ATLMCPROD-8003

common/MadGraph/MadGraphControl_Pythia8EvtGen_A14NNPDF30LO_Pseudoscalar_2HDMa_monoH.py

+from MadGraphControl.MadGraphUtils import *
+
+fcard = open('proc_card_mg5.dat', 'w')
+
+# This control file makes use of UFO v2, registered in https://its.cern.ch/jira/browse/AGENE-1652 
+
+# Z's don't contribute because sinbma (sin(beta-alpha)) is 1.0, so excluding them with '/z' reduces runtime for the LHE generation,
+# without changing the physics/cross-sections/kinematic ditributions
+
+# Process definition
+if initialGluons:
+    # For the gluon-gluon fusion production use the 4FS to take into account the b-quark loops
+    fcard.write("""
+    import model Pseudoscalar_2HDM -modelname
+    define p = g d u s c d~ u~ s~ c~
+    define j = g d u s c d~ u~ s~ c~
+    """)
+    fcard.write("generate g g > h1 xd xd~ / z [QCD]\n")
+else:
+    # For b-initiated production use 5FS
+    fcard.write("""
+    import model Pseudoscalar_2HDM-bbMET_5FS -modelname
+    define p = g d u s c b d~ u~ s~ c~ b~
+    define j = g d u s c b d~ u~ s~ c~ b~
+    """)    
+    fcard.write("generate p p > h1 xd xd~ / z\n")
+fcard.write("""
+output -f
+""")
+fcard.close()
+
+beamEnergy=-999
+if hasattr(runArgs,'ecmEnergy'):
+  beamEnergy = runArgs.ecmEnergy / 2.
+else: 
+  raise RuntimeError("No center of mass energy found.")
+
+process_dir = new_process()
+
+# Build run_card
+extras = {}
+if initialGluons:
+    extras = {
+        'pdlabel'       : "'lhapdf'",
+        'lhaid'         : '260000',
+        'maxjetflavor'  : 4,
+        'asrwgtflavor'  : 4,
+        'lhe_version': '3.0',
+        'cut_decays': 'F',
+        'use_syst': 'True',
+	     'sys_pdf': 'NNPDF30_nlo_as_0118'
+    }
+else:
+    extras = {
+        'pdlabel'       : "'lhapdf'",
+        'lhaid'         : '260000',
+        'maxjetflavor'  : 5,
+        'asrwgtflavor'  : 5,
+        'lhe_version': '3.0',
+        'cut_decays': 'F',
+        'use_syst': 'True',
+	     'sys_pdf': 'NNPDF30_nlo_as_0118'
+    }
+
+qcut = 0 # for consistency with iCKKW=0
+
+# Number of events to generate
+nevents=5000
+multiplier=2 # to take into account ~50% filter efficiency + safety margin (perhaps can be fine-tuned further)
+if decayChannel is "monoHtautau": multiplier=30
+
+if runArgs.maxEvents>0:
+    nevents = runArgs.maxEvents * multiplier
+else:
+    nevents *= multiplier
+    
+# Run card
+build_run_card(run_card_old=get_default_runcard(process_dir),run_card_new='run_card.dat', xqcut = qcut,
+               nevts=nevents,rand_seed=runArgs.randomSeed,beamEnergy=beamEnergy,extras=extras)
+
+print_cards()
+
+# Build param_card.dat
+paramcard = subprocess.Popen(['get_files','-data','MadGraph_param_card_Pseudoscalar2HDM.dat'])
+paramcard.wait()
+if not os.access('MadGraph_param_card_Pseudoscalar2HDM.dat',os.R_OK):
+    print 'ERROR: Could not get param card'
+elif os.access('param_card.dat',os.R_OK):
+    print 'ERROR: Old param card in the current directory.  Dont want to clobber it.  Please move it first.'
+else:
+    oldcard = open('MadGraph_param_card_Pseudoscalar2HDM.dat','r')
+    newcard = open('param_card.dat','w')
+    import re
+    THDM_regexp = re.compile('\s+([0-9]+)\s+([0-9+-.e]+)\s+#\s+(\w+)\s*')
+    for line in oldcard:
+        isTHDMparam = False
+        for param_name, newvalue in THDMparams.items():
+          if param_name in line and "NUMBERS" not in line: # protect against picking up lines with "NUMBERS" when changing bottom quark mass "MB"
+            THDM_match = THDM_regexp.match(line.rstrip('\n'))
+            if THDM_match:
+              THDM_pdgID = int(THDM_match.group(1))
+              THDM_oldvalue = float(THDM_match.group(2))
+              THDM_param_name = str(THDM_match.group(3))
+              if THDM_param_name != param_name:
+                print param_name, THDM_param_name
+                raise RuntimeError('Mismatching parameter names, please double-check logic')
+              newcard.write('     %d %s # %s\n' % (THDM_pdgID, str(newvalue), THDM_param_name))
+              isTHDMparam = True
+            else:
+              print line.rstrip('\n')
+              raise RuntimeError('Unable to parse line')
+        if not isTHDMparam:
+          newcard.write(line)
+    oldcard.close()
+    newcard.close()
+
+runName='run_01'
+
+if initialGluons:
+    # Hack for copying MadLoop card in PROC directory. Needed for MG 2.6 which is affected by this bug
+    from shutil import copyfile
+    copyfile(os.environ['MADPATH']+'/Template/loop_material/StandAlone/Cards/MadLoopParams.dat',process_dir+'/Cards/MadLoopParams_default.dat')
+    if os.path.isfile(process_dir+'/Cards/MadLoopParams_default.dat'):
+        print "MadLoopParams_default.dat copied"
+    else:
+        raise RunTimeError("MadLopParams_default.dat not found")
+    
+    # Another hack for making IREGI compile
+    os.environ['FC'] = "gfortran"
+
+if reweight:
+  # Create reweighting card
+  reweight_card_path = os.getcwd()+'/reweight_card.dat'
+  reweight_card_loc='reweight_card.dat'
+  rwcard = open(reweight_card_loc,'w')
+
+  for rw_name in reweights:
+    rwcard.write("launch --rwgt_name=%s\n" % rw_name)
+    for param in rw_name.split('-'):
+      param_name, value = param.split('_')
+      if param_name == "SINP":
+        rwcard.write("set Higgs 5  %s\n" % value)
