ghbb_s, double ghtt_p, double ghbb_p)
	Interface to smcs_effc_hz() More...
double	SMCS_effC_gg_HZ (double Mh, int collider, double ghZZ, double ghtt_s, double ghbb_s, double ghtt_p, double ghbb_p)
	Interface to smcs_effc_gg_hz() More...
double	SMCS_effC_qq_HZ (double Mh, int collider, double ghZZ, double ghtt_s, double ghbb_s, double ghtt_p, double ghbb_p)
	Interface to smcs_effc_qq_hz() More...
double	SMCS_effC_bb_HZ (double Mh, int collider, double ghbb_s, double ghbb_p)
	Interface to smcs_effc_bb_hz() More...
double	SMCS_effC_HW (double Mh, int collider, double ghWW, double ghtt_s, double ghbb_s)
	Interface to smcs_effc_hw() More...
double	HCCS_tHc (double MHc, double gHcjt, double gHcjb, double BR_tHpjb)
	Interface to hccs_thc() More...

Detailed Description

C interface to the HiggsBounds subroutines.

This API handles conversions in array conventions, string arguments and defines enums for some flags.

• Argument types: All intent(in) scalar values (i.e. non-arrays) are passed by value, all intent(out) scalar values are passed by pointer (e.g. int *HBresult). For arrays, intent(in) arguments are passed as const arrays (e.g. const double Mh[]) and intent(out) arguments are passed as arrays (e.g. int HBresult[] in run_HiggsBounds_full()).
• Array conventions: Multidimensional arrays are stored in row major order in C vs column major order in Fortran. All array arguments have to be contiguous blocks of memory representing an array in row major order. This is true for native C arrays as well as the C accessors returned by most C++ array/tensor libraries (e.g. data() in Eigen3, Xtensor). All multidimensional function arguments are documented with detailed information. A C example:

  // 3 neutral and 1 charged Higgs bosons, e.g. 2HDM
  initialize_HiggsBounds(3, 1, LandH);
  ...
  double BR_HpjhiW[3][1];
  BR_HpjhiW[1][0] = 0.3;
  ...
  HiggsBounds_neutral_input_nonSMBR( ... , BR_HpjhiW);
  

• Any index values passed follow the Fortran convention and start at 1 (see e.g. HiggsBounds_get_neutral_hadr_CS()).
• String Arguments: We avoid passing strings from C to Fortran since it is very messy. T
  • There is no wrapper for initialize_higgsbounds(). Instead we provide a wrapper around initialize_higgsbounds_int() called initialize_HiggsBounds().
  • We replaced some string arguments by enums (e.g. HiggsBounds_likelihood_type).
  • We do not provide wrappers for the _single input subroutines, use the corresponding full input subroutines instead. (The exception is HiggsBounds_neutral_input_hadr_channelrates_single(), which takes no string arguments. Here only a wrapper around the _single verion is provided as it usually more useful than the full verion.)
• Enums: We define enums for some of the integer flags taken as arguments by the Fortran subroutines. This includes the dataset selection in initialize_HiggsBounds() (HiggsBounds_analyses_flag), the collider selection for the hadronic cross sections (HiggsBounds_collider_id), and the likelihood type (HiggsBounds_likelihood_type).

This also includes interfaces to the functions in access_SM.f90 and access_effC.f90. All cross section values are in pb.

Enumeration Type Documentation

HiggsBounds_analyses_flag

enum HiggsBounds_analyses_flag

Select which experimental analyses to use with initialize_HiggsBounds()

Enumerator
onlyL	only Lep data
onlyH	only Tevatron and LHC data
LandH	LEP, Tevatron and LHC data.
onlyP	only published results (i.e. those with an arXiv-id)
list	only data defined in usefulbits::analysislist

HiggsBounds_collider_id

enum HiggsBounds_collider_id

Select which collider the data refers to.

Used with HiggsBounds_neutral_input_hadr() and HiggsBounds_charged_input_hadr(). This value corresponds to the center of mass energy in TeV.

Enumerator
Tevatron	2 TeV \(p \bar{p}\)
LHC7	7 TeV \(pp\)
LHC8	8 TeV \(pp\)
LHC13	13 TeV \(pp\)

HiggsBounds_likelihood_type

enum HiggsBounds_likelihood_type

Select the kind of likelihood to return.

Used with the get_likelihood functions (e.g. HiggsBounds_get_likelihood())

Enumerator
pred	predicted likelihood
obs	observed likelihood

Function Documentation

finish_HiggsBounds()

void finish_HiggsBounds

(

)

Interface to finish_higgsbounds()

Deallocate data structures and close files. This needs to be called exactly once when you are done using HiggsBounds.

finish_HiggsBounds_chisqtables()

void finish_HiggsBounds_chisqtables

(

)

Interface to finish_higgsbounds_chisqtables()

Deallocate data structures used by the LEP Chisq extension. This needs to be called exactly once when you are done using HiggsBounds.

HCCS_tHc()

double HCCS_tHc	(	double	MHc,
		double	gHcjt,
		double	gHcjb,
		double	BR_tHpjb
	)

Interface to hccs_thc()

Cross section (in pb) of \( p p \to t H\pm\) production at the 13TeV LHC. Evaluated on a coefficient grid extracted from the 2HDM results of https://twiki.cern.ch/twiki/bin/view/LHCPhysics/LHCHXSWGMSSMCharged. See references on the website. If \( \mathrm{BR}(t\to H_j^+ b)>0 \) the relation \( \mathrm{BR}(t\to W^+ b) + \mathrm{BR}(t\to H^+_j b)\approx 1\) is assumed.

Parameters

MHc	mass of \( H^\pm_j \) (allowed mass range \([145,2000]~\mathrm{GeV}\))
gHcjt	scaling factor \( \kappa^{j\pm}_t \) of the charged-Higgs top coupling ( \(=1/\tan\beta\) in the 2HDM type-II)
gHcjb	scaling factor \( \kappa^{j\pm}_b \) of the charged-Higgs bottom coupling ( \(=\tan\beta\) in the 2HDM type-II)
BR_tHpjb	\( \mathrm{BR}(t\to H^+_j b) \)

HiggsBounds_charged_input()

void HiggsBounds_charged_input	(	const double	Mhplus[],
		const double	GammaTotal_Hpj[],
		const double	CS_ee_HpjHmj_ratio[],
		double	BR_tWpb,
		const double	BR_tHpjb[],
		const double	BR_Hpjcs[],
		const double	BR_Hpjcb[],
		const double	BR_Hpjtaunu[],
		const double	BR_Hpjtb[],
		const double	BR_HpjWZ[],
		const double	BR_HpjhiW[]
	)

Interface to higgsbounds_charged_input()

The parameter BR_HpjhiW is a 2-dimensional nHiggsplus x nHiggsneut array. The element at BR_HpjhiW[j][i] will be accessible in Fortran as BR_HpjhiW(j,i).

Input of charged Higgs boson's properties (mass, width, LEP cross section, BRs) to HiggsBounds Input of charged Higgs boson's masses, total widths, production cross section at lepton colliders, and branching ratios.

Parameters

Mhplus	mass values (in GeV) of the charged Higgs bosons
GammaTotal_Hpj	total widths (in GeV) of the charged Higgs bosons
CS_ee_HpjHmj_ratio	(2HDM-normalized) cross section for the LEP process \( e^+e^- \to h^+_j h^-_j\) (see manual for details on normalization)
BR_tWpb	Branching ratio for the top quark decay, \( t\to W^+ b \)
BR_tHpjb	Branching ratio for the top quark decay to charged Higgs bosons, \(t\to h^+_j b\)
BR_Hpjcs	Branching ratio for the charged Higgs decay \(h^+_j \to c \bar{s}\)
BR_Hpjcb	Branching ratio for the charged Higgs decay \(h^+_j \to c \bar{b}\)
BR_Hpjtaunu	Branching ratio for the charged Higgs decay \(h^+_j \to \tau \nu \)
BR_Hpjtb	Branching ratio for the charged Higgs decay \(h^+_j \to t\bar{b} \)
BR_HpjWZ	Branching ratio for the charged Higgs decay \(h^+_j \to W^+ Z \)
BR_HpjhiW	Branching ratio for the charged Higgs decay to a neutral Higgs boson, \(h^+_j \to h_i W^+ \)

HiggsBounds_charged_input_effC_fermions()

void HiggsBounds_charged_input_effC_fermions	(	const double	hcjud_L[],
		const double	hcjud_R[],
		const double	hcjcs_L[],
		const double	hcjcs_R[],
		const double	hcjtb_L[],
		const double	hcjtb_R[],
		const double	hcjus_L[],
		const double	hcjus_R[],
		const double	hcjub_L[],
		const double	hcjub_R[],
		const double	hcjcd_L[],
		const double	hcjcd_R[],
		const double	hcjcb_L[],
		const double	hcjcb_R[],
		const double	hcjtd_L[],
		const double	hcjtd_R[],
		const double	hcjts_L[],
		const double	hcjts_R[]
	)

Interface to higgsbounds_charged_input_effc_fermions()

Couplings of the charged Higgs bosons to fermions. The couplings are defines as in eq. 2 of the beyond Higgs paper.

