def sigma_xy():
#beam sigma in x and y
gen = make_gen()
beam = gen.beam_par
gx = TGraph(beam.hz.GetNbinsX() + 1)
gy = TGraph(beam.hz.GetNbinsX() + 1)
for ibin in range(beam.hz.GetNbinsX() + 1):
zpos = beam.hz.GetBinCenter(ibin)
sx = beam.gx[ibin].GetParameter(2)
sy = beam.gy[ibin].GetParameter(2)
gx.SetPoint(ibin, zpos, sx)
gy.SetPoint(ibin, zpos, sy)
ut.set_graph(gx, rt.kBlue)
ut.set_graph(gy, rt.kRed)
can = ut.box_canvas()
frame = gPad.DrawFrame(-10e3, 0, 15.5e3, 3.3)
gx.Draw("lsame")
gy.Draw("lsame")
gPad.SetGrid()
ut.invert_col(gPad)
can.SaveAs("01fig.pdf")
def acc_both():
#acceptance for quasi-real photoproduction and for Pythia
#selection mode, 1 - s1, 2 - s2, 3 - s1 or s2, 4 - ecal, 5 - any
#acc_qr = acc_quasi_real(False)
acc_py_s1 = acc_pythia(False, 1)
acc_py_s2 = acc_pythia(False, 2)
#acc_py_s12 = acc_pythia(False, 3)
acc_py_ecal = acc_pythia(False, 4)
acc_py_all = acc_pythia(False, 5)
#acc_py = acc_gap("../data/ir6_close/lmon_pythia_5M_beff2_close_5Mevt.root")
#make the plot
can = ut.box_canvas()
#ut.set_graph(acc_qr, rt.kRed)
#ut.set_graph(acc_py, rt.kBlue, rt.kFullTriangleUp)
ut.set_graph(acc_py_s1, rt.kYellow+1)
ut.set_graph(acc_py_s2, rt.kGreen+1)
#ut.set_graph(acc_py_s12, rt.kBlack)
ut.set_graph(acc_py_ecal, rt.kBlue)
ut.set_graph(acc_py_all, rt.kBlack)
frame = gPad.DrawFrame(-10, 0, 5, 1.1) # 0.3
frame.Draw()
#ytit = "Acceptance / {0:.1f} %".format(prec*100)
ut.put_yx_tit(frame, "Acceptance", "log_{10}(#it{Q}^{2})", 1.6, 1.2)
frame.Draw()
ut.set_margin_lbtr(gPad, 0.11, 0.1, 0.03, 0.02)
gPad.SetGrid()
#acc_py.Draw("psame")
#acc_qr.Draw("psame")
acc_py_s1.Draw("psame")
acc_py_s2.Draw("psame")
#acc_py_s12.Draw("psame")
acc_py_all.Draw("psame")
acc_py_ecal.Draw("psame")
#leg = ut.prepare_leg(0.2, 0.82, 0.2, 0.12, 0.035)
leg = ut.prepare_leg(0.15, 0.78, 0.2, 0.16, 0.035)
#leg.AddEntry(acc_qr, "Quasi-real photoproduction", "lp")
#leg.AddEntry(acc_py, "Pythia6", "lp")
leg.AddEntry(acc_py_s1, "Tagger 1", "lp")
leg.AddEntry(acc_py_s2, "Tagger 2", "lp")
#leg.AddEntry(acc_py_s12, "Tagger 1 #bf{or} Tagger 2", "lp")
leg.AddEntry(acc_py_ecal, "ecal", "lp")
leg.AddEntry(acc_py_all, "Tagger 1 #bf{or} Tagger 2 #bf{or} ecal", "lp")
leg.Draw("same")
#ut.invert_col(rt.gPad)
can.SaveAs("01fig.pdf")
def div_xy():
#beam divergence in x and y
gen = make_gen()
beam = gen.beam_par
gx = TGraph(beam.hz.GetNbinsX() + 1)
gy = TGraph(beam.hz.GetNbinsX() + 1)
for ibin in range(beam.hz.GetNbinsX() + 1):
zpos = beam.hz.GetBinCenter(ibin)
dx = beam.divx[ibin].GetParameter(2)
dy = beam.divy[ibin].GetParameter(2)
gx.SetPoint(ibin, zpos, dx)
gy.SetPoint(ibin, zpos, dy)
ut.set_graph(gx, rt.kBlue)
ut.set_graph(gy, rt.kRed)
can = ut.box_canvas()
frame = gPad.DrawFrame(-10e3, 0, 15.5e3, 600e-6)
gx.Draw("lsame")
gy.Draw("lsame")
gPad.SetGrid()
ut.invert_col(gPad)
