THDMparams['gPXd']=1.0# The coupling of the additional pseudoscalar mediator to dark matter (DM). This coupling is called $y_\chi$ in (2.5) of arXiv:1701.07427.

THDMparams['tanbeta']=1.0# The ratio of the vacuum expectation values $\tan \beta = v_2/v_1$ of the Higgs doublets $H_2$ and $H_1$, as defined in Section 2.1 of arXiv:1701.07427.

THDMparams['sinbma']=1.0# The sine of the difference of the mixing angles $\sin (\beta - \alpha)$ in the scalar potential containing only the Higgs doublets. This quantity is defined in Section 3.1 of arXiv:1701.07427.

THDMparams['lam3']=3.0# The quartic coupling of the scalar doublets $H_1$ and $H_2$. This parameter corresponds to the coefficient $\lambda_3$ in (2.1) of arXiv:1701.07427.

THDMparams['laP1']=3.0# The quartic coupling between the scalar doublets $H_1$ and the pseudoscalar $P$. This parameter corresponds to the coefficient $\lambda_{P1}$ in (2.2) of arXiv:1701.07427.

THDMparams['laP2']=3.0# The quartic coupling between the scalar doublets $H_2$ and the pseudoscalar $P$. This parameter corresponds to the coefficient $\lambda_{P2}$ in (2.2) of arXiv:1701.07427.

THDMparams['sinp']=0.35# The sine of the mixing angle $\theta$, as defined in Section 2.1 of arXiv:1701.07427.

THDMparams['MXd']=10# The mass of the fermionic DM candidate denoted by $m_\chi$ in arXiv:1701.07427.

THDMparams['mh1']=125.# The mass of the lightest scalar mass eigenstate $h$, which is identified in arXiv:1701.07427 with the Higgs-like resonance found at the LHC.

THDMparams['mh2']=1500# The mass of the heavy scalar mass eigenstate $H$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mh3']=1500# The mass of the heavy pseudoscalar mass eigenstate $A$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mhc']=1500# The mass of the charged scalar eigenstate $H^\pm$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mh4']=500# The mass of the pseudoscalar mass eigenstate $a$ that decouples for $\sin \theta = 0$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['MB']=0.0

initialGluons=False# Determines initial state to generate from. True --> top loop induced production (gluon Fusion). False --> b b~ -initiated production (b-anti-b annihilation). See Sections 5.4 and 6.5 of arXiv:1701.07427 for further details

decayChannel="monoHyy"

reweight=False# Determines whether to store alternative weights for tanb and sinp

THDMparams['gPXd']=1.0# The coupling of the additional pseudoscalar mediator to dark matter (DM). This coupling is called $y_\chi$ in (2.5) of arXiv:1701.07427.

THDMparams['tanbeta']=1.0# The ratio of the vacuum expectation values $\tan \beta = v_2/v_1$ of the Higgs doublets $H_2$ and $H_1$, as defined in Section 2.1 of arXiv:1701.07427.

THDMparams['sinbma']=1.0# The sine of the difference of the mixing angles $\sin (\beta - \alpha)$ in the scalar potential containing only the Higgs doublets. This quantity is defined in Section 3.1 of arXiv:1701.07427.

THDMparams['lam3']=3.0# The quartic coupling of the scalar doublets $H_1$ and $H_2$. This parameter corresponds to the coefficient $\lambda_3$ in (2.1) of arXiv:1701.07427.

THDMparams['laP1']=3.0# The quartic coupling between the scalar doublets $H_1$ and the pseudoscalar $P$. This parameter corresponds to the coefficient $\lambda_{P1}$ in (2.2) of arXiv:1701.07427.

THDMparams['laP2']=3.0# The quartic coupling between the scalar doublets $H_2$ and the pseudoscalar $P$. This parameter corresponds to the coefficient $\lambda_{P2}$ in (2.2) of arXiv:1701.07427.

THDMparams['sinp']=0.35# The sine of the mixing angle $\theta$, as defined in Section 2.1 of arXiv:1701.07427.

THDMparams['MXd']=10# The mass of the fermionic DM candidate denoted by $m_\chi$ in arXiv:1701.07427.