HiggsBounds_charged_input_exoticBR()

void HiggsBounds_charged_input_exoticBR	(	const double	BR_Hpjud[],
		const double	BR_Hpjus[],
		const double	BR_Hpjcd[],
		const double	BR_Hpjub[],
		const double	BR_Hpjenu[],
		const double	BR_Hpjmunu[]
	)

Interface to higgsbounds_charged_input_exoticbr()

Input of charged scalar boson's exotic branching ratios Branching ratios of scalar decays to final states involving first-generation quarks or light leptons (e, mu)

Parameters

BR_Hpjud	Branching ratio for the charged Higgs decay \(h^+_j \to u \bar{d}\)
BR_Hpjus	Branching ratio for the charged Higgs decay \(h^+_j \to u \bar{s}\)
BR_Hpjcd	Branching ratio for the charged Higgs decay \(h^+_j \to c \bar{d}\)
BR_Hpjub	Branching ratio for the charged Higgs decay \(h^+_j \to u \bar{b}\)

HiggsBounds_charged_input_firstgenBR()

void HiggsBounds_charged_input_firstgenBR	(	const double	BR_Hpjud[],
		const double	BR_Hpjus[],
		const double	BR_Hpjcd[],
		const double	BR_Hpjub[],
		const double	BR_Hpjenu[],
		const double	BR_Hpjmunu[]
	)

Interface to higgsbounds_charged_input_firstgenbr()

HiggsBounds_charged_input_hadr()

void HiggsBounds_charged_input_hadr	(	int	collider,
		const double	CS_Hpmjtb[],
		const double	CS_Hpmjcb[],
		const double	CS_Hpmjbjet[],
		const double	CS_Hpmjcjet[],
		const double	CS_Hpmjjetjet[],
		const double	CS_HpmjW[],
		const double	CS_HpmjZ[],
		const double	CS_vbf_Hpmj[],
		const double	CS_HpjHmj[],
		const double	CS_Hpmjhi[]
	)

Interface to higgsbounds_charged_input_hadr()

• The parameter collider should be specified through the corresponding HiggsBounds_collider_id.
• The parameter CS_Hpmjhi is a 2-dimensional nHiggsplus x nHiggsneut array. The element at CS_Hpmjhi[j][i] will be accessible in Fortran as CS_Hpmjhi(j,i).

Input of charged Higgs boson's production cross sections at hadron colliders. Input of charged Higgs boson's production cross sections at hadron colliders to HiggsBounds. The cross section is given in pb and corresponds to the sum of the quoted process and its charge-conjugate.

Parameters

collider	selects the collider experiment for which the input is given collider experiment 2 Tevatron 7 LHC at 7 TeV 8 LHC at 8 TeV 13 LHC at 13 TeV
CS_Hpmjtb	Cross section for \(h_j^+ \bar{t} b\) (+ c.c.) production
CS_Hpmjcb	Cross section for \(h_j^+ \bar{c} b\) (+ c.c.) production
CS_Hpmjbjet	Cross section for \(h_j^+ b + j\) (+ c.c.) production (with light-flavor jet \(j\))
CS_Hpmjcjet	Cross section for \(h_j^+ c + j\) (+ c.c.) production (with light-flavor jet \(j\))
CS_qq_Hpm	Cross section for \(s\)-channel single \(h_j^\pm\) production
CS_HpmjW	Cross section for \(h_j^+ W^-\) (+ c.c.) production
CS_HpmjZ	Cross section for \(h_j^+ Z\) (+ c.c.) production
CS_vbf_Hpmj	Cross section for \(h_j^+\) (+ c.c.) production in vector boson fusion (VBF)
CS_HpjHmj	Cross section for \(h_j^+ h_j^-\) production
CS_Hpmjhi	Cross section for \(h_j^+ h_i\) (+c.c.) production

HiggsBounds_get_LEPChisq()

void HiggsBounds_get_LEPChisq	(	double	theory_uncertainty_1s,
		double *	chisq_withouttheory,
		double *	chisq_withtheory,
		int *	channel
	)

Interface to higgsbounds_get_lepchisq()

Calculate the LEP chisq value. Evaluates the \(\chi^2\) of the tabulated LEP results. Only run this after calling run_higgsbounds_classic().

Parameters

theory_uncertainty_1s	1 sigma mass uncertainty to use in the chisq calculation. This is a separate value from the one set by higgsbounds_set_mass_uncertainties().
chisq_withouttheory	\(\chi^2\)-value ignoring the theory_uncertainty_1s
chisq_withtheory	\(\chi^2\)-value including the theory_uncertainty_1s
channel	code indicating which analysis was used to derive the \(\chi^2\)-value

HiggsBounds_get_likelihood()

void HiggsBounds_get_likelihood	(	int	analysisID,
		int *	Hindex,
		int *	nc,
		int *	cbin,
		double *	M,
		double *	llh,
		int	obspred
	)

Interface to higgsbounds_get_likelihood()

• The parameter obspred should be specified through the HiggsBounds_likelihood_type.

Get exclusion likelihoods. Finds the combination of Higgs bosons (cluster) that gives the maximal likelihood and returns the likelihood for this combination. See 1507.06706 for details.

Parameters

analysisID	likelihood for which analysis
Hindex	index of the Higgs bosons that originated the dominant cluster
nc	number of Higgs bosons in the dominant cluster
cbin	binary code denoting which Higgs bosons are contained in the cluster. Calculated as \( \sum_\mathrm{Higgs} 2^{i-1} \) where the sum goes over all Higgs bosons in the clusters and \(i\) is their index. For example, for the indexing \(h1=h, h2=H, h3=A\), the combination H+A would give cbin = 6 and a cluster formed only by the h gives cbin = 1.
M	averaged mass value
llh	value of the likelihood
obspred	which likelihood to return, 'obs' = observed, 'pred' = expected/predicted

HiggsBounds_get_likelihood_for_comb()

void HiggsBounds_get_likelihood_for_comb	(	int	analysisID,
		int	cbin_in,
		int	Hindex,
		int *	nc,
		int *	cbin,
		double *	M,
		double *	llh,
		int	obspred
	)

Interface to higgsbounds_get_likelihood_for_comb()

• The parameter obspred should be specified through the HiggsBounds_likelihood_type.

Get exclusion likelihoods with some Higgs bosons excluded from the clustering. Finds the combination of Higgs bosons (cluster) that gives the best exclusion without including any of the Higgs bosons indivated by cbin_in and returns the likelihood for this combination. See 1507.06706 for details.

Parameters

analysisID	likelihood for which analysis
cbin_in	binary code indicating which Higgs bosons are not to be included in the clustering, see higgsbounds_get_likelihood() for details.
Hindex	index of the Higgs bosons that originated the dominant cluster
nc	number of Higgs bosons in the dominant cluster
cbin	binary code denoting which Higgs bosons are contained in the cluster, see higgsbounds_get_likelihood() for details.
M	averaged mass value
llh	value of the likelihood
obspred	which likelihood to return, 'obs' = observed, 'pred' = expected/predicted

HiggsBounds_get_likelihood_for_Higgs()

void HiggsBounds_get_likelihood_for_Higgs	(	int	analysisID,
		int	cbin_in,
		int	Hindex,
		int *	nc,
		int *	cbin,
		double *	M,
		double *	llh,
		int	obspred
	)

Interface to higgsbounds_get_likelihood_for_higgs()

• The parameter obspred should be specified through the HiggsBounds_likelihood_type.