can.SaveAs("01fig.pdf")
def make_both():
lqmin = -11
lqmax = 5
ymax = 8.5
gQr = make_qr()
gPy = make_py()
gQr10x100 = make_qr_10x100()
gQr5x41 = make_qr_5x41()
can = ut.box_canvas()
frame = gPad.DrawFrame(lqmin, 0, lqmax, ymax)
frame.Draw()
xtit = "log_{10}(#it{Q}^{2})"
ytit = "#frac{d#it{#sigma}}{d(" + xtit + ")} (#mub/GeV^{2})"
ut.put_yx_tit(frame, ytit, xtit, 1.6, 1.3)
ut.set_margin_lbtr(gPad, 0.14, 0.1, 0.03, 0.02)
gQr.Draw("lsame")
gPy.Draw("lsame")
gQr10x100.Draw("lsame")
gQr5x41.Draw("lsame")
leg = ut.prepare_leg(0.53, 0.83, 0.2, 0.1, 0.035)
leg.AddEntry(gPy, "Pythia6", "l")
leg.AddEntry(gQr, "Quasi-real photoproduction", "l")
leg.AddEntry(gQr10x100, "Quasi-real 10x100", "l")
leg.Draw("same")
ut.invert_col(rt.gPad)
can.SaveAs("01fig.pdf")
def drawrange(x, y, xtit="", ytit=""):
if type(x) != type([]):
if xtit == "":
xtit = x.GetXaxis().GetTitle()
x = [x.GetXaxis().GetBinLowEdge(1), x.GetXaxis().GetBinUpEdge(x.GetNbinsX())]
ldrawn.append(gPad.DrawFrame(x[0], y[0], x[1], y[1], ";" + xtit + ";" + ytit))
ldrawn[-1].GetYaxis().CenterTitle()
def evt_Log10_Q2_ecal_compare():
#compare log_10(Q^2) from ecal for two separate inputs
infile1 = "../data/ir6/lmon_pythia_5M_beff2_5Mevt_v2.root"
#infile2 = "../data/ir6_close/lmon_pythia_5M_beff2_close_5Mevt.root"
#infile2 = "../data/ir6/lmon_pythia_5M_beff2_1p5T_5Mevt.root"
infile2 = "../data/ir6/lmon_pythia_5M_beff2_1p5T_5Mevt_v2.root"
lqbin = 5e-2
lqmin = -2.5
lqmax = 2.5
inp1 = TFile.Open(infile1)
inp2 = TFile.Open(infile2)
tree1 = inp1.Get("DetectorTree")
tree2 = inp2.Get("DetectorTree")
hQ2ecal = ut.prepare_TH1D("hQ2ecal", lqbin, lqmin, lqmax)
hQ2ecal_close = ut.prepare_TH1D("hQ2ecal_close", lqbin, lqmin, lqmax)
tree1.Draw(gL10Q2 + " >> hQ2ecal", "ecal_IsHit==1")
tree2.Draw(gL10Q2 + " >> hQ2ecal_close", "ecal_IsHit==1")
print "All events:", hQ2ecal.GetEntries()
#print "Selected :", hLog10Q2Tag.GetEntries()
can = ut.box_canvas()
frame = gPad.DrawFrame(lqmin, 10, lqmax, 1e5)
frame.Draw()
ytit = "Events / {0:.3f}".format(lqbin)
ut.put_yx_tit(frame, ytit, "log_{10}(#it{Q}^{2})", 1.4, 1.2)
ut.set_margin_lbtr(gPad, 0.1, 0.1, 0.03, 0.02)
ut.line_h1(hQ2ecal, rt.kBlue, 3)
ut.line_h1(hQ2ecal_close, rt.kRed, 3)
#hQ2ecal.SetMinimum(10)
gPad.SetLogy()
gPad.SetGrid()
hQ2ecal.Draw("e1same")
hQ2ecal_close.Draw("e1same")
#hLog10Q2.SetMaximum(2e5) # for qr
leg = ut.prepare_leg(0.6, 0.83, 0.2, 0.1, 0.035)
#leg.AddEntry(hLog10Q2, "All electrons from quasi-real photoproduction", "l")
#leg.AddEntry(hLog10Q2, "All Pythia6 scattered electrons", "l")
#leg.AddEntry(hLog10Q2Tag, "Electrons hitting the tagger", "l")
leg.AddEntry(hQ2ecal, "Default geometry", "l")
#leg.AddEntry(hQ2ecal_close, "Magnets in central det", "l")
leg.AddEntry(hQ2ecal_close, "1.5T solenoid", "l")
leg.Draw("same")
#ut.invert_col(rt.gPad)
can.SaveAs("01fig.pdf")