+      elif param_name == "TANB":
+        rwcard.write("set FRBlock 2  %s\n" % value)
+    rwcard.write("set decay 25 Auto\nset decay 35 Auto\nset decay 36 Auto\nset decay 37 Auto\nset decay 55 Auto\n") 
+  rwcard.write("launch --rwgt_name=no_reweight") #dummy weight
+  rwcard.close()
+    
+# Generate the events    
+if reweight:
+    generate(run_card_loc='run_card.dat',param_card_loc='param_card.dat',mode=0,njobs=1,run_name=runName,proc_dir=process_dir,reweight_card_loc=reweight_card_path)
+else:
+    generate(run_card_loc='run_card.dat',param_card_loc='param_card.dat',mode=0,njobs=1,run_name=runName,proc_dir=process_dir)
+arrange_output(run_name=runName,proc_dir=process_dir,outputDS=runName+'._00001.events.tar.gz',lhe_version=3,saveProcDir=True)                                                                         
+                                                                                                                                                                       
+# Metadata                                                                                                                                                          
+if initialGluons:
+    evgenConfig.process = "g g > xd xd~ h1"
+    initialStateString = "gluon fusion"
+else:
+    evgenConfig.process = "p p > xd xd~ h1"
+    initialStateString = "b quark annihilation"
+
+if decayChannel is "monoHyy":
+   evgenConfig.description = "Pseudoscalar Mediator simplified Model for mono-Higgs(-> gamma gamma) " +initialStateString + " initiated process  \
+   with tan(beta) = " + str(THDMparams['tanbeta']) + ", sin(theta) = " + str(THDMparams['sinp']) + ", mA = " + str(THDMparams['mh3']) + ", ma"\
+    + str(THDMparams['mh4'])
+   evgenConfig.keywords = ["exotic","BSMHiggs","Higgs","WIMP", "simplifiedModel"]
+   evgenConfig.contact = ["Kristian Bjoerke <kristian.bjoerke@cern.ch>"]
+
+if decayChannel is "monoHbb":
+   evgenConfig.description = "Pseudoscalar Mediator simplified Model for mono-Higgs(-> b bbar) " +initialStateString + " initiated process  \
+   with tan(beta) = " + str(THDMparams['tanbeta']) + ", sin(theta) = " + str(THDMparams['sinp']) + ", mA = " + str(THDMparams['mh3']) + ", ma"\
+    + str(THDMparams['mh4'])
+   evgenConfig.keywords = ["exotic","BSMHiggs","Higgs","WIMP", "simplifiedModel","bbbar"]
+   evgenConfig.contact = ["Spyros Argyropoulos <spyridon.argyropoulos@cern.ch>, Chen Zhou <chen.zhou@cern.ch>"]
+
+if decayChannel is "monoHtautau":
+   evgenConfig.description = "Pseudoscalar Mediator simplified Model for mono-Higgs(-> tau tau) " +initialStateString + " initiated process  \
+   with tan(beta) = " + str(THDMparams['tanbeta']) + ", sin(theta) = " + str(THDMparams['sinp']) + ", mA = " + str(THDMparams['mh3']) + ", ma"\
+ + str(THDMparams['mh4'])
+   evgenConfig.keywords = ["exotic","BSMHiggs","Higgs","WIMP", "simplifiedModel"]
+   evgenConfig.contact = ["Julia Djuvsland <julia.djuvsland@cern.ch>"]
+
+evgenConfig.inputfilecheck = runName                                                                                                                                   
+runArgs.inputGeneratorFile=runName+'._00001.events.tar.gz'                                                                                                             
+# Shower includes
+include("MC15JobOptions/Pythia8_A14_NNPDF23LO_EvtGen_Common.py")
+include("MC15JobOptions/Pythia8_MadGraph.py")
+
+# Teach pythia about the dark matter particle
+genSeq.Pythia8.Commands += ["SLHA:allowUserOverride = on",
+                            "1000022:all = xd xd~ 2 0 0 %d 0.0 0.0 0.0 0.0" % (int(THDMparams['MXd'])),
+                            "1000022:isVisible = false",
+			                   "1000022:mayDecay = off"
+                            ]
+
+if decayChannel is "monoHyy":
+   # Force h->gamgam decay in Pythia
+   genSeq.Pythia8.Commands += ["25:oneChannel = on 1.0 100 22 22 "]
+
+   # Generator filter
+   if not hasattr( filtSeq, "DiPhotonFilter" ):
+       from GeneratorFilters.GeneratorFiltersConf import DiPhotonFilter
+       filtSeq += DiPhotonFilter ()
+   
+   DiPhotonFilter = filtSeq.DiPhotonFilter
+   DiPhotonFilter.PtCut1st = 30000.
+   DiPhotonFilter.PtCut2nd = 20000.
+
+if decayChannel is "monoHbb":
+   # Force h->bb decay in Pythia
+   genSeq.Pythia8.Commands += ["25:oneChannel = on 1.0 100 5 -5 "]
+   
+   # Generator filter
+   include("MC15JobOptions/MissingEtFilter.py")
+   filtSeq.MissingEtFilter.METCut = 50*GeV
+   filtSeq.MissingEtFilter.UseNeutrinosFromHadrons = True
+
+if decayChannel is "monoHtautau":
+    # Force h->tautau decay in Pythia
+    genSeq.Pythia8.Commands += ["25:oneChannel = on 1.0 100 15 -15 "]
+
+    # Generator filter
+    include("MC15JobOptions/MissingEtFilter.py")
+    filtSeq.MissingEtFilter.METCut = 100*GeV
+    filtSeq.MissingEtFilter.UseNeutrinosFromHadrons = True
+        
+    include('MC15JobOptions/MultiElecMuTauFilter.py')
+    MultiElecMuTauFilter = filtSeq.MultiElecMuTauFilter
+    MultiElecMuTauFilter.NLeptons = 2
+    MultiElecMuTauFilter.MinPt = 1e10
+    MultiElecMuTauFilter.MaxEta = 2.8
+    MultiElecMuTauFilter.MinVisPtHadTau =  12000
+    MultiElecMuTauFilter.IncludeHadTaus = 1
+
+    filtSeq.Expression = "MultiElecMuTauFilter and MissingEtFilter"  
+    