Get exclusion likelihoods involving the specified Higgs boson. Similar to higgsbounds_get_likelihood_for_comb() but only consider clusters involving the Higgs specified by Hindex.

Parameters

analysisID	likelihood for which analysis
cbin_in	binary code indicating which Higgs bosons are not to be included in the clustering, see higgsbounds_get_likelihood() for details.
Hindex	index of the Higgs bosons to always include
nc	number of Higgs bosons in the dominant cluster
cbin	binary code denoting which Higgs bosons are contained in the cluster, see higgsbounds_get_likelihood() for details.
M	averaged mass value
llh	value of the likelihood
obspred	which likelihood to return, 'obs' = observed, 'pred' = expected/predicted

HiggsBounds_get_most_sensitive_channels()

void HiggsBounds_get_most_sensitive_channels	(	int	pos,
		int *	HBresult,
		int *	chan,
		double *	obsratio,
		double *	predratio,
		int *	ncombined
	)

Interface to higgsbounds_get_most_sensitive_channels()

This routine provides information about the overall most sensitive channel(s). After the HiggsBounds run this provides information about the most sensitive channels (with the position in the ranking specified by the user, up to maximal rank usefulbits::numres). The routine returns both the ratio of predicted rate over the expected limit (predratio), and over the observed limit (obsratio).

Parameters

pos	Rank in sensitivity of the channel (with 1 being the most sensitive channel)
HBresult	The HiggsBounds result (0,1 or -1) from this specific channel and Higgs boson
chan	Number of the channel, as defined in Key.dat
obsratio	Ratio of the predicted rate over the observed limit for this channel
predratio	Ratio of the predicted rate over the expected limit for this channel
ncombined	Number of Higgs bosons that have been combined in order to calculate the predicted rate

HiggsBounds_get_most_sensitive_channels_per_Higgs()

void HiggsBounds_get_most_sensitive_channels_per_Higgs	(	int	nH,
		int	pos,
		int *	HBresult,
		int *	chan,
		double *	obsratio,
		double *	predratio,
		int *	ncombined
	)

Interface to higgsbounds_get_most_sensitive_channels_per_higgs()

This routine provides information about the most sensitive channel(s) for a specific Higgs boson. After the HiggsBounds run this subroutine provides information about the most sensitive channels (with the position in the ranking specified by the user, up to maximal rank usefulbits::numres) for a given Higgs boson. The routine returns both the ratio of predicted rate over the expected limit (predratio), and over the observed limit (obsratio).

Parameters

nH	Index of the Higgs boson, enumerating first over the neutral Higgs bosons then the charged Higgs bosons
pos	Rank in sensitivity of the channel (with 1 being the most sensitive channel)
HBresult	The HiggsBounds result (0,1 or -1) from this specific channel and Higgs boson
chan	Number of the channel, as defined in Key.dat
obsratio	Ratio of the predicted rate over the observed limit for this channel
predratio	Ratio of the predicted rate over the expected limit for this channel
ncombined	Number of Higgs bosons that have been combined in order to calculate the predicted rate

HiggsBounds_get_neutral_BR()

void HiggsBounds_get_neutral_BR	(	int	i,
		double *	BR_hjss,
		double *	BR_hjcc,
		double *	BR_hjbb,
		double *	BR_hjtt,
		double *	BR_hjmumu,
		double *	BR_hjtautau,
		double *	BR_hjWW,
		double *	BR_hjZZ,
		double *	BR_hjZga,
		double *	BR_hjgaga,
		double *	BR_hjgg
	)

Interface to higgsbounds_get_neutral_br()

The index i of the requested Higgs boson starts at 1.

Get neutral Higgs boson's branching ratios (for Higgs decays into SM final states). This subroutine returns the branching ratios of the neutral Higgs boson \(h_i\) decays into SM final states from the internal data in HiggsBounds.

Parameters

i	Index of the neutral Higgs boson
BR_hjss	Branching ratio of Higgs decay to strange quarks, \( h_i \to s \bar{s} \)
BR_hjcc	Branching ratio of Higgs decay to charm quarks, \( h_i \to c \bar{c} \)
BR_hjbb	Branching ratio of Higgs decay to bottom quarks, \( h_i \to b \bar{b} \)
BR_hjtt	Branching ratio of Higgs decay to top quarks, \( h_i \to t \bar{t} \)
BR_hjmumu	Branching ratio of Higgs decay to muons, \( h_i \to \mu^+ \mu^- \)
BR_hjtautau	Branching ratio of Higgs decay to tau leptons, \( h_i \to \tau^+ \tau^- \)
BR_hjWW	Branching ratio of Higgs decay to W bosons, \( h_i \to W^+W^- \)
BR_hjZZ	Branching ratio of Higgs decay to Z bosons, \( h_i \to ZZ \)
BR_hjZga	Branching ratio of Higgs decay to a Z boson and a photon, \( h_i \to Z\gamma \)
BR_hjgaga	Branching ratio of Higgs decay to photons, \( h_i \to \gamma\gamma \)
BR_hjgg	Branching ratio of Higgs decay to gluons, \( h_i \to gg \)

HiggsBounds_get_neutral_hadr_CS()

void HiggsBounds_get_neutral_hadr_CS	(	int	i,
		int	collider,
		double *	singleH,
		double *	ggH,
		double *	bbH,
		double *	VBF,
		double *	WH,
		double *	ZH,
		double *	ttH,
		double *	tH_tchan,
		double *	tH_schan,
		double *	qqZH,
		double *	ggZH
	)

Interface to higgsbounds_get_neutral_hadr_cs()

• The index i of the requested Higgs boson starts at 1.
• The parameter collider should be specified through the corresponding HiggsBounds_collider_id.

Get neutral Higgs boson's (SM-normalized) hadronic cross section. This subroutines returns the SM-normalized hadronic cross sections for the neutral Higgs boson \(h_i\) and the specified hadron collider from the internal data in HiggsBounds.

Parameters

i	Index of the neutral Higgs boson
collider	selects the collider experiment for which the input is given collider experiment 2 Tevatron 7 LHC at 7 TeV 8 LHC at 8 TeV 13 LHC at 13 TeV
singleH	(SM-normalized) cross section for single Higgs production
ggH	(SM-normalized) cross section for Higgs production in gluon fusion, \( gg\to h_i\)
bbH	(SM-normalized) cross section for Higgs production in association with bottom quarks, \( b\bar{b}\to h_i\)
VBF	(SM-normalized) cross section for Higgs production in vector boson fusion
WH	(SM-normalized) cross section for Higgs production in association with a W boson
ZH	(SM-normalized) cross section for Higgs production in association with a Z boson
ttH	(SM-normalized) cross section for Higgs production in association with a top quark pair
tH_tchan	(SM-normalized) cross section for Higgs production in association with a top quark (t-channel)
tH_schan	(SM-normalized) cross section for Higgs production in association with a top quark (s-channel)
qqZH	(SM-normalized) cross section for qq-bar-initiated Higgs production in association with a Z boson
ggZH	(SM-normalized) cross section for gg-initiated Higgs production in association with a Z boson

HiggsBounds_neutral_input_effC()

void HiggsBounds_neutral_input_effC	(	const double	ghjss_s[],
		const double	ghjss_p[],
		const double	ghjcc_s[],
		const double	ghjcc_p[],
		const double	ghjbb_s[],
		const double	ghjbb_p[],
		const double	ghjtt_s[],
		const double	ghjtt_p[],
		const double	ghjmumu_s[],
		const double	ghjmumu_p[],
		const double	ghjtautau_s[],
		const double	ghjtautau_p[],
		const double	ghjWW[],
		const double	ghjZZ[],
		const double	ghjZga[],
		const double	ghjgaga[],
		const double	ghjgg[],
		const double	ghjhiZ[]
	)

Interface to higgsbounds_neutral_input_effc().

The parameter ghjhiZ is a 2-dimensional nHiggsneut x nHiggsneut symmetric array.

Input of neutral Higgs boson's effective couplings (aka scale factors) to HiggsBounds. These are used to obtain production cross sections and branching ratios by approximately rescaling the corresponding predictions for a SM Higgs boson.