def eta():
#acceptance in electron polar angle as pi - theta in mrad
i1 = "/home/jaroslav/sim/lmon/data/taggers/tag1a/hits_tag.root"
i2 = "/home/jaroslav/sim/lmon/data/taggers/tag1ax1/hits_tag.root"
#tag = ["s1_IsHit", "Tagger 1", 0.15]
tag = ["s2_IsHit", "Tagger 2", 0.3]
in1 = TFile.Open(i1)
t1 = in1.Get("event")
in2 = TFile.Open(i2)
t2 = in2.Get("event")
#eta
xmin = -17
xmax = -3
a1 = rt.acc_Q2_kine(t1, "true_el_theta", tag[0])
a1.modif = 0 # eta from theta
a1.prec = 0.01
a1.bmin = 0.1
#a1.nev = int(1e5)
g1 = a1.get()
a2 = rt.acc_Q2_kine(t2, "true_el_theta", tag[0])
a2.modif = 0 # eta from theta
a2.prec = 0.01
a2.bmin = 0.1
#a2.nev = int(1e5)
g2 = a2.get()
can = ut.box_canvas()
frame = gPad.DrawFrame(xmin, 0, xmax, tag[2])
ut.put_yx_tit(frame, "Tagger acceptance",
"Electron pseudorapidity #it{#eta}", 1.6, 1.3)
frame.Draw()
ut.set_margin_lbtr(gPad, 0.11, 0.1, 0.03, 0.02)
ut.set_graph(g1, rt.kRed)
g1.Draw("psame")
ut.set_graph(g2, rt.kBlue)
g2.Draw("psame")
gPad.SetGrid()
leg = ut.prepare_leg(0.15, 0.8, 0.24, 0.14, 0.035) # x, y, dx, dy, tsiz
leg.AddEntry("", tag[1], "")
leg.AddEntry(g1, "Quasi-real photoproduction", "lp")
leg.AddEntry(g2, "Pythia 6", "lp")
leg.Draw("same")
#ut.invert_col(rt.gPad)
can.SaveAs("01fig.pdf")
def energy():
#acceptance in electron energy
i1 = "/home/jaroslav/sim/lmon/data/taggers/tag1a/hits_tag.root"
i2 = "/home/jaroslav/sim/lmon/data/taggers/tag1ax1/hits_tag.root"
#tag = ["s1_IsHit", "Tagger 1", 2]
tag = ["s2_IsHit", "Tagger 2", 11]
in1 = TFile.Open(i1)
t1 = in1.Get("event")
in2 = TFile.Open(i2)
t2 = in2.Get("event")
#mrad
xmin = tag[2]
xmax = 19
amax = 0.9
a1 = rt.acc_Q2_kine(t1, "true_el_E", tag[0])
a1.prec = 0.05
a1.bmin = 0.1
#a1.nev = int(1e5)
g1 = a1.get()
a2 = rt.acc_Q2_kine(t2, "true_el_E", tag[0])
a2.prec = 0.05
a2.bmin = 0.1
#a2.nev = int(1e5)
g2 = a2.get()
can = ut.box_canvas()
frame = gPad.DrawFrame(xmin, 0, xmax, amax)
ut.put_yx_tit(frame, "Tagger acceptance", "Electron energy #it{E} (GeV)",
1.6, 1.3)
frame.Draw()
ut.set_margin_lbtr(gPad, 0.11, 0.1, 0.03, 0.02)
ut.set_graph(g1, rt.kRed)
g1.Draw("psame")
ut.set_graph(g2, rt.kBlue)
g2.Draw("psame")
gPad.SetGrid()
leg = ut.prepare_leg(0.15, 0.8, 0.24, 0.14, 0.035) # x, y, dx, dy, tsiz
leg.AddEntry("", tag[1], "")
leg.AddEntry(g1, "Quasi-real photoproduction", "lp")
leg.AddEntry(g2, "Pythia 6", "lp")
leg.Draw("same")
#ut.invert_col(rt.gPad)
can.SaveAs("01fig.pdf")
def acc_mlt_theta_s12():
#acceptance in electron polar angle as -log10(pi - theta) in mrad for tagger 1 and tagger 2
#inp = "/home/jaroslav/sim/lmon/data/taggers/tag1a/hits_tag.root"
#inp = "/home/jaroslav/sim/lmon/data/taggers/tag1ax1/hits_tag.root"
inp = "/home/jaroslav/sim/lmon/data/taggers/tag2a/hits_tag_10files.root"
infile = TFile.Open(inp)
tree = infile.Get("event")
#mrad
tmin = 1.5
tmax = 7.5