THDMparams['mh1']=125.# The mass of the lightest scalar mass eigenstate $h$, which is identified in arXiv:1701.07427 with the Higgs-like resonance found at the LHC.

THDMparams['mh2']=1500# The mass of the heavy scalar mass eigenstate $H$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mh3']=1500# The mass of the heavy pseudoscalar mass eigenstate $A$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mhc']=1500# The mass of the charged scalar eigenstate $H^\pm$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mh4']=500# The mass of the pseudoscalar mass eigenstate $a$ that decouples for $\sin \theta = 0$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['MB']=4.7

initialGluons=True# Determines initial state to generate from. True --> top loop induced production (gluon Fusion). False --> b b~ -initiated production (b-anti-b annihilation). See Sections 5.4 and 6.5 of arXiv:1701.07427 for further details

decayChannel="monoHyy"

reweight=False# Determines whether to store alternative weights for tanb and sinp

THDMparams['gPXd']=1.0# The coupling of the additional pseudoscalar mediator to dark matter (DM). This coupling is called $y_\chi$ in (2.5) of arXiv:1701.07427.

THDMparams['tanbeta']=5.0# The ratio of the vacuum expectation values $\tan \beta = v_2/v_1$ of the Higgs doublets $H_2$ and $H_1$, as defined in Section 2.1 of arXiv:1701.07427.

THDMparams['sinbma']=1.0# The sine of the difference of the mixing angles $\sin (\beta - \alpha)$ in the scalar potential containing only the Higgs doublets. This quantity is defined in Section 3.1 of arXiv:1701.07427.

THDMparams['lam3']=3.0# The quartic coupling of the scalar doublets $H_1$ and $H_2$. This parameter corresponds to the coefficient $\lambda_3$ in (2.1) of arXiv:1701.07427.

THDMparams['laP1']=3.0# The quartic coupling between the scalar doublets $H_1$ and the pseudoscalar $P$. This parameter corresponds to the coefficient $\lambda_{P1}$ in (2.2) of arXiv:1701.07427.

THDMparams['laP2']=3.0# The quartic coupling between the scalar doublets $H_2$ and the pseudoscalar $P$. This parameter corresponds to the coefficient $\lambda_{P2}$ in (2.2) of arXiv:1701.07427.

THDMparams['sinp']=0.35# The sine of the mixing angle $\theta$, as defined in Section 2.1 of arXiv:1701.07427.

THDMparams['MXd']=10# The mass of the fermionic DM candidate denoted by $m_\chi$ in arXiv:1701.07427.

THDMparams['mh1']=125.# The mass of the lightest scalar mass eigenstate $h$, which is identified in arXiv:1701.07427 with the Higgs-like resonance found at the LHC.

THDMparams['mh2']=1500# The mass of the heavy scalar mass eigenstate $H$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mh3']=1500# The mass of the heavy pseudoscalar mass eigenstate $A$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mhc']=1500# The mass of the charged scalar eigenstate $H^\pm$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mh4']=500# The mass of the pseudoscalar mass eigenstate $a$ that decouples for $\sin \theta = 0$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['MB']=0.0

initialGluons=False# Determines initial state to generate from. True --> top loop induced production (gluon Fusion). False --> b b~ -initiated production (b-anti-b annihilation). See Sections 5.4 and 6.5 of arXiv:1701.07427 for further details

decayChannel="monoHyy"

reweight=False# Determines whether to store alternative weights for tanb and sinp

THDMparams['gPXd']=1.0# The coupling of the additional pseudoscalar mediator to dark matter (DM). This coupling is called $y_\chi$ in (2.5) of arXiv:1701.07427.

THDMparams['tanbeta']=5.0# The ratio of the vacuum expectation values $\tan \beta = v_2/v_1$ of the Higgs doublets $H_2$ and $H_1$, as defined in Section 2.1 of arXiv:1701.07427.

THDMparams['sinbma']=1.0# The sine of the difference of the mixing angles $\sin (\beta - \alpha)$ in the scalar potential containing only the Higgs doublets. This quantity is defined in Section 3.1 of arXiv:1701.07427.