Parameters

ghjss_s	Scalar (SM-normalized) effective Higgs couplings to strange quarks
ghjss_p	Pseudoscalar (SM-normalized) effective Higgs coupling to strange quarks
ghjcc_s	Scalar (SM-normalized) effective Higgs coupling to charm quarks
ghjcc_p	Pseudoscalar (SM-normalized) effective Higgs coupling to charm quarks
ghjbb_s	Scalar (SM-normalized) effective Higgs coupling to bottom quarks
ghjbb_p	Pseudoscalar (SM-normalized) effective Higgs coupling to bottom quarks
ghjtt_s	Scalar (SM-normalized) effective Higgs coupling to top quarks
ghjtt_p	Pseudoscalar (SM-normalized) effective Higgs coupling to top quarks
ghjmumu_s	Scalar (SM-normalized) effective Higgs coupling to muons
ghjmumu_p	Pseudoscalar (SM-normalized) effective Higgs coupling to muons
ghjtautau_s	Scalar (SM-normalized) effective Higgs coupling to tau leptons
ghjtautau_p	Pseudoscalar (SM-normalized) effective Higgs coupling to tau leptons
ghjWW	(SM-normalized) effective Higgs coupling to W bosons
ghjZZ	(SM-normalized) effective Higgs coupling to Z bosons
ghjZga	(SM-normalized) effective Higgs coupling to a Z boson and a photon
ghjgaga	(SM-normalized) effective Higgs coupling to photons
ghjgg	(SM-normalized) effective Higgs coupling to gluons
ghjhiZ	(SM-normalized) effective Higgs-Higgs-Z boson coupling

HiggsBounds_neutral_input_effC_firstgen()

void HiggsBounds_neutral_input_effC_firstgen	(	const double	ghjuu_s[],
		const double	ghjuu_p[],
		const double	ghjdd_s[],
		const double	ghjdd_p[],
		const double	ghjee_s[],
		const double	ghjee_p[]
	)

Interface to higgsbounds_neutral_input_effc_firstgen()

Input of neutral Higgs boson's effective couplings (aka scale factors) to HiggsBounds. These are used to obtain production cross sections.

Parameters

ghjuu_s	Scalar (SM-normalized) effective Higgs couplings to up quarks
ghjuu_p	Pseudoscalar (SM-normalized) effective Higgs coupling to up quarks
ghjdd_s	Scalar (SM-normalized) effective Higgs coupling to down quarks
ghjdd_p	Pseudoscalar (SM-normalized) effective Higgs coupling to down quarks
ghjee_s	Scalar (SM-normalized) effective Higgs coupling to electrons
ghjee_p	Pseudoscalar (SM-normalized) effective Higgs coupling to electrons

HiggsBounds_neutral_input_effC_FV()

void HiggsBounds_neutral_input_effC_FV	(	const double	ghjuc_s[],
		const double	ghjuc_p[],
		const double	ghjut_s[],
		const double	ghjut_p[],
		const double	ghjct_s[],
		const double	ghjct_p[],
		const double	ghjds_s[],
		const double	ghjds_p[],
		const double	ghjdb_s[],
		const double	ghjdb_p[],
		const double	ghjsb_s[],
		const double	ghjsb_p[]
	)

Interface to higgsbounds_neutral_input_effc_fv()

Input of neutral Higgs boson's flavor violating couplings to HiggsBounds. These dimensionless couplings are absent in the SM.

Parameters

ghjuc_s	Scalar flavor violating Higgs coupling to up and charm quark
ghjuc_p	Pseudoscalar flavor violating Higgs coupling to up and charm quark
ghjut_s	Scalar flavor violating Higgs coupling to up and top quark
ghjut_p	Pseudoscalar flavor violating Higgs coupling to up and top quark
ghjct_s	Scalar flavor violating Higgs coupling to charm and top quark
ghjct_p	Pseudoscalar flavor violating Higgs coupling to charm and top quark
ghjds_s	Scalar flavor violating Higgs coupling to down and strange quark
ghjds_p	Pseudoscalar flavor violating Higgs coupling to down and strange quark
ghjdb_s	Scalar flavor violating Higgs coupling to down and bottom quark
ghjdb_p	Pseudoscalar flavor violating Higgs coupling to down and bottom quark
ghjsb_s	Scalar flavor violating Higgs coupling to strange and bottom quark
ghjsb_p	Pseudoscalar flavor violating Higgs coupling to strange and bottom quark

HiggsBounds_neutral_input_firstgenBR()

void HiggsBounds_neutral_input_firstgenBR	(	const double	BR_hjuu[],
		const double	BR_hjdd[],
		const double	BR_hjee[]
	)

Interface to higgsbounds_neutral_input_firstgenbr()

Input of neutral Higgs boson's branching ratios to first generation SM fermions.

Parameters

BR_hjuu	Branching ratio of Higgs decay into up-quarks, \( h_j \to u \bar{u} \)
BR_hjuu	Branching ratio of Higgs decay into down-quarks, \( h_j \to d \bar{d} \)
BR_hjuu	Branching ratio of Higgs decay into electrons, \( h_j \to e^+e^- \)

HiggsBounds_neutral_input_FVBR()

void HiggsBounds_neutral_input_FVBR	(	const double	BR_hjuc[],
		const double	BR_hjds[],
		const double	BR_hjut[],
		const double	BR_hjdb[],
		const double	BR_hjct[],
		const double	BR_hjsb[]
	)

Interface to higgsbounds_neutral_input_fvbr()

Input of neutral Higgs boson's branching ratios to first generation SM fermions.

Parameters

BR_hjuc	Branching ratio of Higgs decay into up-quark and charm quark, \( h_j \to u \bar{d} + c.c. \)
BR_hjds	Branching ratio of Higgs decay into down-quark and strange quark, \( h_j \to d \bar{s} + c.c. \)
BR_hjut	Branching ratio of Higgs decay into up-quark and top quark, \( h_j \to u \bar{t} + c.c. \)
BR_hjdb	Branching ratio of Higgs decay into down-quark and bottom quark, \( h_j \to d \bar{b} + c.c. \)
BR_hjct	Branching ratio of Higgs decay into charm-quark and top quark, \( h_j \to c \bar{t} + c.c. \)
BR_hjsb	Branching ratio of Higgs decay into strange-quark and bottom quark, \( h_j \to s \bar{b} + c.c. \)

HiggsBounds_neutral_input_hadr()

void HiggsBounds_neutral_input_hadr	(	int	collider,
		const double	CS_hj_ratio[],
		const double	CS_gg_hj_ratio[],
		const double	CS_bb_hj_ratio[],
		const double	CS_hjW_ratio[],
		const double	CS_hjZ_ratio[],
		const double	CS_vbf_ratio[],
		const double	CS_tthj_ratio[],
		const double	CS_thj_tchan_ratio[],
		const double	CS_thj_schan_ratio[],
		const double	CS_qq_hjZ_ratio[],
		const double	CS_gg_hjZ_ratio[],
		const double	CS_tWhj_ratio[],
		const double	CS_hjhi[]
	)

Interface to higgsbounds_neutral_input_hadr()

• The parameter collider should be specified through the corresponding HiggsBounds_collider_id.
• The parameter CS_hjhi is a 2-dimensional nHiggsneut x nHiggsneut symmetric array.

Input of neutral Higgs boson's cross sections for hadron colliders.

