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How to use addsubstitutions method in tox

Best Python code snippet using tox_python

MdependentWaves.py

Source:MdependentWaves.py

1from ROOT import *2from math import *3from array import *4from Urania import PDG5from Urania.Helicity import *6from Urania import RooInterfaces as D7spins = [0,1]8## ### Generate the pdf using the tools in Urania.Helicity9A = doB2VX(spins, helicities = [1,-1], transAmp = 1)#0)10### masage a bit the expression to make it more suitable for fitting11pdf_split = DecomposeAmplitudes(A,TransAmplitudes.values())#H.values())12phys = 013DefineStrongPhases()14SpinMap = { v:k for k,v in TransAmplitudes.items()}15for key in pdf_split: phys += StrongPhases(key)*pdf_split[key]16    17#BREAK18### change the free variables to cosines19x = Symbol("helcosthetaK",real = True)20y = Symbol("helcosthetaL", real = True)21z = Symbol("helphi", real = True)22CThL = Cos(ThetaL)23CThK = Cos(ThetaK)24def changeFreeVars(function):25    ### Phi now as in DTT !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!26    function  = function.subs( Sin(2*ThetaK), 2*Sin(ThetaK)*Cos(ThetaK))27    function  = function.subs( Cos(2*ThetaK), 2*Cos(ThetaK)**2 - 1)28    function  = function.subs( Sin(ThetaK), Sqrt(1-Cos(ThetaK)**2))29    function  = function.subs( Sin(ThetaL), Sqrt(1-Cos(ThetaL)**2))30    function = function.subs([(CThK,x),(CThL,y), (Phi, -z)])31    return function32func = changeFreeVars(phys)33### Replace amplitudes by more suitable fit parameters34s_As2 = Symbol("As2",positive = True)35s_fL = Symbol("fL",positive = True)36s_fpa = Symbol("fpa",positive = True)37#s_xpa = Symbol("xpa",positive = True)38fpe = 1-s_fL - s_fpa39Ap2 = 1-s_As240from Urania.MassAmplitudes import *41Pw  = NoRelBW.subs( [(m0,PDG.Kst0.mass), (Gamma0,PDG.Kst0.width)])42Sw = Kmatrix_KpiSwave43mass_subs = [(TransAmpModuli["1_pa"], Pw*Sqrt(Ap2*s_fpa)),(TransAmpModuli["1_0"], Pw*Sqrt(Ap2*s_fL)),(TransAmpModuli["1_pe"], Pw*Sqrt(Ap2*fpe)),(TransAmpModuli["0_0"],Sw*Sqrt(s_As2))] 44#func = func.subs( [ (TransAmpModuli["2_pe"], Sqrt(Ad2*f2pe)),(TransAmpModuli["2_pa"], Sqrt(Ad2*f2pa)),(TransAmpModuli["2_0"], Sqrt(Ad2*s_f2L))])45#BREAK46c1_psi = Symbol("c1_psi",real = True)47c2_psi = Symbol("c2_psi",real = True)48c3_psi = Symbol("c3_psi",real = True)49c4_psi = Symbol("c4_psi",real = True)50y_acc = Symbol("y_acc", positive = True)51c2_theta = Symbol("c2_theta", real = True)52c5_psi = -1-c1_psi - c2_psi - c3_psi - c4_psi + y_acc53acc = (1. + c1_psi*x + c2_psi*x*x + c3_psi*x*x*x + c4_psi*x*x*x*x + c5_psi*x*x*x*x*x)*(1.  + c2_theta*y*y)54#func = func*acc55ang_integral = iter_integrate(func, (z,-Pi,Pi),(x,-1,1),(y,-1,1))56func = func.subs( mass_subs )57ang_integral = ang_integral.subs(mass_subs)58func *= B2JpsiKpi_ps59ang_integral *= B2JpsiKpi_ps60### Figure out which variables the fit will depend on61# potential_list = [x,y,z]+TransAmpModuli.values()+TransAmpPhases.values()62potential_list = [x,y,z]+[ s_As2, s_fL, s_fpa]+TransAmpPhases.values() + [c1_psi,c2_psi,c3_psi,c4_psi,y_acc, c2_theta, mass]63final_list = []64for thing in potential_list:65    if thing in func.atoms(): final_list.append(thing)66### Generate and compile a fitting class corresponding to "func"67op2 = D.RooClassGenerator(func, final_list,"NoAccMdepAngJpsiKpi_J" +str( max(spins)))68op2.addSubstitutions([(Sqrt(-x**2+1),"sthk"),(Sqrt(-y**2+1),"sthl"),((-x**2+1),"sthk2"),((-y**2+1),"sthl2")])69op2.addSubstitutions([(x**2,"cthk2"),(y**2,"cthl2"),(Cos(z)**2,"cosphi2"),(Sin(z)**2,"sinphi2"),(Cos(z),"cosphi"),(Sin(z),"sinphi")])70op2.addSubstitutions([(Sqrt(s_As2),"As")])#,(Sqrt(s_fD),"sqfD")])71op2.addSubstitutions([(Sqrt(s_fL),"sqfL"),(Sqrt(s_fpa),"sqfpa")])72#op2.addSubstitutions([(Sqrt(s_f2L),"sqf2L"),(Sqrt(s_x2pa),"sqx2pa")])73#op2.addSubstitutions([(Cos(TransAmpPhases["2_0"]), "cdelta20"),(Cos(TransAmpPhases["2_pa"]), "cdelta2pa"),(Cos(TransAmpPhases["2_pe"]), "cdelta2pe")])74#op2.addSubstitutions([(Sin(TransAmpPhases["2_0"]), "sdelta20"),(Sin(TransAmpPhases["2_pa"]), "sdelta2pa"),(Sin(TransAmpPhases["2_pe"]), "sdelta2pe")])75op2.addSubstitutions([(Cos(TransAmpPhases["1_pa"]), "cdelta_pa"),(Cos(TransAmpPhases["1_pe"]), "cdelta_pe")])76op2.addSubstitutions([(Sin(TransAmpPhases["1_pa"]), "sdelta_pa"),(Sin(TransAmpPhases["1_pe"]), "sdelta_pe")])77op2.addSubstitutions([(Sin(TransAmpPhases["0_0"]), "sdelta_s"),(Cos(TransAmpPhases["0_0"]), "cdelta_s")])78op2.addSubstitutions([(Sqrt(2),"sq2"),(Sqrt(3),"sq3"),(Sqrt(5),"sq5")])79#op2.addSubstitutions([((-x**2+1),"sthk2"),((-y**2+1),"sthl2"),(x**2,"cthk2"),(y**2,"cthl2"),(Cos(z),"cosphi"),(Sin(z),"sinphi"),(Sqrt(2),"sq2"),(Sqrt(5),"sq5")])80op2.makePdf(integrable = kTRUE)81#zz = integrate(func,(z,-Pi,Pi))82op2.forceIntegral(1,[x,y,z], ang_integral)83#op2.doIntegralM(2,(x,-1,1),(y,-1,1))84#op2.doIntegralM(3,(z,-Pi,Pi),(x,-1,1))85#op2.doIntegralM(4,(z,-Pi,Pi),(y,-1,1))86#op2.doIntegralM(5,(x,-1,1))87#op2.doIntegralM(6,(y,-1,1))88#op2.doIntegralM(7,(z,-Pi,Pi))89op2.overwrite()90op2.invoke()91BREAK92##############  MAKING TREE93label = 'PLOT'94f=TFile("NewAngleTree.root")95tree=f.Get("T")96f1=TFile("/tmp/trash.root","recreate")97tree1 = tree.CopyTree("MC_k>0")98tree2 = tree.CopyTree("MC_k<0")99###################  CONSTRUCTING THE MODEL100As2 = RooRealVar("As2","As2",0.,1.)101#As = RooFormulaVar("As","As","sqrt(As2)",RooArgList(As2))102fD = RooRealVar("fD","fD",0.,1)103#Ad2 = RooFormulaVar("Ad2","Ad2", "fD*(1-As2)",RooArgList(As2,fD))104#Ap2 = RooFormulaVar("Ap2","Ap2", "(1-fD)*(1-As2)", RooArgList(As2,fD))105fL = RooRealVar("fL","fL",0.,1)106xpa = RooRealVar("xpa","xpa", 0.,1)107#fpa = RooFormulaVar("fpa","fpa","xpa*(1-fL)",RooArgList(xpa,fL))108#fpe = RooFormulaVar("fpe","fpe","(1-xpa)*(1-fL)",RooArgList(xpa,fL))109#A0 = RooFormulaVar("A0","A0","sqrt(Ap2*fL)",RooArgList(Ap2,fL))110#Apa = RooFormulaVar("Apa","Apa","sqrt(Ap2*fpa)",RooArgList(Ap2,fpa))111#Ape = RooFormulaVar("Ape","Ape","sqrt(Ap2*fpe)",RooArgList(Ap2,fpe))112### D-wave polarization fractions113f2L = RooRealVar("f2L","f2L",0.,1)114x2pa = RooRealVar("x2pa","x2pa", 0.,1)115#f2pa = RooFormulaVar("f2pa","f2pa","x2pa*(1-f2L)",RooArgList(x2pa,f2L))116#f2pe = RooFormulaVar("f2pe","f2pe","(1-x2pa)*(1-f2L)",RooArgList(x2pa,f2L))117#A20 = RooFormulaVar("A20","A20","sqrt(Ad2*f2L)",RooArgList(Ad2,f2L))118#A2pa = RooFormulaVar("A2pa","A2pa","sqrt(Ad2*f2pa)",RooArgList(Ad2,f2pa))119#A2pe = RooFormulaVar("A2pe","A2pe","sqrt(Ad2*f2pe)",RooArgList(Ad2,f2pe))120CThetaL = RooRealVar("cL","cos(ThetaL) ", -1,1)121CThetaK = RooRealVar("cK","cos(ThetaK) ", -1,1)122Phi = RooRealVar("ph","Phi", -pi,pi)123#A0 = RooRealVar("A0","A0",0.77,0.5,1.)124#Apa = RooRealVar("Apa","Apa",0.5,0.3,1.)125#Ape  = RooRealVar("Ape" ,"Ape" ,1/2,0.,1.)126#Ape = RooFormulaVar("Ape","Ape","sqrt(1-As*As-Apa*Apa-A0*A0)",RooArgList(A0,As,Apa))127deltaPa = RooRealVar("deltaPa","deltaPa",2.501,2.,2*pi)128deltaPe = RooRealVar("deltaPe","deltaPe",1,  -pi,pi)129deltaS  = RooRealVar("deltaS" ,"deltaS" ,0.9,0.,2*pi)130#A20 = RooRealVar("A0","A0",0.77,0.,1.)131#A2pa = RooRealVar("A2pa","A2pa",0.5,0.,1.)132#A2pe = RooRealVar("A2pe","A2pe",0.5,0.,1.)133#As  = RooRealVar("As" ,"As" ,1/2,0.,1.)134#As = RooFormulaVar("As","As","sqrt(1-Ape*Ape-Apa*Apa-A0*A0-A2pe*A2pe-A2pa*A2pa-A20*A20)",RooArgList(A0,Ape,Apa,A20,A2pa,A2pe))135delta2Pa = RooRealVar("delta2Pa","delta2Pa",2.501,2.,2*pi)136delta2Pe = RooRealVar("delta2Pe","delta2Pe",1,  -pi,pi)137delta20  = RooRealVar("delta20" ,"delta20" ,0.9,0.,2*pi)138#model=RooFirst("model","model",CThetaK,CThetaL,Phi,As2,139model2=AngJpsiKpi_J1("model2","model2",CThetaK,CThetaL,Phi,As2,fL,xpa,deltaPa,deltaPe,deltaS)140## As2.setVal(1)141## fr = CThetaK.frame()142## model2.plotOn(fr)143## fr.Draw()144## BREAK145###################  FITTING DATA146  ### tree - mix of B & Bbar147  ### tree1 - K+148  ### tree2 - K-149data = RooDataSet(label, label,tree1,RooArgSet(CThetaL,CThetaK,Phi))150#data = model.generate(RooArgSet(CThetaL,CThetaK,Phi),100000) ;151#As.setVal(0)152#As.setConstant(kTRUE)153#deltaS.setConstant(kTRUE)154#deltaPe.setConstant(kTRUE)155def test(model):156    res = model.fitTo(data,RooFit.Minos(kTRUE))#, RooFit.Range("REDUCED"))157    Angframe = CThetaK.frame()158    data.plotOn(Angframe)159    model.plotOn(Angframe)160    Angframe.Draw()161    return res, Angframe162#w_1 = test(model)163w_2 = test(model2)...