THDMparams['lam3']=3.0# The quartic coupling of the scalar doublets $H_1$ and $H_2$. This parameter corresponds to the coefficient $\lambda_3$ in (2.1) of arXiv:1701.07427.

THDMparams['laP1']=3.0# The quartic coupling between the scalar doublets $H_1$ and the pseudoscalar $P$. This parameter corresponds to the coefficient $\lambda_{P1}$ in (2.2) of arXiv:1701.07427.

THDMparams['laP2']=3.0# The quartic coupling between the scalar doublets $H_2$ and the pseudoscalar $P$. This parameter corresponds to the coefficient $\lambda_{P2}$ in (2.2) of arXiv:1701.07427.

THDMparams['sinp']=0.35# The sine of the mixing angle $\theta$, as defined in Section 2.1 of arXiv:1701.07427.

THDMparams['MXd']=10# The mass of the fermionic DM candidate denoted by $m_\chi$ in arXiv:1701.07427.

THDMparams['mh1']=125.# The mass of the lightest scalar mass eigenstate $h$, which is identified in arXiv:1701.07427 with the Higgs-like resonance found at the LHC.

THDMparams['mh2']=1500# The mass of the heavy scalar mass eigenstate $H$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mh3']=1500# The mass of the heavy pseudoscalar mass eigenstate $A$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mhc']=1500# The mass of the charged scalar eigenstate $H^\pm$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mh4']=500# The mass of the pseudoscalar mass eigenstate $a$ that decouples for $\sin \theta = 0$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['MB']=4.7

initialGluons=True# Determines initial state to generate from. True --> top loop induced production (gluon Fusion). False --> b b~ -initiated production (b-anti-b annihilation). See Sections 5.4 and 6.5 of arXiv:1701.07427 for further details

decayChannel="monoHyy"

reweight=False# Determines whether to store alternative weights for tanb and sinp

THDMparams['gPXd']=1.0# The coupling of the additional pseudoscalar mediator to dark matter (DM). This coupling is called $y_\chi$ in (2.5) of arXiv:1701.07427.

THDMparams['tanbeta']=1.0# The ratio of the vacuum expectation values $\tan \beta = v_2/v_1$ of the Higgs doublets $H_2$ and $H_1$, as defined in Section 2.1 of arXiv:1701.07427.

THDMparams['sinbma']=1.0# The sine of the difference of the mixing angles $\sin (\beta - \alpha)$ in the scalar potential containing only the Higgs doublets. This quantity is defined in Section 3.1 of arXiv:1701.07427.

THDMparams['lam3']=3.0# The quartic coupling of the scalar doublets $H_1$ and $H_2$. This parameter corresponds to the coefficient $\lambda_3$ in (2.1) of arXiv:1701.07427.

THDMparams['laP1']=3.0# The quartic coupling between the scalar doublets $H_1$ and the pseudoscalar $P$. This parameter corresponds to the coefficient $\lambda_{P1}$ in (2.2) of arXiv:1701.07427.

THDMparams['laP2']=3.0# The quartic coupling between the scalar doublets $H_2$ and the pseudoscalar $P$. This parameter corresponds to the coefficient $\lambda_{P2}$ in (2.2) of arXiv:1701.07427.

THDMparams['sinp']=0.35# The sine of the mixing angle $\theta$, as defined in Section 2.1 of arXiv:1701.07427.

THDMparams['MXd']=10# The mass of the fermionic DM candidate denoted by $m_\chi$ in arXiv:1701.07427.

THDMparams['mh1']=125.# The mass of the lightest scalar mass eigenstate $h$, which is identified in arXiv:1701.07427 with the Higgs-like resonance found at the LHC.

THDMparams['mh2']=200# The mass of the heavy scalar mass eigenstate $H$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mh3']=200# The mass of the heavy pseudoscalar mass eigenstate $A$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mhc']=200# The mass of the charged scalar eigenstate $H^\pm$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mh4']=100# The mass of the pseudoscalar mass eigenstate $a$ that decouples for $\sin \theta = 0$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['MB']=0.0

initialGluons=False# Determines initial state to generate from. True --> top loop induced production (gluon Fusion). False --> b b~ -initiated production (b-anti-b annihilation). See Sections 5.4 and 6.5 of arXiv:1701.07427 for further details

decayChannel="monoHyy"

reweight=False# Determines whether to store alternative weights for tanb and sinp

THDMparams['gPXd']=1.0# The coupling of the additional pseudoscalar mediator to dark matter (DM). This coupling is called $y_\chi$ in (2.5) of arXiv:1701.07427.