#amax = 0.3
amax = 1
as1 = rt.acc_Q2_kine(tree, "true_el_theta", "s1_IsHit")
as1.modif = 3 # -log10(pi - theta)
as1.prec = 0.05
as1.bmin = 0.1
#as1.nev = int(1e5)
gs1 = as1.get()
as2 = rt.acc_Q2_kine(tree, "true_el_theta", "s2_IsHit")
as2.modif = 3 # -log10(pi - theta)
as2.prec = 0.05
as2.bmin = 0.1
#as2.nev = int(1e5)
gs2 = as2.get()
can = ut.box_canvas()
frame = gPad.DrawFrame(tmin, 0, tmax, amax)
ut.put_yx_tit(frame, "Acceptance", "Electron -log_{10}(#pi - #it{#theta}_{e})", 1.6, 1.3)
frame.Draw()
ut.set_margin_lbtr(gPad, 0.11, 0.1, 0.03, 0.02)
ut.set_graph(gs1, rt.kBlue)
gs1.Draw("psame")
ut.set_graph(gs2, rt.kRed)
gs2.Draw("psame")
gPad.SetGrid()
#leg = ut.prepare_leg(0.15, 0.78, 0.24, 0.16, 0.035) # x, y, dx, dy, tsiz
#leg.AddEntry(None, "Tagger 1", "")
#leg.AddEntry(glQ2Py, "Pythia6", "l")
#leg.AddEntry(glQ2Qr, "QR", "l")
#leg.Draw("same")
ut.invert_col(rt.gPad)
can.SaveAs("01fig.pdf")
def acc_gap_both():
#acceptance in gap between taggers and ecal
lqmin = -2.9
lqmax = -0.2
#lqmin = -8
#lqmax = 3
acc_py = acc_gap("../data/ir6/lmon_pythia_5M_beff2_5Mevt_v2.root", lqmin, lqmax)
#acc_py = acc_gap("../data/ir6/lmon_pythia_5M_beff2_NoSol_5Mevt.root", lqmin, lqmax)
#acc_py_close = acc_gap("../data/ir6_close/lmon_pythia_5M_beff2_close_5Mevt.root", -2.4, 0)
#acc_py_close = acc_gap("../data/ir6/lmon_pythia_5M_beff2_1p5T_5Mevt.root", -2.9, -0.2)
acc_py_close = acc_gap("../data/ir6/lmon_pythia_5M_beff2_1p5T_5Mevt_v2.root", lqmin, lqmax)
#acc_py_close = acc_gap("../data/ir6/lmon_pythia_5M_beff2_5Mevt_v2.root", lqmin, lqmax)
#acc_py_close = acc_gap("../data/ir6/lmon_pythia_5M_beff2_NoSol_5Mevt_v2.root", lqmin, lqmax)
#acc_py_3 = acc_gap("../data/ir6/lmon_pythia_5M_beff2_NoSol_5Mevt.root", lqmin, lqmax)
#make the plot
can = ut.box_canvas()
ut.set_graph(acc_py, rt.kBlue)
ut.set_graph(acc_py_close, rt.kRed)
#ut.set_graph(acc_py_3, rt.kGreen)
#frame = gPad.DrawFrame(-3, 0, 0.1, 1.1)
frame = gPad.DrawFrame(-3, 0.03, 0.1, 1.4) # for log scale
#frame = gPad.DrawFrame(-10, 0, 4, 1.1)
frame.Draw()
#ytit = "Acceptance / {0:.1f} %".format(prec*100)
ut.put_yx_tit(frame, "Acceptance", "log_{10}(#it{Q}^{2})", 1.6, 1.2)
frame.Draw()
ut.set_margin_lbtr(gPad, 0.11, 0.1, 0.03, 0.02)
gPad.SetGrid()
gPad.SetLogy()
frame.GetYaxis().SetMoreLogLabels()
acc_py.Draw("psame")
acc_py_close.Draw("psame")
#acc_py_3.Draw("psame")
leg = ut.prepare_leg(0.2, 0.84, 0.2, 0.1, 0.035)
#leg.AddEntry(acc_qr, "Quasi-real photoproduction", "lp")
#leg.AddEntry(acc_py, "Pythia6", "lp")
leg.AddEntry(acc_py, "Default geometry", "lp")
#leg.AddEntry(acc_py_close, "Magnets in central det", "lp")
leg.AddEntry(acc_py_close, "1.5T solenoid", "lp")
#leg.AddEntry(acc_py_3, "No solenoid", "lp")
leg.Draw("same")
#ut.invert_col(rt.gPad)
can.SaveAs("01fig.pdf")
def plot_dSigDe_all():
