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Utility scripts for non-prompt studies + model predictions (#224)
* Add GMVFNS predictions with two-step approach * Add NNLO predictions * Add utility scripts for non-prompt studies * remove NNLO
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''' | ||
python script to get the fraction of the non-prompt charmed hadrons coming from each B hadron | ||
''' | ||
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import argparse | ||
import numpy as np | ||
from ROOT import TFile #pylint: disable=import-error,no-name-in-module | ||
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parser = argparse.ArgumentParser(description='Arguments to pass') | ||
parser.add_argument('inFileName', metavar='text', default='predictions.root', | ||
help='input root or txt file with non-prompt FONLL predictions') | ||
args = parser.parse_args() | ||
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charmHadronNames = ['D0 ', 'Dplus', 'Ds ', 'Lc ', 'Dstar'] | ||
beautyHadronNames = ['B0', 'Bplus', 'Bs', 'Lb'] | ||
histNames = ['hBRHbtoD0', 'hBRHbtoDplus', 'hBRHbtoDs', 'hBRHbtoLc', 'hBRHbtoDstar'] | ||
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brMatrix = np.zeros((len(charmHadronNames), len(beautyHadronNames))) | ||
ffArray = np.zeros(len(beautyHadronNames)) | ||
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#hHbFF | ||
inFile = TFile.Open(args.inFileName) | ||
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ffHisto = inFile.Get('hHbFF') | ||
for iBin in range(ffHisto.GetNbinsX()): | ||
ffArray[iBin] = ffHisto.GetBinContent(iBin+1) | ||
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for iHadron, histName in enumerate(histNames): | ||
histo = inFile.Get(histName) | ||
for iBin in range(histo.GetNbinsX()): | ||
brMatrix[iHadron][iBin] = histo.GetBinContent(iBin+1) | ||
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contrMatrix = np.multiply(brMatrix, ffArray) | ||
normContrMatrix = (contrMatrix.T/contrMatrix.sum(axis=1)).T | ||
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print(' ', *beautyHadronNames, sep=' ') | ||
for iHadron, hadronName in enumerate(charmHadronNames): | ||
print(hadronName, normContrMatrix[iHadron]) |
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""" | ||
Utility script to estimate the "natural" non-prompt fraction from FONLL + PYTHIA8 | ||
""" | ||
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import sys | ||
import numpy as np | ||
from ROOT import TFile, TCanvas, TLegend #pylint: disable=import-error,no-name-in-module | ||
from ROOT import kRed, kOrange, kGreen #pylint: disable=import-error,no-name-in-module | ||
sys.path.append('..') | ||
from utils.StyleFormatter import SetGlobalStyle, SetObjectStyle #pylint: disable=wrong-import-position,import-error | ||
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def main(): #pylint: disable=too-many-statements | ||
SetGlobalStyle(padleftmargin=0.18, padbottommargin=0.14, titleoffsety=1.6, maxdigits=2, optstat=0) | ||
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inFileFONLL = TFile.Open('fonll/feeddown/DmesonLcPredictions_502TeV_y05_FFee_BRpythia8_SepContr_PDG2020.root') | ||
hFONLLPromptD0 = inFileFONLL.Get('hD0Kpipred_max') | ||
hFONLLPromptDplus = inFileFONLL.Get('hDpluskpipipred_max') | ||
hFONLLPromptDs = inFileFONLL.Get('hDsPhipitoKkpipred_max') | ||
hFONLLNonPromptD0 = inFileFONLL.Get('hD0KpifromBpred_central_corr') | ||
hFONLLNonPromptDplus = inFileFONLL.Get('hDpluskpipifromBpred_central_corr') | ||
hFONLLNonPromptDs = inFileFONLL.Get('hDsPhipitoKkpifromBpred_central_corr') | ||
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binLims = np.array([0., 1., 2., 3., 4., 5., 6., 7., 8., 10., 12., 16., 24.], 'd') | ||
nBins = 12 | ||
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hFONLLPromptD0 = hFONLLPromptD0.Rebin(nBins, 'hFONLLPromptD0', binLims) | ||
hFONLLPromptDplus = hFONLLPromptDplus.Rebin(nBins, 'hFONLLPromptDplus', binLims) | ||
hFONLLPromptDs = hFONLLPromptDs.Rebin(nBins, 'hFONLLPromptDs', binLims) | ||
hFONLLNonPromptD0 = hFONLLNonPromptD0.Rebin(nBins, 'hFONLLNonPromptD0', binLims) | ||
hFONLLNonPromptDplus = hFONLLNonPromptDplus.Rebin(nBins, 'hFONLLNonPromptDplus', binLims) | ||
hFONLLNonPromptDs = hFONLLNonPromptDs.Rebin(nBins, 'hFONLLNonPromptDs', binLims) | ||