Parameters

collider	selects the collider experiment for which the input is given collider experiment 2 Tevatron 7 LHC at 7 TeV 8 LHC at 8 TeV 13 LHC at 13 TeV
CS_hj_ratio	(SM-normalized) cross section for single Higgs production
CS_gg_hj_ratio	(SM-normalized) cross section for gluon fusion production, \(gg\to h_j\)
CS_bb_hj_ratio	(SM-normalized) cross section for Higgs production in association with bottom quarks, \(b\bar{b}\to h_j\)
CS_hjW_ratio	(SM-normalized) cross section for Higgs production in association with a W boson
CS_hjZ_ratio	(SM-normalized) cross section for Higgs production in association with a Z boson
CS_vbf_ratio	(SM-normalized) cross section for Higgs production in vector boson fusion
CS_tthj_ratio	(SM-normalized) cross section for Higgs production in association with a top quark pair
CS_thj_tchan_ratio	(SM-normalized) cross section for Higgs production in association with single top quark (t-channel process)
CS_thj_schan_ratio	(SM-normalized) cross section for Higgs production in association with single top quark (s-channel process)
CS_qq_hjZ_ratio	(SM-normalized) cross section for qq-bar-initiated Higgs production in association with a Z boson
CS_gg_hjZ_ratio	(SM-normalized) cross section for gg-initiated Higgs production in association with a Z boson
CS_tWhj_ratio	(SM-normalized) cross sections fo Higgs prodoction in association with a top quark and a W
CS_hjhi	Cross section (in pb) for non-resonant double Higgs production

HiggsBounds_neutral_input_hadr_channelrates_clean()

void HiggsBounds_neutral_input_hadr_channelrates_clean

(

)

Interface to higgsbounds_neutral_input_hadr_channelrates_clean()

Resets the channelrates. Use to undo values set by HiggsBounds_neutral_input_hadr_channelrates_single() and HiggsBounds_neutral_input_hadr_channelrates()

HiggsBounds_neutral_input_hadr_channelrates_single()

void HiggsBounds_neutral_input_hadr_channelrates_single	(	int	collider,
		int	nHiggs,
		int	p,
		int	d,
		double	val
	)

Interface to higgsbounds_neutral_input_hadr_channelrates_single()

• We do not provide a C interface to higgsbounds_neutral_input_hadr_channelrates(), use this function instead.
• The parameter collider should be specified through the corresponding HiggsBounds_collider_id.

Sets a single channelrate. Input an element of the channelrate matrix, see higgsbounds_neutral_input_hadr_channelrates() Elements of the matrix channelrates with values < 0 will be overwritten by XS times BR using the narrow width approximation.

Parameters

collider	selects the collider experiment for which the input is given collider experiment 2 Tevatron 7 LHC at 7 TeV 8 LHC at 8 TeV 13 LHC at 13 TeV
nHiggs	Index of the Higgs boson
p	Index of the production mode
d	Index of the decay mode
val	value to set

HiggsBounds_neutral_input_LEP()

void HiggsBounds_neutral_input_LEP	(	const double	XS_ee_hjZ_ratio[],
		const double	XS_ee_bbhj_ratio[],
		const double	XS_ee_tautauhj_ratio[],
		const double	XS_ee_hjhi_ratio[]
	)

Interface to higgsbounds_neutral_input_lep()

The parameter XS_ee_hjhi_ratio is a 2-dimensional nHiggsneut x nHiggsneut symmetric array.

Input of neutral Higgs boson's cross sections for lepton collider (LEP). (See manual for details on normalization.)

Parameters

XS_ee_hjZ_ratio	(SM-normalized) cross section for Higgs-Strahlung, \( e^+e^- \to h_j Z\)
XS_ee_bbhj_ratio	(SM-normalized) cross section for \( b\bar{b}\)-associated production, \( e^+e^- \to h_j b\bar{b}\)
XS_ee_tautauhj_ratio	(SM-normalized) cross section for \( \tau^+\tau^-\)-associated production, \( e^+e^- \to h_j \tau^+\tau^-\)
XS_ee_hjhi_ratio	(2HDM-normalized) cross section for double Higgs production, \( e^+e^- \to h_i h_j\)

HiggsBounds_neutral_input_nonSMBR()

void HiggsBounds_neutral_input_nonSMBR	(	const double	BR_hjinvisible[],
		const double	BR_hkhjhi[],
		const double	BR_hjhiZ[],
		const double	BR_hjemu[],
		const double	BR_hjetau[],
		const double	BR_hjmutau[],
		const double	BR_hjHpiW[]
	)

Interface to higgsbounds_neutral_input_nonsmbr()

• The parameter BR_hkhjhi is a 3-dimensional nHiggsneut x nHiggsneut x nHiggsneut array. The element BR_hkhjhi[k][j][i] will be accessible in Fortran as BR_hkhjhi(k,j,i).
• The parameter BR_hjhiZ is a 2-dimensional nHiggsneut x nHiggsneut array. The element at BR_hjhiZ[j][i] will be accessible in Fortran as BR_hjhiZ(j,i).
• The parameter BR_hjHpiW is a 2-dimensional nHiggsneut x nHiggsplus array. The element at BR_hjHpiW[j][i] will be accessible in Fortran as BR_hjHpiW(j,i).

Input of neutral Higgs boson's branching ratios for non-Standard Model final states to HiggsBounds.

Parameters

BR_hjinvisible	Branching ratio of Higgs decay into invisible final states, \( h_j \to \mathrm{invisible} \)
BR_hkhjhi	Branching ratio of Higgs decay into two other Higgs bosons, \(h_k\to h_i h_j\)
BR_hjhiZ	Branching ratio of Higgs decay into a Higgs boson and a Z boson, \(h_j\to h_i Z\)
BR_hjemu	Branching ratio of lepton-flavor-violating Higgs decay into electron and muon, \(h_j\to e^\pm \mu^\mp\)
BR_hjetau	Branching ratio of lepton-flavor-violating Higgs decay into electron and tau lepton, \(h_j\to e^\pm \tau^\mp\)
BR_hjmutau	Branching ratio of lepton-flavor-violating Higgs decay into muon and tau lepton, \(h_j\to \mu^\pm \tau^\mp\)
BR_hjHpiW	Branching ratio of Higgs decay into a charged Higgs boson and a W boson, \(h_j\to h^\pm_i W^\mp\)

HiggsBounds_neutral_input_properties()

void HiggsBounds_neutral_input_properties	(	const double	Mh[],
		const double	GammaTotal_hj[],
		const int	CP_value[]
	)

Interface to higgsbounds_neutral_input_properties()

Input of neutral Higgs boson's properties (mass, total width, CP) to HiggsBounds. Note: When using the effective coupling input the total width can be internally derived from the provided input (effective couplings and branching ratios of Higgs decays to non-SM final states) under the assumption of no additional BSM contributions to the total width beyond those provided in the input. This derivation is activated when providing a negative value for the total width.

Parameters

Mh	mass values (in GeV) of the neutral Higgs bosons
GammaTotal_hj	total decay width (in GeV) of the neutral Higgs bosons
CP_value	CP properties of neutral Higgs bosons (+1: CP-even, -1: CP-odd, 0: CP-mixed)

HiggsBounds_set_mass_uncertainties()

void HiggsBounds_set_mass_uncertainties	(	const double	dMhneut[],
		const double	dMhch[]
	)

Interface to higgsbounds_set_mass_uncertainties()

Input of theoretical Higgs mass uncertainties to HiggsBounds.

Parameters

dMhneut	Theoretical mass uncertainties (in GeV) for the neutral Higgs bosons
dMhch	Theoretical mass uncertainties (in GeV) for the charged Higgs bosons

initialize_HiggsBounds()

void initialize_HiggsBounds	(	size_t	nHiggsneut,
		size_t	nHiggsplus,
		int	analyses_flag
	)

Interface to initialize_higgsbounds_int()

Parameters

nHiggsneut	Number of neutral Higgs bosons in the model
nHiggsplus	Number of charged Higgs bosons in the model
analyses_flag	dataset from HiggsBounds_analyses_flag

initialize_HiggsBounds_chisqtables()

void initialize_HiggsBounds_chisqtables

(

)

Interface to initialize_higgsbounds_chisqtables()

Initialize the LEP Chisq extension. If the extension is used this needs to be called exactly once and before the call to initialize_higgsbounds

run_HiggsBounds()

void run_HiggsBounds	(	int *	HBresult,
		int *	chan,
		double *	obsratio,
		int *	ncombined
	)

Interface to run_higgsbounds()

Runs HiggsBounds. Runs HiggsBounds on the previously specified model point. Per default, it calls higgsbounds_subroutines::run_higgsbounds_full, i.e. for each Higgs boson in the model, HiggsBounds first finds the most sensitive experimental analysis (out of the dataset specified earlier by whichanalyses in initialize_higgsbounds), and then tests the predicted rate against the observed limit in this analysis. The output is then connected by a logical "OR", i.e. if one Higgs boson of the model is excluded, then the model is regarded excluded.

If the logical parameter usefulbits::run_HB_classic is set True, however, the old (version 3) method of determining the output only from the experimental analysis that is most sensitive among all Higgs bosons is being used.

Note, that if many data points are tested at the same time (as for inputmethod==datfiles), this subroutine only returns the results of the last datapoint. The full results are saved in fullHBres.