Paula2.py

Source:Paula2.py

1from ROOT import *2from Urania.Helicity import *3#AccessPackage("Urania")4#import Helicity as H5from Urania.SympyBasic import *6from Urania.RooInterfaces import *7from os import *8MyTransAmplitudes = {}9MyTransAmplitudes["A0"] = Symbol("A_0")10MyTransAmplitudes["Apa"] = Symbol("A_pa")11MyTransAmplitudes["Ape"] = Symbol("A_pe")12MyTransAmplitudes["ASS"] = Symbol("A_SS")13MyTransAmplitudes["ASplus"] = Symbol("A_Splus")14MyTransAmplitudes["ASminus"] = Symbol("A_Sminus")15for key in MyTransAmplitudes:16    amp = str(MyTransAmplitudes[key])17    if key not in TransAmpModuli.keys(): TransAmpModuli[key] = Symbol(amp+"_mod",positive = True)18    if key not in TransAmpPhases.keys(): TransAmpPhases[key] = Symbol("delta" + amp.replace("A",""),real = True)19### convencion delta0 = 020TransAmpPhases.pop("A0")21Hmod, Hphases = {}, {}22A = doB2XhhYhh([1],range(2))23A = A.subs([(H["Ja1_Jb1_0"], MyTransAmplitudes["A0"]), (H["Ja1_Jb1_1"],1/Sqrt(2)*( MyTransAmplitudes["Apa"] + MyTransAmplitudes["Ape"])),(H["Ja1_Jb1_-1"],1/Sqrt(2)*( MyTransAmplitudes["Apa"]-MyTransAmplitudes["Ape"]))]) ### De momentosolo te sustituyo los del PP-wave....24A = A.subs([(H["Ja0_Jb0_0"], MyTransAmplitudes["ASS"]), (H["Ja1_Jb0_0"],1/Sqrt(2)*( MyTransAmplitudes["ASplus"] + MyTransAmplitudes["ASminus"])),(H["Ja0_Jb1_0"],1/Sqrt(2)*( MyTransAmplitudes["ASplus"]-MyTransAmplitudes["ASminus"]))]) ### Y las Ss, SP25A = A.expand()/9 ### Normalizacion de London26for key in H:27    amp = str(H[key])28    Hmod[key] = Symbol(amp+"_mod",positive = True)29    Hphases[key] = Symbol("delta" + amp.replace("H",""),real = True)30pdf_split = DecomposeAmplitudes(A,MyTransAmplitudes.values() + H.values())31### Deleting terms not present in the Untagged fit32pdf_delete = {}33ape = TransAmplitudes["1_pe"]34asp = TransAmplitudes["asp"]35for ak in TransAmplitudes.values():36    if ape!=ak: 37        _re, _im = TermsAsReImag(A,ak,ape)38        pdf_delete[re(ak*ape.conjugate())]=_re39        pdf_delete[im(ak*ape.conjugate())]=_im40        pdf_delete[re(ape*ak.conjugate())]=_re41        pdf_delete[im(ape*ak.conjugate())]=_im42    if asp!=ak:43        _re, _im = TermsAsReImag(A,ak,asp)44        pdf_delete[re(ak*asp.conjugate())]=_re45        pdf_delete[im(ak*asp.conjugate())]=_im46        pdf_delete[re(asp*ak.conjugate())]=_re47        pdf_delete[im(asp*ak.conjugate())]=_im48phys = 049def MyStrongPhases(expr, free_delta0=0):50    """ Modifies a term written as A1*conj(A2) as a function of the strong phases51    """52    modlist = []53    #DefineStrongPhases()54    for key in MyTransAmplitudes.keys():55        if key == "A0" and not free_delta0:56            modlist.append( (MyTransAmplitudes[key], TransAmpModuli[key]))57            continue58        modlist.append( (MyTransAmplitudes[key],TransAmpModuli[key]*Exp(I*TransAmpPhases[key])) )59    for key in H.keys(): ### These we keep in Helicity formalism because... well, because I don't know otherwise60        modlist.append( (H[key],Hmod[key]*Exp(I*Hphases[key])) )61    