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hFONLLNPfracD0 = hFONLLPromptD0.Clone('hFONLLNPfracD0') | ||
hFONLLNPfracD0.Divide(hFONLLNonPromptD0, hFONLLNPfracD0) | ||
hFONLLNPfracDplus = hFONLLPromptDplus.Clone('hFONLLNPfracDplus') | ||
hFONLLNPfracDplus.Divide(hFONLLNonPromptDplus, hFONLLNPfracDplus) | ||
hFONLLNPfracDs = hFONLLPromptDs.Clone('hFONLLNPfracDs') | ||
hFONLLNPfracDs.Divide(hFONLLNonPromptDs, hFONLLNPfracDs) | ||
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SetObjectStyle(hFONLLNPfracD0, color=kRed, linewitdh=2, markerstyle=0, fillstyle=0) | ||
SetObjectStyle(hFONLLNPfracDplus, color=kGreen, linewitdh=2, markerstyle=0, fillstyle=0) | ||
SetObjectStyle(hFONLLNPfracDs, color=kOrange, linewitdh=2, markerstyle=0, fillstyle=0) | ||
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mesonList = ['D0', 'D+', 'Ds'] | ||
histoList = [hFONLLNPfracD0, hFONLLNPfracDplus, hFONLLNPfracDs] | ||
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print(*binLims, sep=' ') | ||
for meson, histo in zip(mesonList, histoList): | ||
valueList = [] | ||
for iBin in range(1, nBins + 1): | ||
valueList.append(f'{histo.GetBinContent(iBin):.3f}') | ||
print(meson) | ||
print(*valueList, sep=' ') | ||
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legMeson = TLegend(0.65, 0.6, 0.85, 0.8) | ||
legMeson.SetTextSize(0.04) | ||
legMeson.SetFillStyle(0) | ||
legMeson.AddEntry(hFONLLNPfracD0, 'D^{0}', 'l') | ||
legMeson.AddEntry(hFONLLNPfracDplus, 'D^{+}', 'l') | ||
legMeson.AddEntry(hFONLLNPfracDs, 'D_{s}^{+}', 'l') | ||
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cFrac = TCanvas('cFrac', '', 500, 500) | ||
hFrame = cFrac.DrawFrame(0., 0.01, 24., 1.05, ';#it{p}_{T} (GeV/#it{c}); #it{f}_{non-prompt}') | ||
hFrame.GetYaxis().SetDecimals() | ||
hFrame.Draw('axis same') | ||
hFONLLNPfracD0.Draw('same') | ||
hFONLLNPfracDplus.Draw('same') | ||
hFONLLNPfracDs.Draw('same') | ||
legMeson.Draw('same') | ||
cFrac.Update() | ||
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TFile('./NaturalNonPromptFrac_FONLL_FFee_BRpythia8.root', 'recreate') | ||
hFONLLNPfracD0.Write() | ||
hFONLLNPfracDplus.Write() | ||
hFONLLNPfracDs.Write() | ||
cFrac.Write() | ||
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input('Press enter to exit') | ||
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main() |
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models/gvmfs/GMVFNS-nonPromptDplus-pp5-y05-2Steps-2021.txt
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#pp -> Dplus+X from pp -> b-quark | ||
#(using the two-step approach Bolzoni, Kramer, J.Phys.G 41 (2014) 075006) | ||
#for ALICE at 5.02 TeV | ||
#CT14nlo, m_b = 4.5 GeV, m_c = 1.3 GeV | ||
#sig-min/max from varying renormalization scale by factors 1/2-2 (nb/GeV) | ||
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pTmin pTmax cen min max | ||
2.00 3.00 8.1497E+02 6.0081E+02 1.1792E+03 | ||
3.00 4.00 4.0445E+02 2.9910E+02 5.8251E+02 | ||
4.00 5.00 2.3112E+02 1.7164E+02 3.3081E+02 | ||
5.00 6.00 1.3774E+02 1.0350E+02 1.9385E+02 | ||
6.00 8.00 7.0719E+01 5.4000E+01 9.7244E+01 | ||
8.00 10.00 3.0133E+01 2.3535E+01 4.0089E+01 | ||
10.00 12.00 1.4078E+01 1.1240E+01 1.8133E+01 | ||
12.00 16.00 5.5852E+00 4.5651E+00 6.9491E+00 |
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models/gvmfs/GMVFNS-nonPromptDzero-pp5-y05-2Steps-2021.txt
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#pp -> D0+X from pp -> b-quark | ||
#(using the two-step approach Bolzoni, Kramer, J.Phys.G 41 (2014) 075006) | ||
#for ALICE at 5.02 TeV | ||
#CT14nlo, m_b = 4.5 GeV, m_c = 1.3 GeV | ||
#sig-min/max from varying renormalization scale by factors 1/2-2 (nb/GeV) | ||
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pTmin pTmax cen min max | ||
1.00 2.00 4.2973E+03 3.1851E+03 6.1719E+03 | ||
2.00 3.00 2.1125E+03 1.5453E+03 3.0562E+03 | ||
3.00 4.00 1.0598E+03 7.7617E+02 1.5379E+03 | ||
4.00 5.00 5.8139E+02 4.2811E+02 8.3531E+02 | ||
5.00 6.00 3.3950E+02 2.5758E+02 4.7889E+02 | ||
6.00 7.00 2.1198E+02 1.6094E+02 2.9442E+02 | ||
7.00 8.00 1.3360E+02 1.0284E+02 1.8207E+02 | ||
8.00 10.00 7.2144E+01 5.6764E+01 9.5963E+01 | ||
10.00 12.00 3.3512E+01 2.6667E+01 4.3157E+01 | ||
12.00 16.00 1.3045E+01 1.0696E+01 1.6161E+01 | ||
16.00 24.00 2.9370E+00 2.4936E+00 3.4488E+00 |