THDMparams['tanbeta']=1.0# The ratio of the vacuum expectation values $\tan \beta = v_2/v_1$ of the Higgs doublets $H_2$ and $H_1$, as defined in Section 2.1 of arXiv:1701.07427.

THDMparams['sinbma']=1.0# The sine of the difference of the mixing angles $\sin (\beta - \alpha)$ in the scalar potential containing only the Higgs doublets. This quantity is defined in Section 3.1 of arXiv:1701.07427.

THDMparams['lam3']=3.0# The quartic coupling of the scalar doublets $H_1$ and $H_2$. This parameter corresponds to the coefficient $\lambda_3$ in (2.1) of arXiv:1701.07427.

THDMparams['laP1']=3.0# The quartic coupling between the scalar doublets $H_1$ and the pseudoscalar $P$. This parameter corresponds to the coefficient $\lambda_{P1}$ in (2.2) of arXiv:1701.07427.

THDMparams['laP2']=3.0# The quartic coupling between the scalar doublets $H_2$ and the pseudoscalar $P$. This parameter corresponds to the coefficient $\lambda_{P2}$ in (2.2) of arXiv:1701.07427.

THDMparams['sinp']=0.35# The sine of the mixing angle $\theta$, as defined in Section 2.1 of arXiv:1701.07427.

THDMparams['MXd']=10# The mass of the fermionic DM candidate denoted by $m_\chi$ in arXiv:1701.07427.

THDMparams['mh1']=125.# The mass of the lightest scalar mass eigenstate $h$, which is identified in arXiv:1701.07427 with the Higgs-like resonance found at the LHC.

THDMparams['mh2']=200# The mass of the heavy scalar mass eigenstate $H$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mh3']=200# The mass of the heavy pseudoscalar mass eigenstate $A$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mhc']=200# The mass of the charged scalar eigenstate $H^\pm$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mh4']=100# The mass of the pseudoscalar mass eigenstate $a$ that decouples for $\sin \theta = 0$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['MB']=4.7

initialGluons=True# Determines initial state to generate from. True --> top loop induced production (gluon Fusion). False --> b b~ -initiated production (b-anti-b annihilation). See Sections 5.4 and 6.5 of arXiv:1701.07427 for further details

decayChannel="monoHyy"

reweight=False# Determines whether to store alternative weights for tanb and sinp

THDMparams['gPXd']=1.0# The coupling of the additional pseudoscalar mediator to dark matter (DM). This coupling is called $y_\chi$ in (2.5) of arXiv:1701.07427.

THDMparams['tanbeta']=1.0# The ratio of the vacuum expectation values $\tan \beta = v_2/v_1$ of the Higgs doublets $H_2$ and $H_1$, as defined in Section 2.1 of arXiv:1701.07427.

THDMparams['sinbma']=1.0# The sine of the difference of the mixing angles $\sin (\beta - \alpha)$ in the scalar potential containing only the Higgs doublets. This quantity is defined in Section 3.1 of arXiv:1701.07427.

THDMparams['lam3']=3.0# The quartic coupling of the scalar doublets $H_1$ and $H_2$. This parameter corresponds to the coefficient $\lambda_3$ in (2.1) of arXiv:1701.07427.

THDMparams['laP1']=3.0# The quartic coupling between the scalar doublets $H_1$ and the pseudoscalar $P$. This parameter corresponds to the coefficient $\lambda_{P1}$ in (2.2) of arXiv:1701.07427.

THDMparams['laP2']=3.0# The quartic coupling between the scalar doublets $H_2$ and the pseudoscalar $P$. This parameter corresponds to the coefficient $\lambda_{P2}$ in (2.2) of arXiv:1701.07427.

THDMparams['sinp']=0.35# The sine of the mixing angle $\theta$, as defined in Section 2.1 of arXiv:1701.07427.