Parameters

HBresult	Main binary HiggsBounds result, HBresult description 0 excluded (95CL) 1 allowed (95CL) -1 invalid point
chan	Number of the channel predicted to have the highest statistical sensitivity, as defined in Key.dat
obsratio	Ratio of the predicted rate over the observed limit for this channel
ncombined	Number of Higgs bosons that have been combined in order to calculate the obsratio

run_HiggsBounds_classic()

void run_HiggsBounds_classic	(	int *	HBresult,
		int *	chan,
		double *	obsratio,
		int *	ncombined
	)

Interface to run_higgsbounds_classic()

Run HiggsBounds in classic mode. Uses the old (version 3) method of determining the output only from the experimental analysis that is most sensitive among all Higgs bosons.

This should only be used for comparison purposes or as a prerequisite to the LEP Chisq extension (see higgsbounds_get_lepchisq()).

Parameters

HBresult	Main binary HiggsBounds result, HBresult description 0 excluded (95CL) 1 allowed (95CL) -1 invalid point
chan	Number of the channel predicted to have the highest statistical sensitivity, as defined in Key.dat
obsratio	Ratio of the predicted rate over the observed limit for this channel
ncombined	Number of Higgs bosons that have been combined in order to calculate the obsratio

run_HiggsBounds_full()

void run_HiggsBounds_full	(	int	HBresult[],
		int	chan[],
		double	obsratio[],
		int	ncombined[]
	)

Interface to run_higgsbounds_full()

Runs HiggsBounds. Runs HiggsBounds on the previously specified model point. For each Higgs boson in the model, HiggsBounds first finds the most sensitive experimental analysis (out of the dataset specified earlier by usefulbits::whichanalyses in higgsbounds_subroutines::initialize_higgsbounds), and then tests the predicted rate against the observed limit in this analysis.

The output arrays are of (length number of neutral and charged Higgs bosons) + 1. The zeroth entry represents the global result (i.e. a logical AND combination of the outcomes of the individual Higgs bosons), the remaining entries enumerate the outcome for the neutral and charged Higgs bosons.

Parameters

HBresult	Main binary HiggsBounds result, HBresult description 0 excluded (95CL) 1 allowed (95CL) -1 invalid point
chan	Number of the channel predicted to have the highest statistical sensitivity, as defined in Key.dat
obsratio	Ratio of the predicted rate over the observed limit for this channel
ncombined	Number of Higgs bosons that have been combined in order to calculate the obsratio

run_HiggsBounds_single()

void run_HiggsBounds_single	(	int	h,
		int *	HBresult,
		int *	chan,
		double *	obsratio,
		int *	ncombined
	)

Interface to run_higgsbounds_single()

Runs HiggsBounds and returns results for a single Higgs boson. Runs HiggsBounds by internally calling higgsbounds_subroutines::run_higgsbounds and extracting the result for a single Higgs boson specified by the index h.

Parameters

h	Index of the Higgs boson for which the results should be given
HBresult	Main binary HiggsBounds result, HBresult description 0 excluded (95CL) 1 allowed (95CL) -1 invalid point
chan	Number of the channel predicted to have the highest statistical sensitivity, as defined in Key.dat
obsratio	Ratio of the predicted rate over the observed limit for this channel
ncombined	Number of Higgs bosons that have been combined in order to calculate the obsratio

SMBR_Hbb()

double SMBR_Hbb

(

double

Mh

)

Interface to smbr_hbb()

SM Higgs branching ratio for the decay \( H\to bb\) as a function of mass. Prediction is taken from the CERN Yellow Report 4 by the LHC Higgs Cross Section Working Group.

Parameters

Mh	mass of the SM Higgs boson (allowed range \([0,1000]~\mathrm{GeV}\))

SMBR_Hcc()

double SMBR_Hcc

(

double

Mh

)

Interface to smbr_hcc()

SM Higgs branching ratio for the decay \( H\to cc\) as a function of mass. Prediction is taken from the CERN Yellow Report 4 by the LHC Higgs Cross Section Working Group.

Parameters

Mh	mass of the SM Higgs boson (allowed range \([0,1000]~\mathrm{GeV}\))

SMBR_Hgamgam()

double SMBR_Hgamgam

(

double

Mh

)

Interface to smbr_hgamgam()

SM Higgs branching ratio for the decay \( H\to \gamma\gamma\) as a function of mass. Prediction is taken from the CERN Yellow Report 4 by the LHC Higgs Cross Section Working Group.

Parameters

Mh	mass of the SM Higgs boson (allowed range \([0,1000]~\mathrm{GeV}\))

SMBR_Hgg()

double SMBR_Hgg

(

double

Mh

)

Interface to smbr_hgg()

SM Higgs branching ratio for the decay \( H\to gg\) as a function of mass. Prediction is taken from the CERN Yellow Report 4 by the LHC Higgs Cross Section Working Group.

Parameters

Mh	mass of the SM Higgs boson (allowed range \([0,1000]~\mathrm{GeV}\))

SMBR_Hmumu()

double SMBR_Hmumu

(

double

Mh

)

Interface to smbr_hmumu()

SM Higgs branching ratio for the decay \( H\to \mu\mu\) as a function of mass. Prediction is taken from the CERN Yellow Report 4 by the LHC Higgs Cross Section Working Group.

Parameters

Mh	mass of the SM Higgs boson (allowed range \([0,1000]~\mathrm{GeV}\))

SMBR_Hss()

double SMBR_Hss

(

double

Mh

)

Interface to smbr_hss()

SM Higgs branching ratio for the decay \( H\to ss\) as a function of mass. Prediction is taken from the CERN Yellow Report 4 by the LHC Higgs Cross Section Working Group.

Parameters

Mh	mass of the SM Higgs boson (allowed range \([0,1000]~\mathrm{GeV}\))

SMBR_Htautau()

double SMBR_Htautau

(

double

Mh

)

Interface to smbr_htautau()

SM Higgs branching ratio for the decay \( H\to \tau\tau\) as a function of mass. Prediction is taken from the CERN Yellow Report 4 by the LHC Higgs Cross Section Working Group.

Parameters

Mh	mass of the SM Higgs boson (allowed range \([0,1000]~\mathrm{GeV}\))

SMBR_Htoptop()

double SMBR_Htoptop

(

double

Mh

)

Interface to smbr_htoptop()

SM Higgs branching ratio for the decay \( H\to tt\) as a function of mass. Prediction is taken from the CERN Yellow Report 4 by the LHC Higgs Cross Section Working Group.

Parameters

Mh	mass of the SM Higgs boson (allowed range \([0,1000]~\mathrm{GeV}\))

SMBR_HWW()

double SMBR_HWW

(

double

Mh

)

Interface to smbr_hww()

SM Higgs branching ratio for the decay \( H\to WW^{(*)}\) as a function of mass. Prediction is taken from the CERN Yellow Report 4 by the LHC Higgs Cross Section Working Group.

Parameters

Mh	mass of the SM Higgs boson (allowed range \([0,1000]~\mathrm{GeV}\))

SMBR_HZgam()

double SMBR_HZgam

(

double

Mh

)

Interface to smbr_hzgam()

SM Higgs branching ratio for the decay \( H\to Z\gamma \) as a function of mass. Prediction is taken from the CERN Yellow Report 4 by the LHC Higgs Cross Section Working Group.

Parameters

Mh	mass of the SM Higgs boson (allowed range \([0,1000]~\mathrm{GeV}\))

SMBR_HZZ()

double SMBR_HZZ

(

double

Mh

)

Interface to smbr_hzz()

SM Higgs branching ratio for the decay \( H\to ZZ^{(*)}\) as a function of mass. Prediction is taken from the CERN Yellow Report 4 by the LHC Higgs Cross Section Working Group.

Parameters

Mh	mass of the SM Higgs boson (allowed range \([0,1000]~\mathrm{GeV}\))

SMCS_effC_bb_HZ()

double SMCS_effC_bb_HZ	(	double	Mh,
		int	collider,
		double	ghbb_s,
		double	ghbb_p
	)

Interface to smcs_effc_bb_hz()

The parameter collider should be specified through the corresponding HiggsBounds_collider_id.

Cross section (in pb) of \(b\bar{b}\to HZ\) production, as a function of mass and effective Higgs couplings (aka scale factors). Both scalar and pseudoscalar coupling to fermions are taken into account (see manual for more information). Prediction is evaluated from fits to VH@NNLO-2 data.