# dSigma / dEgamma over all energies, ZEUS parametrization
parse = ConfigParser.RawConfigParser()
parse.add_section("main")
parse.set("main", "emin", "0.1") # GeV
parse.set("main", "Ee", "18")
parse.set("main", "Ep", "275")
sig_top = gen_zeus(parse).dSigDe
parse.set("main", "Ee", "10")
parse.set("main", "Ep", "110")
sig_mid = gen_zeus(parse).dSigDe
parse.set("main", "Ee", "5")
parse.set("main", "Ep", "41")
sig_low = gen_zeus(parse).dSigDe
gStyle.SetPadTickY(1)
can = ut.box_canvas()
frame = gPad.DrawFrame(0.1, 1, 19, 80)
frame.Draw()
ut.set_F1(sig_top)
ut.set_F1(sig_mid, rt.kYellow + 1)
ut.set_F1(sig_low, rt.kBlue)
sig_top.Draw("same")
sig_mid.Draw("same")
sig_low.Draw("same")
ytit = "d#sigma / d#it{E}_{#gamma} (mb/GeV)"
xtit = "#it{E}_{#gamma} (GeV)"
ut.put_yx_tit(frame, ytit, xtit, 1.6, 1.4)
ut.set_margin_lbtr(gPad, 0.12, 0.1, 0.01, 0.01)
frame.GetYaxis().SetMoreLogLabels()
leg = ut.prepare_leg(0.65, 0.77, 0.24, 0.16, 0.035) # x, y, dx, dy, tsiz
leg.AddEntry(sig_top, "18 #times 275 GeV", "l")
leg.AddEntry(sig_mid, "10 #times 100 GeV", "l")
leg.AddEntry(sig_low, "5 #times 41 GeV", "l")
leg.Draw("same")
gPad.SetLogy()
gPad.SetGrid()
ut.invert_col(gPad)
can.SaveAs("01fig.pdf")
def acc_eta_s2():
#Tagger 2 pseudorapidity
emin = -17
emax = -3
amax = 0.3
acc_qr = rt.acc_Q2_kine(tree_qr, "true_el_theta", "lowQ2s2_IsHit")
acc_qr.modif = 0 # eta from theta
acc_qr.prec = 0.01
acc_qr.bmin = 0.1
#acc_qr.nev = int(1e5)
gEtaQr = acc_qr.get()
#gprint(gPtQr)
acc_py = rt.acc_Q2_kine(tree_py, "true_el_theta", "lowQ2s2_IsHit")
acc_py.modif = 0
acc_py.prec = 0.01
acc_py.bmin = 0.1
#acc_py.nev = int(1e5)
gEtaPy = acc_py.get()
can = ut.box_canvas()
frame = gPad.DrawFrame(emin, 0, emax, amax)
#ytit = "Acceptance / {0:.1f} %".format(acc_qr.prec*100)
ut.put_yx_tit(frame, "Acceptance", "Electron pseudorapidity #eta", 1.6,
1.3)
frame.Draw()
ut.set_margin_lbtr(gPad, 0.11, 0.1, 0.03, 0.02)
ut.set_graph(gEtaQr, rt.kRed)
gEtaQr.Draw("psame")
ut.set_graph(gEtaPy, rt.kBlue)
gEtaPy.Draw("psame")
gPad.SetGrid()
leg = ut.prepare_leg(0.15, 0.78, 0.24, 0.16, 0.035) # x, y, dx, dy, tsiz
leg.AddEntry(None, "Tagger 2", "")
leg.AddEntry(gEtaPy, "Pythia6", "l")
leg.AddEntry(gEtaQr, "QR", "l")
leg.Draw("same")
#ut.invert_col(rt.gPad)
can.SaveAs("01fig.pdf")
def acc_eta_s12():
#acceptance in electron pseudorapidity for tagger 1 and tagger 2
inp = "/home/jaroslav/sim/lmon/data/taggers/tag1a/hits_tag.root"
infile = TFile.Open(inp)
tree = infile.Get("event")
emin = -17
emax = -3
amax = 0.3
as1 = rt.acc_Q2_kine(tree, "true_el_theta", "s1_IsHit")
as1.modif = 0 # eta from theta
as1.prec = 0.01
as1.bmin = 0.1
#as1.nev = int(1e5)
gs1 = as1.get()
as2 = rt.acc_Q2_kine(tree, "true_el_theta", "s2_IsHit")
as2.modif = 0 # eta from theta
as2.prec = 0.01
as2.bmin = 0.1
#as2.nev = int(1e5)
gs2 = as2.get()
can = ut.box_canvas()