THDMparams['MXd']=10# The mass of the fermionic DM candidate denoted by $m_\chi$ in arXiv:1701.07427.

THDMparams['mh1']=125.# The mass of the lightest scalar mass eigenstate $h$, which is identified in arXiv:1701.07427 with the Higgs-like resonance found at the LHC.

THDMparams['mh2']=200# The mass of the heavy scalar mass eigenstate $H$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mh3']=200# The mass of the heavy pseudoscalar mass eigenstate $A$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mhc']=200# The mass of the charged scalar eigenstate $H^\pm$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mh4']=300# The mass of the pseudoscalar mass eigenstate $a$ that decouples for $\sin \theta = 0$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['MB']=0.0

initialGluons=False# Determines initial state to generate from. True --> top loop induced production (gluon Fusion). False --> b b~ -initiated production (b-anti-b annihilation). See Sections 5.4 and 6.5 of arXiv:1701.07427 for further details

decayChannel="monoHyy"

reweight=False# Determines whether to store alternative weights for tanb and sinp

THDMparams['gPXd']=1.0# The coupling of the additional pseudoscalar mediator to dark matter (DM). This coupling is called $y_\chi$ in (2.5) of arXiv:1701.07427.

THDMparams['tanbeta']=1.0# The ratio of the vacuum expectation values $\tan \beta = v_2/v_1$ of the Higgs doublets $H_2$ and $H_1$, as defined in Section 2.1 of arXiv:1701.07427.

THDMparams['sinbma']=1.0# The sine of the difference of the mixing angles $\sin (\beta - \alpha)$ in the scalar potential containing only the Higgs doublets. This quantity is defined in Section 3.1 of arXiv:1701.07427.

THDMparams['lam3']=3.0# The quartic coupling of the scalar doublets $H_1$ and $H_2$. This parameter corresponds to the coefficient $\lambda_3$ in (2.1) of arXiv:1701.07427.

THDMparams['laP1']=3.0# The quartic coupling between the scalar doublets $H_1$ and the pseudoscalar $P$. This parameter corresponds to the coefficient $\lambda_{P1}$ in (2.2) of arXiv:1701.07427.

THDMparams['laP2']=3.0# The quartic coupling between the scalar doublets $H_2$ and the pseudoscalar $P$. This parameter corresponds to the coefficient $\lambda_{P2}$ in (2.2) of arXiv:1701.07427.

THDMparams['sinp']=0.35# The sine of the mixing angle $\theta$, as defined in Section 2.1 of arXiv:1701.07427.

THDMparams['MXd']=10# The mass of the fermionic DM candidate denoted by $m_\chi$ in arXiv:1701.07427.

THDMparams['mh1']=125.# The mass of the lightest scalar mass eigenstate $h$, which is identified in arXiv:1701.07427 with the Higgs-like resonance found at the LHC.

THDMparams['mh2']=200# The mass of the heavy scalar mass eigenstate $H$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mh3']=200# The mass of the heavy pseudoscalar mass eigenstate $A$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mhc']=200# The mass of the charged scalar eigenstate $H^\pm$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mh4']=300# The mass of the pseudoscalar mass eigenstate $a$ that decouples for $\sin \theta = 0$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['MB']=4.7

initialGluons=True# Determines initial state to generate from. True --> top loop induced production (gluon Fusion). False --> b b~ -initiated production (b-anti-b annihilation). See Sections 5.4 and 6.5 of arXiv:1701.07427 for further details

decayChannel="monoHyy"

reweight=False# Determines whether to store alternative weights for tanb and sinp

THDMparams['gPXd']=1.0# The coupling of the additional pseudoscalar mediator to dark matter (DM). This coupling is called $y_\chi$ in (2.5) of arXiv:1701.07427.

THDMparams['tanbeta']=1.0# The ratio of the vacuum expectation values $\tan \beta = v_2/v_1$ of the Higgs doublets $H_2$ and $H_1$, as defined in Section 2.1 of arXiv:1701.07427.

THDMparams['sinbma']=1.0# The sine of the difference of the mixing angles $\sin (\beta - \alpha)$ in the scalar potential containing only the Higgs doublets. This quantity is defined in Section 3.1 of arXiv:1701.07427.