Parameters

Mh	mass of the Higgs boson (allowed mass range \([10,3000]~\mathrm{GeV}\))
collider	selects the collider experiment for which the input is given collider experiment 2 Tevatron 7 LHC at 7 TeV 8 LHC at 8 TeV 13 LHC at 13 TeV
ghbb_s	Scalar (SM-normalized) effective Higgs coupling to bottom quarks
ghbb_p	Pseudoscalar (SM-normalized) effective Higgs coupling to bottom quarks

SMCS_effC_gg_HZ()

double SMCS_effC_gg_HZ	(	double	Mh,
		int	collider,
		double	ghZZ,
		double	ghtt_s,
		double	ghbb_s,
		double	ghtt_p,
		double	ghbb_p
	)

Interface to smcs_effc_gg_hz()

The parameter collider should be specified through the corresponding HiggsBounds_collider_id.

Cross section (in pb) of \(gg\to HZ\) production, as a function of mass and effective Higgs couplings (aka scale factors). Both scalar and pseudoscalar coupling to fermions are taken into account (see manual for more information). Prediction is evaluated from fits to VH@NNLO-2 data.

Parameters

Mh	mass of the Higgs boson (allowed mass range \([10,3000]~\mathrm{GeV}\))
collider	selects the collider experiment for which the input is given collider experiment 2 Tevatron 7 LHC at 7 TeV 8 LHC at 8 TeV 13 LHC at 13 TeV
ghZZ	(SM-normalized) effective Higgs coupling to Z bosons
ghtt_s	Scalar (SM-normalized) effective Higgs coupling to top quarks
ghbb_s	Scalar (SM-normalized) effective Higgs coupling to bottom quarks
ghtt_p	Pseudoscalar (SM-normalized) effective Higgs coupling to top quarks
ghbb_p	Pseudoscalar (SM-normalized) effective Higgs coupling to bottom quarks

SMCS_effC_HW()

double SMCS_effC_HW	(	double	Mh,
		int	collider,
		double	ghWW,
		double	ghtt_s,
		double	ghbb_s
	)

Interface to smcs_effc_hw()

The parameter collider should be specified through the corresponding HiggsBounds_collider_id.

Cross section (in pb) of inclusive \(HZ\) production, as a function of mass and effective Higgs couplings. Both scalar and pseudoscalar coupling to fermions are taken into account (see manual for more information). Prediction is evaluated from fits to VH@NNLO-2 data.

Parameters

Mh	mass of the Higgs boson (allowed mass range \([10,3000]~\mathrm{GeV}\))
collider	selects the collider experiment for which the input is given collider experiment 2 Tevatron 7 LHC at 7 TeV 8 LHC at 8 TeV 13 LHC at 13 TeV
ghWW	(SM-normalized) effective Higgs coupling to Z bosons
ghtt_s	Scalar (SM-normalized) effective Higgs coupling to top quarks
ghbb_s	Scalar (SM-normalized) effective Higgs coupling to bottom quarks

SMCS_effC_HZ()

double SMCS_effC_HZ	(	double	Mh,
		int	collider,
		double	ghZZ,
		double	ghtt_s,
		double	ghbb_s,
		double	ghtt_p,
		double	ghbb_p
	)

Interface to smcs_effc_hz()

The parameter collider should be specified through the corresponding HiggsBounds_collider_id.

Cross section (in pb) of inclusive \(HZ\) production, as a function of mass and effective Higgs couplings. Both scalar and pseudoscalar coupling to fermions are taken into account (see manual for more information). Prediction is evaluated from fits to VH@NNLO-2 data.

Parameters

Mh	mass of the Higgs boson (allowed mass range \([10,3000]~\mathrm{GeV}\))
collider	selects the collider experiment for which the input is given collider experiment 2 Tevatron 7 LHC at 7 TeV 8 LHC at 8 TeV 13 LHC at 13 TeV
ghZZ	(SM-normalized) effective Higgs coupling to Z bosons
ghtt_s	Scalar (SM-normalized) effective Higgs coupling to top quarks
ghbb_s	Scalar (SM-normalized) effective Higgs coupling to bottom quarks
ghtt_p	Pseudoscalar (SM-normalized) effective Higgs coupling to top quarks
ghbb_p	Pseudoscalar (SM-normalized) effective Higgs coupling to bottom quarks

SMCS_effC_qq_HZ()

double SMCS_effC_qq_HZ	(	double	Mh,
		int	collider,
		double	ghZZ,
		double	ghtt_s,
		double	ghbb_s,
		double	ghtt_p,
		double	ghbb_p
	)

Interface to smcs_effc_qq_hz()

The parameter collider should be specified through the corresponding HiggsBounds_collider_id.

Cross section (in pb) of \(q\bar{q}\to HZ\) production (including \(b\bar{b} \to HZ\)), as a function of mass and effective Higgs couplings (aka scale factors). Both scalar and pseudoscalar coupling to fermions are taken into account (see manual for more information). Prediction is evaluated from fits to VH@NNLO-2 data.

Parameters

Mh	mass of the Higgs boson (allowed mass range \([10,3000]~\mathrm{GeV}\))
collider	selects the collider experiment for which the input is given collider experiment 2 Tevatron 7 LHC at 7 TeV 8 LHC at 8 TeV 13 LHC at 13 TeV
ghZZ	(SM-normalized) effective Higgs coupling to Z bosons
ghtt_s	Scalar (SM-normalized) effective Higgs coupling to top quarks
ghbb_s	Scalar (SM-normalized) effective Higgs coupling to bottom quarks
ghtt_p	Pseudoscalar (SM-normalized) effective Higgs coupling to top quarks
ghbb_p	Pseudoscalar (SM-normalized) effective Higgs coupling to bottom quarks

SMCS_lhc13_bb_H()

double SMCS_lhc13_bb_H

(

double

Mh

)

Interface to smcs_lhc13_bb_h()

SM cross section (in pb) of \(b\bar{b}\to H\) production at the LHC with \(\sqrt{s}=13~\mathrm{TeV}\), as a function of mass.

Parameters

Mh	mass of the SM Higgs boson (mass range \([10,3000]~\mathrm{GeV}\))

SMCS_lhc13_gg_H()

double SMCS_lhc13_gg_H

(

double

Mh

)

Interface to smcs_lhc13_gg_h()

SM cross section (in pb) of \(gg\to H\) production at the LHC with \(\sqrt{s}=13~\mathrm{TeV}\), as a function of mass.

Parameters

Mh	mass of the SM Higgs boson (mass range \([10,3000]~\mathrm{GeV}\))

SMCS_lhc13_HW()

double SMCS_lhc13_HW

(

double

Mh

)

Interface to smcs_lhc13_hw()

SM cross section (in pb) of \(HW\) production at the LHC with \(\sqrt{s}=13~\mathrm{TeV}\), as a function of mass.

Parameters

Mh	mass of the SM Higgs boson (mass range \([10,3000]~\mathrm{GeV}\))

SMCS_lhc13_HZ()

double SMCS_lhc13_HZ

(

double

Mh

)

Interface to smcs_lhc13_hz()

SM cross section (in pb) of inclusive \(HZ\) production at the LHC with \(\sqrt{s}=13~\mathrm{TeV}\), as a function of mass. Prediction is evaluated from fits toVH@NNLO-2data.

Parameters

Mh	mass of the SM Higgs boson (mass range \([10,3000]~\mathrm{GeV}\))

SMCS_lhc13_ttH()

double SMCS_lhc13_ttH

(

double

Mh

)

Interface to smcs_lhc13_tth()

SM cross section (in pb) of \(Ht\bar{t}\) production at the LHC with \(\sqrt{s}=13~\mathrm{TeV}\), as a function of mass.

Parameters

Mh	mass of the SM Higgs boson (mass range \([10,3000]~\mathrm{GeV}\))

SMCS_lhc13_vbf_H()

double SMCS_lhc13_vbf_H

(

double

Mh

)

Interface to smcs_lhc13_vbf_h()

SM cross section (in pb) of \(Hqq\) (VBF) production at the LHC with \(\sqrt{s}=13~\mathrm{TeV}\), as a function of mass.