frame = gPad.DrawFrame(emin, 0, emax, amax)
ut.put_yx_tit(frame, "Acceptance", "Electron pseudorapidity #eta", 1.6, 1.3)
frame.Draw()
ut.set_margin_lbtr(gPad, 0.11, 0.1, 0.03, 0.02)
ut.set_graph(gs1, rt.kBlue)
gs1.Draw("psame")
ut.set_graph(gs2, rt.kRed)
gs2.Draw("psame")
gPad.SetGrid()
#leg = ut.prepare_leg(0.15, 0.78, 0.24, 0.16, 0.035) # x, y, dx, dy, tsiz
#leg.AddEntry(None, "Tagger 1", "")
#leg.AddEntry(glQ2Py, "Pythia6", "l")
#leg.AddEntry(glQ2Qr, "QR", "l")
#leg.Draw("same")
ut.invert_col(rt.gPad)
can.SaveAs("01fig.pdf")
def el_eta_beff():
#electron pseudorapidity eta and angular divergence
xbin = 0.1
xmin = -20
xmax = 10
qrpy = 0
if qrpy == 0:
tree = tree_qr
lab_data = "QR"
col = rt.kBlue
else:
tree = tree_py
lab_data = "Pythia6"
col = rt.kRed
can = ut.box_canvas()
hE = ut.prepare_TH1D("hE", xbin, xmin, xmax)
hB = ut.prepare_TH1D("hB", xbin, xmin, xmax)
form = "-TMath::Log(TMath::Tan(true_el_theta/2.))"
form2 = "-TMath::Log(TMath::Tan(el_theta/2.))"
tree.Draw(form + " >> hE")
tree.Draw(form2 + " >> hB")
ut.line_h1(hE, col)
ut.line_h1(hB, rt.kViolet)
vmax = hB.GetMaximum() + 0.1 * hB.GetMaximum()
frame = gPad.DrawFrame(xmin, 0.5, xmax, vmax)
ut.put_yx_tit(frame, "Counts", "Electron #eta", 1.6, 1.3)
frame.Draw()
ut.set_margin_lbtr(gPad, 0.11, 0.1, 0.05, 0.02)
gPad.SetGrid()
#gPad.SetLogy()
hB.Draw("same")
hE.Draw("same")
leg = ut.prepare_leg(0.56, 0.8, 0.24, 0.12, 0.035) # x, y, dx, dy, tsiz
leg.AddEntry(hE, lab_data + ", no divergence", "l")
leg.AddEntry(hB, "Divergence included", "l")
leg.Draw("same")
#ut.invert_col(rt.gPad)
can.SaveAs("01fig.pdf")
def el_theta_beff():
#electron polar angle theta and effect of angular divergence
xbin = 5e-5
#xmin = TMath.Pi() - 2.2e-2
xmin = 3.13
xmax = TMath.Pi() + 0.2e-2
qrpy = 0
if qrpy == 0:
tree = tree_qr
lab_data = "QR"
col = rt.kBlue
else:
tree = tree_py
lab_data = "Pythia6"
col = rt.kRed
can = ut.box_canvas()
hT = ut.prepare_TH1D("hT", xbin, xmin, xmax)
hB = ut.prepare_TH1D("hB", xbin, xmin, xmax)
tree.Draw("true_el_theta >> hT")
tree.Draw("el_theta >> hB")
ut.line_h1(hT, col)
ut.line_h1(hB, rt.kViolet)
vmax = hT.GetMaximum() + 0.4 * hT.GetMaximum()
frame = gPad.DrawFrame(xmin, 1e3, xmax, vmax)
ut.put_yx_tit(frame, "Counts", "Electron #theta (rad)", 1.6, 1.3)
frame.Draw()
ut.set_margin_lbtr(gPad, 0.11, 0.1, 0.03, 0.02)
gPad.SetGrid()
gPad.SetLogy()
hB.Draw("same")
hT.Draw("same")
leg = ut.prepare_leg(0.14, 0.8, 0.24, 0.12, 0.035) # x, y, dx, dy, tsiz
leg.AddEntry(hT, lab_data + ", no divergence", "l")
leg.AddEntry(hB, "Divergence included", "l")
leg.Draw("same")
#ut.invert_col(rt.gPad)
can.SaveAs("01fig.pdf")
def acc_theta_s12():
#acceptance in electron polar angle for tagger 1 and tagger 2
inp = "/home/jaroslav/sim/lmon/data/taggers/tag1a/hits_tag.root"
#inp = "/home/jaroslav/sim/lmon/data/taggers/tag1ax1/hits_tag.root"