THDMparams['lam3']=3.0# The quartic coupling of the scalar doublets $H_1$ and $H_2$. This parameter corresponds to the coefficient $\lambda_3$ in (2.1) of arXiv:1701.07427.

THDMparams['laP1']=3.0# The quartic coupling between the scalar doublets $H_1$ and the pseudoscalar $P$. This parameter corresponds to the coefficient $\lambda_{P1}$ in (2.2) of arXiv:1701.07427.

THDMparams['laP2']=3.0# The quartic coupling between the scalar doublets $H_2$ and the pseudoscalar $P$. This parameter corresponds to the coefficient $\lambda_{P2}$ in (2.2) of arXiv:1701.07427.

THDMparams['sinp']=0.35# The sine of the mixing angle $\theta$, as defined in Section 2.1 of arXiv:1701.07427.

THDMparams['MXd']=10# The mass of the fermionic DM candidate denoted by $m_\chi$ in arXiv:1701.07427.

THDMparams['mh1']=125.# The mass of the lightest scalar mass eigenstate $h$, which is identified in arXiv:1701.07427 with the Higgs-like resonance found at the LHC.

THDMparams['mh2']=200# The mass of the heavy scalar mass eigenstate $H$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mh3']=200# The mass of the heavy pseudoscalar mass eigenstate $A$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mhc']=200# The mass of the charged scalar eigenstate $H^\pm$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mh4']=500# The mass of the pseudoscalar mass eigenstate $a$ that decouples for $\sin \theta = 0$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['MB']=0.0

initialGluons=False# Determines initial state to generate from. True --> top loop induced production (gluon Fusion). False --> b b~ -initiated production (b-anti-b annihilation). See Sections 5.4 and 6.5 of arXiv:1701.07427 for further details

decayChannel="monoHyy"

reweight=False# Determines whether to store alternative weights for tanb and sinp

THDMparams['gPXd']=1.0# The coupling of the additional pseudoscalar mediator to dark matter (DM). This coupling is called $y_\chi$ in (2.5) of arXiv:1701.07427.

THDMparams['tanbeta']=1.0# The ratio of the vacuum expectation values $\tan \beta = v_2/v_1$ of the Higgs doublets $H_2$ and $H_1$, as defined in Section 2.1 of arXiv:1701.07427.

THDMparams['sinbma']=1.0# The sine of the difference of the mixing angles $\sin (\beta - \alpha)$ in the scalar potential containing only the Higgs doublets. This quantity is defined in Section 3.1 of arXiv:1701.07427.

THDMparams['lam3']=3.0# The quartic coupling of the scalar doublets $H_1$ and $H_2$. This parameter corresponds to the coefficient $\lambda_3$ in (2.1) of arXiv:1701.07427.

THDMparams['laP1']=3.0# The quartic coupling between the scalar doublets $H_1$ and the pseudoscalar $P$. This parameter corresponds to the coefficient $\lambda_{P1}$ in (2.2) of arXiv:1701.07427.

THDMparams['laP2']=3.0# The quartic coupling between the scalar doublets $H_2$ and the pseudoscalar $P$. This parameter corresponds to the coefficient $\lambda_{P2}$ in (2.2) of arXiv:1701.07427.

THDMparams['sinp']=0.35# The sine of the mixing angle $\theta$, as defined in Section 2.1 of arXiv:1701.07427.

THDMparams['MXd']=10# The mass of the fermionic DM candidate denoted by $m_\chi$ in arXiv:1701.07427.

THDMparams['mh1']=125.# The mass of the lightest scalar mass eigenstate $h$, which is identified in arXiv:1701.07427 with the Higgs-like resonance found at the LHC.

THDMparams['mh2']=200# The mass of the heavy scalar mass eigenstate $H$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mh3']=200# The mass of the heavy pseudoscalar mass eigenstate $A$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mhc']=200# The mass of the charged scalar eigenstate $H^\pm$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mh4']=500# The mass of the pseudoscalar mass eigenstate $a$ that decouples for $\sin \theta = 0$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['MB']=4.7

initialGluons=True# Determines initial state to generate from. True --> top loop induced production (gluon Fusion). False --> b b~ -initiated production (b-anti-b annihilation). See Sections 5.4 and 6.5 of arXiv:1701.07427 for further details

decayChannel="monoHyy"

reweight=False# Determines whether to store alternative weights for tanb and sinp

THDMparams['gPXd']=1.0# The coupling of the additional pseudoscalar mediator to dark matter (DM). This coupling is called $y_\chi$ in (2.5) of arXiv:1701.07427.