Parameters

Mh	mass of the SM Higgs boson (mass range \([10,3000]~\mathrm{GeV}\))

SMCS_lhc7_bb_H()

double SMCS_lhc7_bb_H

(

double

Mh

)

Interface to smcs_lhc7_bb_h()

SM cross section (in pb) of \(b\bar{b}\to H\) production at the LHC with \(\sqrt{s}=7~\mathrm{TeV}\), as a function of mass.

Parameters

Mh	mass of the SM Higgs boson (mass range \([10,3000]~\mathrm{GeV}\))

SMCS_lhc7_gg_H()

double SMCS_lhc7_gg_H

(

double

Mh

)

Interface to smcs_lhc7_gg_h()

SM cross section (in pb) of \(gg\to H\) production at the LHC with \(\sqrt{s}=7~\mathrm{TeV}\), as a function of mass.

Parameters

Mh	mass of the SM Higgs boson (mass range \([10,3000]~\mathrm{GeV}\))

SMCS_lhc7_HW()

double SMCS_lhc7_HW

(

double

Mh

)

Interface to smcs_lhc7_hw()

SM cross section (in pb) of \(HW\) production at the LHC with \(\sqrt{s}=7~\mathrm{TeV}\), as a function of mass.

Parameters

Mh	mass of the SM Higgs boson (mass range \([10,3000]~\mathrm{GeV}\))

SMCS_lhc7_HZ()

double SMCS_lhc7_HZ

(

double

Mh

)

Interface to smcs_lhc7_hz()

SM cross section (in pb) of inclusive \(HZ\) production at the LHC with \(\sqrt{s}=8~\mathrm{TeV}\), as a function of mass. Prediction is evaluated from fits toVH@NNLO-2data.

Parameters

Mh	mass of the SM Higgs boson (mass range \([10,3000]~\mathrm{GeV}\))

SMCS_lhc7_ttH()

double SMCS_lhc7_ttH

(

double

Mh

)

Interface to smcs_lhc7_tth()

SM cross section (in pb) of \(Ht\bar{t}\) production at the LHC with \(\sqrt{s}=7~\mathrm{TeV}\), as a function of mass.

Parameters

Mh	mass of the SM Higgs boson (mass range \([10,3000]~\mathrm{GeV}\))

SMCS_lhc7_vbf_H()

double SMCS_lhc7_vbf_H

(

double

Mh

)

Interface to smcs_lhc7_vbf_h()

SM cross section (in pb) of \(Hqq\) (VBF) production at the LHC with \(\sqrt{s}=7~\mathrm{TeV}\), as a function of mass.

Parameters

Mh	mass of the SM Higgs boson (mass range \([10,3000]~\mathrm{GeV}\))

SMCS_lhc8_bb_H()

double SMCS_lhc8_bb_H

(

double

Mh

)

Interface to smcs_lhc8_bb_h()

SM cross section (in pb) of \(b\bar{b}\to H\) production at the LHC with \(\sqrt{s}=8~\mathrm{TeV}\), as a function of mass.

Parameters

Mh	mass of the SM Higgs boson (mass range \([10,3000]~\mathrm{GeV}\))

SMCS_lhc8_gg_H()

double SMCS_lhc8_gg_H

(

double

Mh

)

Interface to smcs_lhc8_gg_h()

SM cross section (in pb) of \(gg\to H\) production at the LHC with \(\sqrt{s}=8~\mathrm{TeV}\), as a function of mass.

Parameters

Mh	mass of the SM Higgs boson (mass range \([10,3000]~\mathrm{GeV}\))

SMCS_lhc8_HW()

double SMCS_lhc8_HW

(

double

Mh

)

Interface to smcs_lhc8_hw()

SM cross section (in pb) of \(HW\) production at the LHC with \(\sqrt{s}=8~\mathrm{TeV}\), as a function of mass.

Parameters

Mh	mass of the SM Higgs boson (mass range \([10,3000]~\mathrm{GeV}\))

SMCS_lhc8_HZ()

double SMCS_lhc8_HZ

(

double

Mh

)

Interface to smcs_lhc8_hz()

SM cross section (in pb) of inclusive \(HZ\) production at the LHC with \(\sqrt{s}=8~\mathrm{TeV}\), as a function of mass. Prediction is evaluated from fits toVH@NNLO-2data.

Parameters

Mh	mass of the SM Higgs boson (mass range \([10,3000]~\mathrm{GeV}\))

SMCS_lhc8_ttH()

double SMCS_lhc8_ttH

(

double

Mh

)

Interface to smcs_lhc8_tth()

SM cross section (in pb) of \(Ht\bar{t}\) production at the LHC with \(\sqrt{s}=8~\mathrm{TeV}\), as a function of mass.

Parameters

Mh	mass of the SM Higgs boson (mass range \([10,3000]~\mathrm{GeV}\))

SMCS_lhc8_vbf_H()

double SMCS_lhc8_vbf_H

(

double

Mh

)

Interface to smcs_lhc8_vbf_h()

SM cross section (in pb) of \(Hqq\) (VBF) production at the LHC with \(\sqrt{s}=8~\mathrm{TeV}\), as a function of mass.

Parameters

Mh	mass of the SM Higgs boson (mass range \([10,3000]~\mathrm{GeV}\))

SMCS_tev_bb_H()

double SMCS_tev_bb_H

(

double

Mh

)

Interface to smcs_tev_bb_h()

SM cross section (in pb) of \(b\bar{b}\to H\) production at the Tevatron, as a function of mass.

Parameters

Mh	mass of the SM Higgs boson (fitted mass range \([60,360]~\mathrm{GeV}\))

SMCS_tev_bg_Hb()

double SMCS_tev_bg_Hb

(

double

Mh

)

Interface to smcs_tev_bg_hb()

SM cross section (in pb) of \(bg \to Hb\) production at the Tevatron, as a function of mass.

Parameters

Mh	mass of the SM Higgs boson (fitted mass range \([60,360]~\mathrm{GeV}\))

SMCS_tev_gg_H()

double SMCS_tev_gg_H

(

double

Mh

)

Interface to smcs_tev_gg_h()

SM cross section (in pb) of \(gg\to H\) production at the Tevatron, as a function of mass.

Parameters

Mh	mass of the SM Higgs boson (fitted mass range \([60,360]~\mathrm{GeV}\))

SMCS_tev_HW()

double SMCS_tev_HW

(

double

Mh

)

Interface to smcs_tev_hw()

SM cross section (in pb) of \(HW\) production at the Tevatron, as a function of mass.

Parameters

Mh	mass of the SM Higgs boson (fitted mass range \([60,360]~\mathrm{GeV}\))

SMCS_tev_HZ()

double SMCS_tev_HZ

(

double

Mh

)

Interface to smcs_tev_hz()

SM cross section (in pb) of inclusive \(HZ\) production at the Tevatron, as a function of mass. Prediction is evaluated from fits to VH@NNLO-2 data.

Parameters

Mh	mass of the SM Higgs boson (mass range \([10,3000]~\mathrm{GeV}\))

SMCS_tev_ttH()

double SMCS_tev_ttH

(

double

Mh

)

Interface to smcs_tev_tth()

SM cross section (in pb) of \(Ht\bar{t}\) production at the Tevatron, as a function of mass.

Parameters

Mh	mass of the SM Higgs boson (fitted mass range \([60,360]~\mathrm{GeV}\))

SMCS_tev_vbf_H()

double SMCS_tev_vbf_H

(

double

Mh

)

Interface to smcs_tev_vbf_h()

SM cross section (in pb) of \(Hqq\) (VBF) production at the Tevatron, as a function of mass.

Parameters

Mh	mass of the SM Higgs boson (fitted mass range \([60,360]~\mathrm{GeV}\))

SMGamma_H()

double SMGamma_H

(

double

Mh

)

Interface to smgamma_h()

SM Higgs total decay width (in GeV) as a function of mass. Prediction is taken from the CERN Yellow Report 4 by the LHC Higgs Cross Section Working Group.

Parameters

Mh	mass of the SM Higgs boson (allowed range \([0,1000]~\mathrm{GeV}\))

SMGamma_tWpb()

double SMGamma_tWpb

(

double

mt

)

Interface to smgamma_twpb()

Decay width (in GeV) of the top quark into a W-boson and a b-quark, as a function of mass. Numbers and equation read from http://pdg.lbl.gov/2018/reviews/rpp2018-rev-top-quark.pdf, Eq. (67.1).

Parameters

mt	mass of the top quark