share/DSID312xxx/MC15.312662.MGPy8EG_A14N30LO_2HDMa_bb_monoHyy_tb1_sp035_mA1500_ma500.py

+THDMparams = {}
+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
+Reweight = {}
+Reweight['tanbeta'] = "scan:[0.3, 1, 5, 10, 20]"
+Reweight['sinp'] = "scan:[0.1, 0.35, 0.7, 0.9]"
+
+include("MadGraphControl_Pythia8EvtGen_A14NNPDF30LO_Pseudoscalar_2HDMa_monoH.py")

share/DSID312xxx/MC15.312663.MGPy8EG_A14N30LO_2HDMa_ggF_monoHyy_tb1_sp035_mA1500_ma500.py

+THDMparams = {}
+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
+Reweight = {}
+Reweight['tanbeta'] = "scan:[0.3, 1, 5, 10, 20]"
+Reweight['sinp'] = "scan:[0.1, 0.35, 0.7, 0.9]"
+
+include("MadGraphControl_Pythia8EvtGen_A14NNPDF30LO_Pseudoscalar_2HDMa_monoH.py")

share/DSID312xxx/MC15.312664.MGPy8EG_A14N30LO_2HDMa_bb_monoHyy_tb5_sp035_mA1500_ma500.py

+THDMparams = {}
+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
+Reweight = {}
+Reweight['tanbeta'] = "scan:[0.3, 1, 5, 10, 20]"
+Reweight['sinp'] = "scan:[0.1, 0.35, 0.7, 0.9]"
+
+include("MadGraphControl_Pythia8EvtGen_A14NNPDF30LO_Pseudoscalar_2HDMa_monoH.py")

share/DSID312xxx/MC15.312665.MGPy8EG_A14N30LO_2HDMa_ggF_monoHyy_tb5_sp035_mA1500_ma500.py