THDMparams['tanbeta']=1.0# The ratio of the vacuum expectation values $\tan \beta = v_2/v_1$ of the Higgs doublets $H_2$ and $H_1$, as defined in Section 2.1 of arXiv:1701.07427.

THDMparams['sinbma']=1.0# The sine of the difference of the mixing angles $\sin (\beta - \alpha)$ in the scalar potential containing only the Higgs doublets. This quantity is defined in Section 3.1 of arXiv:1701.07427.

THDMparams['lam3']=3.0# The quartic coupling of the scalar doublets $H_1$ and $H_2$. This parameter corresponds to the coefficient $\lambda_3$ in (2.1) of arXiv:1701.07427.

THDMparams['laP1']=3.0# The quartic coupling between the scalar doublets $H_1$ and the pseudoscalar $P$. This parameter corresponds to the coefficient $\lambda_{P1}$ in (2.2) of arXiv:1701.07427.

THDMparams['laP2']=3.0# The quartic coupling between the scalar doublets $H_2$ and the pseudoscalar $P$. This parameter corresponds to the coefficient $\lambda_{P2}$ in (2.2) of arXiv:1701.07427.

THDMparams['sinp']=0.35# The sine of the mixing angle $\theta$, as defined in Section 2.1 of arXiv:1701.07427.

THDMparams['MXd']=10# The mass of the fermionic DM candidate denoted by $m_\chi$ in arXiv:1701.07427.

THDMparams['mh1']=125.# The mass of the lightest scalar mass eigenstate $h$, which is identified in arXiv:1701.07427 with the Higgs-like resonance found at the LHC.

THDMparams['mh2']=600# The mass of the heavy scalar mass eigenstate $H$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mh3']=600# The mass of the heavy pseudoscalar mass eigenstate $A$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mhc']=600# The mass of the charged scalar eigenstate $H^\pm$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['mh4']=100# The mass of the pseudoscalar mass eigenstate $a$ that decouples for $\sin \theta = 0$. See Section 2.1 of arXiv:1701.07427 for further details.

THDMparams['MB']=0.0

initialGluons=False# Determines initial state to generate from. True --> top loop induced production (gluon Fusion). False --> b b~ -initiated production (b-anti-b annihilation). See Sections 5.4 and 6.5 of arXiv:1701.07427 for further details

decayChannel="monoHyy"

reweight=False# Determines whether to store alternative weights for tanb and sinp

THDMparams['gPXd']=1.0# The coupling of the additional pseudoscalar mediator to dark matter (DM). This coupling is called $y_\chi$ in (2.5) of arXiv:1701.07427.

THDMparams['tanbeta']=1.0# The ratio of the vacuum expectation values $\tan \beta = v_2/v_1$ of the Higgs doublets $H_2$ and $H_1$, as defined in Section 2.1 of arXiv:1701.07427.

THDMparams['sinbma']=1.0# The sine of the difference of the mixing angles $\sin (\beta - \alpha)$ in the scalar potential containing only the Higgs doublets. This quantity is defined in Section 3.1 of arXiv:1701.07427.

THDMparams['lam3']=3.0# The quartic coupling of the scalar doublets $H_1$ and $H_2$. This parameter corresponds to the coefficient $\lambda_3$ in (2.1) of arXiv:1701.07427.

THDMparams['laP1']=3.0# The quartic coupling between the scalar doublets $H_1$ and the pseudoscalar $P$. This parameter corresponds to the coefficient $\lambda_{P1}$ in (2.2) of arXiv:1701.07427.

THDMparams['laP2']=3.0# The quartic coupling between the scalar doublets $H_2$ and the pseudoscalar $P$. This parameter corresponds to the coefficient $\lambda_{P2}$ in (2.2) of arXiv:1701.07427.