infile = TFile.Open(inp)
tree = infile.Get("event")
tmin = TMath.Pi() - 1.1e-2
tmax = TMath.Pi() + 1e-3
#amax = 0.25
amax = 0.4
as1 = rt.acc_Q2_kine(tree, "true_el_theta", "s1_IsHit")
as1.prec = 0.1
as1.bmin = 2e-4
#as1.nev = int(1e5)
gs1 = as1.get()
as2 = rt.acc_Q2_kine(tree, "true_el_theta", "s2_IsHit")
as2.prec = 0.1
as2.bmin = 2e-4
#as2.nev = int(1e5)
gs2 = as2.get()
can = ut.box_canvas()
frame = gPad.DrawFrame(tmin, 0, tmax, amax)
ut.put_yx_tit(frame, "Tagger acceptance", "Electron polar angle #it{#theta} (rad)", 1.6, 1.3)
frame.Draw()
ut.set_margin_lbtr(gPad, 0.11, 0.1, 0.03, 0.02)
ut.set_graph(gs1, rt.kRed)
gs1.Draw("psame")
ut.set_graph(gs2, rt.kBlue)
gs2.Draw("psame")
gPad.SetGrid()
leg = ut.prepare_leg(0.15, 0.82, 0.24, 0.12, 0.035) # x, y, dx, dy, tsiz
leg.AddEntry(gs1, "Tagger 1", "lp")
leg.AddEntry(gs2, "Tagger 2", "lp")
leg.Draw("same")
ut.invert_col(rt.gPad)
can.SaveAs("01fig.pdf")
def acc_en_s1():
#Tagger 1 energy
emin = 0
emax = 15
amax = 1
acc_qr = rt.acc_Q2_kine(tree_qr, "true_el_E", "lowQ2s1_IsHit")
acc_qr.prec = 0.05
acc_qr.bmin = 0.1
#acc_qr.nev = int(1e5)
gEnQr = acc_qr.get()
#gprint(gPtQr)
acc_py = rt.acc_Q2_kine(tree_py, "true_el_E", "lowQ2s1_IsHit")
acc_py.prec = 0.05
acc_py.bmin = 0.1
#acc_py.nev = int(1e5)
gEnPy = acc_py.get()
can = ut.box_canvas()
frame = gPad.DrawFrame(emin, 0, emax, amax)
#ytit = "Acceptance / {0:.1f} %".format(acc_qr.prec*100)
ut.put_yx_tit(frame, "Acceptance", "Electron energy #it{E} (GeV)", 1.6,
1.3)
frame.Draw()
ut.set_margin_lbtr(gPad, 0.11, 0.1, 0.03, 0.02)
ut.set_graph(gEnQr, rt.kRed)
gEnQr.Draw("psame")
ut.set_graph(gEnPy, rt.kBlue)
gEnPy.Draw("psame")
gPad.SetGrid()
leg = ut.prepare_leg(0.15, 0.78, 0.24, 0.16, 0.035) # x, y, dx, dy, tsiz
leg.AddEntry(None, "Tagger 1", "")
leg.AddEntry(gEnPy, "Pythia6", "l")
leg.AddEntry(gEnQr, "QR", "l")
leg.Draw("same")
ut.invert_col(rt.gPad)
can.SaveAs("01fig.pdf")
def el_phi_beff():
#electron azimuthal angle phi
xbin = 3e-2
xmin = -TMath.Pi() - 0.3
xmax = TMath.Pi() + 0.3
qrpy = 0
if qrpy == 0:
tree = tree_qr
lab_data = "QR"
col = rt.kBlue
else:
tree = tree_py
lab_data = "Pythia6"
col = rt.kRed
can = ut.box_canvas()
hP = ut.prepare_TH1D("hP", xbin, xmin, xmax)
hB = ut.prepare_TH1D("hB", xbin, xmin, xmax)
tree.Draw("true_el_phi >> hP")
tree.Draw("el_phi >> hB")
ut.line_h1(hP, col)
ut.line_h1(hB, rt.kViolet)
vmax = hP.GetMaximum() + 0.5 * hP.GetMaximum()
frame = gPad.DrawFrame(xmin, 0.5, xmax, vmax)
ut.put_yx_tit(frame, "Counts", "Electron #phi (rad)", 1.6, 1.3)
frame.Draw()
ut.set_margin_lbtr(gPad, 0.11, 0.1, 0.05, 0.02)
gPad.SetGrid()
#gPad.SetLogy()
hB.Draw("same")
hP.Draw("same")
leg = ut.prepare_leg(0.55, 0.8, 0.24, 0.12, 0.035) # x, y, dx, dy, tsiz
leg.AddEntry(hP, lab_data + ", no divergence", "l")
leg.AddEntry(hB, "Divergence included", "l")