f = expr.func62    if f in [im,re]:63        arg = expr.args[0]64        arg = arg.subs( modlist )65        arg = arg.rewrite(Exp,Cos)66        return simplify(f(arg))67    out = expr.subs( modlist )68    out = out.rewrite(Exp,Cos)69    return simplify(out)70for key in pdf_split: phys += MyStrongPhases(key)*pdf_split[key]71### change the free variables to cosines72x = Symbol("helcosthetaK",real = True)73y = Symbol("helcosthetaL", real = True)74z = Symbol("helphi", real = True)75CThL = Cos(ThetaL)76CThK = Cos(ThetaK)77def changeFreeVars(function):78    function  = function.subs( Sin(ThetaK), Sqrt(1-Cos(ThetaK)**2))79    function  = function.subs( Sin(ThetaL), Sqrt(1-Cos(ThetaL)**2))80    function = function.subs([(CThK,x),(CThL,y), (Phi,z)])81    return function82func = changeFreeVars(phys)83##### Generate and compile a fitting class corresponding to "func"84### Trial 1, w/o analytical integrals85potential_list = [x,y,z]+TransAmpModuli.values() + TransAmpPhases.values() + Hmod.values() + Hphases.values()  ### Esto es una chapuza, por no pensar cuales son los parametros del modelo, meto todas86                                                                                                               ### las amplitudes y phases, y luego filtro las que no estan en la formula :D87final_list = []88for thing in potential_list:89     if thing in func.atoms() and thing not in final_list: final_list.append(thing)90op2 = RooClassGenerator(func, final_list ,"RooCrap")91### Define intermediate variables to be calculated once92op2.addSubstitutions([(Sqrt(-x**2+1),"sthk"),(Sqrt(-y**2+1),"sthl"),((-x**2+1),"sthk2"),((-y**2+1),"sthl2")])93op2.addSubstitutions([(x**2,"cthk2"),(y**2,"cthl2"),(Cos(z)**2,"cosphi2"),(Sin(z)**2,"sinphi2"),(Cos(z),"cosphi"),(Sin(z),"sinphi")])94### Mira si puedes poner cosas como las de abajo, para hacer el codigo mas rapido95#op2.addSubstitutions([(Sqrt(s_As2),"As"),(Sqrt(s_fD),"sqfD")])96#op2.addSubstitutions([(Sqrt(s_fL),"sqfL"),(Sqrt(s_xpa),"sqxpa")])97#op2.addSubstitutions([(Sqrt(s_f2L),"sqf2L"),(Sqrt(s_x2pa),"sqx2pa")])98#op2.addSubstitutions([(Cos(TransAmpPhases["2_0"]), "cdelta20"),(Cos(TransAmpPhases["2_pa"]), "cdelta2pa"),(Cos(TransAmpPhases["2_pe"]), "cdelta2pe")])99#op2.addSubstitutions([(Sin(TransAmpPhases["2_0"]), "sdelta20"),(Sin(TransAmpPhases["2_pa"]), "sdelta2pa"),(Sin(TransAmpPhases["2_pe"]), "sdelta2pe")])100#op2.addSubstitutions([(Cos(TransAmpPhases["1_pa"]), "cdelta_pa"),(Cos(TransAmpPhases["1_pe"]), "cdelta_pe")])101#op2.addSubstitutions([(Sin(TransAmpPhases["1_pa"]), "sdelta_pa"),(Sin(TransAmpPhases["1_pe"]), "sdelta_pe")])102#op2.addSubstitutions([(Sin(TransAmpPhases["0_0"]), "sdelta_s"),(Cos(TransAmpPhases["0_0"]), "cdelta_s")])103op2.makePdf(integrable = kTRUE)104op2.doIntegral(1,(x,-1,1))105op2.doIntegral(2,(y,-1,1))106op2.doIntegral(3,(z,-Pi,Pi))107op2.doIntegral(4,(x,-1,1),(y,-1,1))108op2.doIntegral(5,(x,-1,1),(z,-Pi,Pi))109op2.doIntegral(6,(y,-1,1),(z,-Pi,Pi))110op2.doIntegral(7,(x,-1,1),(y,-1,1),(z,-Pi,Pi))111op2.overwrite()...