+THDMparams = {}
+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
+Reweight = {}
+Reweight['tanbeta'] = "scan:[0.3, 1, 5, 10, 20]"
+Reweight['sinp'] = "scan:[0.1, 0.35, 0.7, 0.9]"
+
+include("MadGraphControl_Pythia8EvtGen_A14NNPDF30LO_Pseudoscalar_2HDMa_monoH.py")

share/DSID312xxx/MC15.312666.MGPy8EG_A14N30LO_2HDMa_bb_monoHyy_tb1_sp035_mA200_ma100.py

+THDMparams = {}
+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
+Reweight = {}
+Reweight['tanbeta'] = "scan:[0.3, 1, 5, 10, 20]"
+Reweight['sinp'] = "scan:[0.1, 0.35, 0.7, 0.9]"
+
+include("MadGraphControl_Pythia8EvtGen_A14NNPDF30LO_Pseudoscalar_2HDMa_monoH.py")

share/DSID312xxx/MC15.312667.MGPy8EG_A14N30LO_2HDMa_ggF_monoHyy_tb1_sp035_mA200_ma100.py

+THDMparams = {}
+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
+Reweight = {}
+Reweight['tanbeta'] = "scan:[0.3, 1, 5, 10, 20]"
+Reweight['sinp'] = "scan:[0.1, 0.35, 0.7, 0.9]"
+
+include("MadGraphControl_Pythia8EvtGen_A14NNPDF30LO_Pseudoscalar_2HDMa_monoH.py")

share/DSID312xxx/MC15.312668.MGPy8EG_A14N30LO_2HDMa_bb_monoHyy_tb1_sp035_mA200_ma300.py

+THDMparams = {}
+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
+Reweight = {}
+Reweight['tanbeta'] = "scan:[0.3, 1, 5, 10, 20]"
+Reweight['sinp'] = "scan:[0.1, 0.35, 0.7, 0.9]"
+
+include("MadGraphControl_Pythia8EvtGen_A14NNPDF30LO_Pseudoscalar_2HDMa_monoH.py")

share/DSID312xxx/MC15.312669.MGPy8EG_A14N30LO_2HDMa_ggF_monoHyy_tb1_sp035_mA200_ma300.py

+THDMparams = {}
+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
+Reweight = {}
+Reweight['tanbeta'] = "scan:[0.3, 1, 5, 10, 20]"
+Reweight['sinp'] = "scan:[0.1, 0.35, 0.7, 0.9]"
+
+include("MadGraphControl_Pythia8EvtGen_A14NNPDF30LO_Pseudoscalar_2HDMa_monoH.py")

share/DSID312xxx/MC15.312670.MGPy8EG_A14N30LO_2HDMa_bb_monoHyy_tb1_sp035_mA200_ma500.py

+THDMparams = {}
+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
+Reweight = {}
+Reweight['tanbeta'] = "scan:[0.3, 1, 5, 10, 20]"
+Reweight['sinp'] = "scan:[0.1, 0.35, 0.7, 0.9]"
+
+include("MadGraphControl_Pythia8EvtGen_A14NNPDF30LO_Pseudoscalar_2HDMa_monoH.py")

share/DSID312xxx/MC15.312671.MGPy8EG_A14N30LO_2HDMa_ggF_monoHyy_tb1_sp035_mA200_ma500.py

+THDMparams = {}
+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
+Reweight = {}
+Reweight['tanbeta'] = "scan:[0.3, 1, 5, 10, 20]"
+Reweight['sinp'] = "scan:[0.1, 0.35, 0.7, 0.9]"
+
+include("MadGraphControl_Pythia8EvtGen_A14NNPDF30LO_Pseudoscalar_2HDMa_monoH.py")

share/DSID312xxx/MC15.312672.MGPy8EG_A14N30LO_2HDMa_bb_monoHyy_tb1_sp035_mA600_ma100.py

+THDMparams = {}
+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
+Reweight = {}
+Reweight['tanbeta'] = "scan:[0.3, 1, 5, 10, 20]"
+Reweight['sinp'] = "scan:[0.1, 0.35, 0.7, 0.9]"
+
+include("MadGraphControl_Pythia8EvtGen_A14NNPDF30LO_Pseudoscalar_2HDMa_monoH.py")

share/DSID312xxx/MC15.312673.MGPy8EG_A14N30LO_2HDMa_ggF_monoHyy_tb1_sp035_mA600_ma100.py

+THDMparams = {}
+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.