WavesTristanWeights.py

Source:WavesTristanWeights.py

1from ROOT import *2from math import *3from array import *4from Urania import PDG5from Urania.Helicity import *6from Urania import RooInterfaces as D7spins = [0,1,2]8## ### Generate the pdf using the tools in Urania.Helicity9A = doB2VX(spins, helicities = [1,-1], transAmp = 1)#0)10### masage a bit the expression to make it more suitable for fitting11pdf_split = DecomposeAmplitudes(A,TransAmplitudes.values())#H.values())12#pdf_split = DecomposeAmplitudes_withCSP(A,TransAmplitudes)#H.values())13phys = 014TristanIntegral = 015TristanWeights = {}16### CSP factors17DefineStrongPhases()18SpinMap = { v:k for k,v in TransAmplitudes.items()}19CSP_factors = []20for key in pdf_split:21    Amp1 = list(key.atoms())[0]22    Amp2 = list(key.atoms())[1]23    cte = One24    if Amp2 != 2 and Amp1 !=2:25        J1 = max( SpinMap[Amp1][0],  SpinMap[Amp2][0])26        J2 = min( SpinMap[Amp1][0],  SpinMap[Amp2][0])27        if J1 != J2 :28            cte = USymbol("Cfact_" + J1 + J2 , "C_{" + J1 + "," + J2 + "}", real = True)29            if cte not in CSP_factors: CSP_factors.append(cte)30        31    phys += StrongPhases(key)*pdf_split[key]*cte32    if pdf_split[key]:33        TristanWeights[key] =  Symbol("w_" + str(Amp1) + str(Amp2), positive = True)34        TristanIntegral += StrongPhases(key) *  TristanWeights[key]*cte35#BREAK36### change the free variables to cosines37x = USymbol("helcosthetaK","c\\theta_K",real = True)38y = USymbol("helcosthetaL","c\\theta_l",  real = True)39z = USymbol("helphi","\\phi",  real = True)40CThL = Cos(ThetaL)41CThK = Cos(ThetaK)42def changeFreeVars(function):43    function  = function.subs( Sin(2*ThetaK), 2*Sin(ThetaK)*Cos(ThetaK))44    function  = function.subs( Cos(2*ThetaK), 2*Cos(ThetaK)**2 - 1)45    function  = function.subs( Sin(ThetaK), Sqrt(1-Cos(ThetaK)**2))46    function  = function.subs( Sin(ThetaL), Sqrt(1-Cos(ThetaL)**2))47    #function = function.subs([(CThK,x),(CThL,y), (Phi,-Pi-z)])48    function = function.subs([(CThK,x),(CThL,y), (Phi,-z)])49    return function50func = changeFreeVars(phys)51### Replace amplitudes by more suitable fit parameters52#BREAK53#s_xpa = Symbol("xpa",positive = True)54#s_x2pa = Symbol("x2pa",positive = True)55# S-wave amplitude.56s_As2 = USymbol("As2","F_S",positive = True)57# D-wave amplitudes.58s_fD = Symbol("fD", positive = True)59Ad2 = (1-s_As2)*s_fD60s_f2L = Symbol("f2L",positive = True)61s_f2pa = Symbol("f2pa",positive = True)#x2pa*(1-s_f2L)62f2pe = 1-s_f2L - s_f2pa63# P-wave amplitudes.64Ap2 = 1-s_As2 - Ad265s_fL = USymbol("fL","f_L",positive = True)66s_fpa = USymbol("fpa","f_{||}",positive = True)#s_xpa*(1-s_fL)67fpe = 1-s_fL - s_fpa68func = func.subs( [ (TransAmpModuli["2_pe"], Sqrt(Ad2*f2pe)),(TransAmpModuli["2_pa"], Sqrt(Ad2*s_f2pa)),(TransAmpModuli["2_0"], Sqrt(Ad2*s_f2L))])69func = func.subs( [(TransAmpModuli["1_pa"], Sqrt(Ap2*s_fpa)),(TransAmpModuli["1_0"], Sqrt(Ap2*s_fL)),(TransAmpModuli["1_pe"], Sqrt(Ap2*fpe))] )70func = func.subs( TransAmpModuli["0_0"],Sqrt(s_As2))71TristanIntegral = TristanIntegral.subs( [ (TransAmpModuli["2_pe"], Sqrt(Ad2*f2pe)),(TransAmpModuli["2_pa"], Sqrt(Ad2*s_f2pa)),(TransAmpModuli["2_0"], Sqrt(Ad2*s_f2L))])72TristanIntegral = TristanIntegral.subs( [(TransAmpModuli["1_pa"], Sqrt(Ap2*s_fpa)),(TransAmpModuli["1_0"], Sqrt(Ap2*s_fL)),(TransAmpModuli["1_pe"], Sqrt(Ap2*fpe))] )73TristanIntegral = TristanIntegral.subs( TransAmpModuli["0_0"],Sqrt(s_As2))74### Figure out which variables the fit will depend on75potential_list = [x,y,z]+[ s_As2, s_fD, s_fL, s_fpa, s_f2L, s_f2pa ]+TransAmpPhases.values() + CSP_factors +  TristanWeights.values() 76final_list = []77for thing in potential_list:78    if thing in func.atoms() or thing in TristanIntegral.atoms(): final_list.append(thing)79    80### Generate and compile a fitting class corresponding to "func"81#BREAK82class_name = "TristanJpsiKpi_J" +str( max(spins))83op2 = D.RooClassGenerator(func, final_list,class_name)84op2.PrintToLatex()85BREAK86op2.addSubstitutions([(Sqrt(-x**2+1),"sthk"),(Sqrt(-y**2+1),"sthl"),((-x**2+1),"sthk2"),((-y**2+1),"sthl2")])87op2.addSubstitutions([(x**2,"cthk2"),(y**2,"cthl2"),(Cos(z)**2,"cosphi2"),(Sin(z)**2,"sinphi2"),(Cos(z),"cosphi"),(Sin(z),"sinphi")])88op2.addSubstitutions([(Sqrt(s_As2),"As"),(Sqrt(s_fD),"sqfD")])89op2.addSubstitutions([(Sqrt(s_fL),"sqfL"),(Sqrt(s_fpa),"sqfpa")])90op2.addSubstitutions([(Sqrt(s_f2L),"sqf2L"),(Sqrt(s_f2pa),"sqf2pa")])91#op2.addSubstitutions([(Sqrt(s_f2L),"sqf2L"),(Sqrt(s_x2pa),"sqx2pa")])92op2.addSubstitutions([(Cos(TransAmpPhases["2_0"]), "cdelta20"),(Cos(TransAmpPhases["2_pa"]), "cdelta2pa"),(Cos(TransAmpPhases["2_pe"]), "cdelta2pe")])93op2.addSubstitutions([(Sin(TransAmpPhases["2_0"]), "sdelta20"),(Sin(TransAmpPhases["2_pa"]), "sdelta2pa"),(Sin(TransAmpPhases["2_pe"]), "sdelta2pe")])94op2.addSubstitutions([(Cos(TransAmpPhases["1_pa"]), "cdelta_pa"),(Cos(TransAmpPhases["1_pe"]), "cdelta_pe")])95op2.addSubstitutions([(Sin(TransAmpPhases["1_pa"]), "sdelta_pa"),(Sin(TransAmpPhases["1_pe"]), "sdelta_pe")])96op2.addSubstitutions([(Sin(TransAmpPhases["0_0"]), "sdelta_s"),(Cos(TransAmpPhases["0_0"]), "cdelta_s")])97op2.addSubstitutions([(Sqrt(2),"sq2"),(Sqrt(3),"sq3"),(Sqrt(5),"sq5")])98#op2.addSubstitutions([((-x**2+1),"sthk2"),((-y**2+1),"sthl2"),(x**2,"cthk2"),(y**2,"cthl2"),(Cos(z),"cosphi"),(Sin(z),"sinphi"),(Sqrt(2),"sq2"),(Sqrt(5),"sq5")])99op2.makePdf(integrable = kTRUE)100op2.forceIntegral(1,[x,y,z], TristanIntegral)101op2.overwrite()102#op2.invoke()103gROOT.ProcessLine(".L "+class_name + ".cxx++")...

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