leg.Draw("same")
#ut.invert_col(rt.gPad)
can.SaveAs("01fig.pdf")
def acc_phi_s2():
#Tagger 2 phi
pmin = -TMath.Pi() - 0.3
pmax = TMath.Pi() + 0.3
amax = 0.3
acc_qr = rt.acc_Q2_kine(tree_qr, "true_el_phi", "lowQ2s2_IsHit")
acc_qr.prec = 0.01
#acc_qr.bmin = 2e-4
#acc_qr.nev = int(1e5)
gPhiQr = acc_qr.get()
#gprint(gPtQr)
acc_py = rt.acc_Q2_kine(tree_py, "true_el_phi", "lowQ2s2_IsHit")
acc_py.prec = 0.01
#acc_py.bmin = 2e-4
#acc_py.nev = int(1e4)
gPhiPy = acc_py.get()
can = ut.box_canvas()
frame = gPad.DrawFrame(pmin, 0, pmax, amax)
#ytit = "Acceptance / {0:.1f} %".format(acc_qr.prec*100)
ut.put_yx_tit(frame, "Acceptance", "Electron azimuthal angle #phi (rad)",
1.6, 1.3)
frame.Draw()
ut.set_margin_lbtr(gPad, 0.11, 0.1, 0.03, 0.02)
ut.set_graph(gPhiQr, rt.kRed)
gPhiQr.Draw("psame")
ut.set_graph(gPhiPy, rt.kBlue)
gPhiPy.Draw("psame")
gPad.SetGrid()
leg = ut.prepare_leg(0.72, 0.78, 0.24, 0.16, 0.035) # x, y, dx, dy, tsiz
leg.AddEntry(None, "Tagger 2", "")
leg.AddEntry(gPhiPy, "Pythia6", "l")
leg.AddEntry(gPhiQr, "QR", "l")
leg.Draw("same")
#ut.invert_col(rt.gPad)
can.SaveAs("01fig.pdf")
def conv_theta():
#conversion probablity as a function of polar angle theta
tbin = 2e-4
tmin = 0
tmax = 2.5e-3
prec = 0.01
delt = 1e-6
gROOT.LoadMacro("get_ew_conv.C")
#hEffV1 = rt.get_ew_conv(tree_v1, "phot_theta", "ew_conv", prec, delt, -1., TMath.Pi())
hEffV2 = rt.get_ew_conv(tree_v2, "phot_theta", "ew_conv", prec, delt, -1.,
TMath.Pi())
#hEffV1 = get_eff(tree_v1, "TMath::Pi()-phot_theta", "ew_conv", tbin, tmin, tmax)
#hEffV2 = get_eff(tree_v2, "TMath::Pi()-phot_theta", "ew_conv", tbin, tmin, tmax)
#ut.set_graph(hEffV1, rt.kBlue)
#ut.set_graph(hEffV2, rt.kRed, rt.kFullTriangleUp)
#hEffV2.SetMarkerSize(1.5)
ut.set_graph(hEffV2)
#plot the probability
can = ut.box_canvas()
frame = gPad.DrawFrame(tmin, 0.065, tmax, 0.095)
frame.SetXTitle("Generated #vartheta (rad)")
frame.SetYTitle("Conversion probability")
frame.SetTitleOffset(2.1, "Y")
frame.SetTitleOffset(1.5, "X")
ut.set_margin_lbtr(gPad, 0.14, 0.11, 0.02, 0.01)
frame.Draw()
#hEffV1.Draw("psame")
hEffV2.Draw("psame")
leg = ut.prepare_leg(0.2, 0.84, 0.2, 0.1, 0.035)
#leg.AddEntry(hEffV1, "Tilted plane", "lp")
leg.AddEntry(hEffV2, "Half-cylinder", "lp")
#leg.Draw("same")
gPad.SetLogx()
#ut.invert_col(rt.gPad)
can.SaveAs("01fig.pdf")
def acc_theta_s1():
tmin = TMath.Pi() - 2.1e-2
tmax = TMath.Pi() + 0.5e-2
amax = 0.08
acc_qr = rt.acc_Q2_kine(tree_qr, "true_el_theta", "lowQ2s1_IsHit")
acc_qr.prec = 0.05
acc_qr.bmin = 2e-4
#acc_qr.nev = int(1e5)
gThetaQr = acc_qr.get()
#gprint(gPtQr)
acc_py = rt.acc_Q2_kine(tree_py, "true_el_theta", "lowQ2s1_IsHit")
acc_py.prec = 0.05
acc_py.bmin = 2e-4
#acc_py.nev = int(1e4)
gThetaPy = acc_py.get()
can = ut.box_canvas()
frame = gPad.DrawFrame(tmin, 0, tmax, amax)
#ytit = "Acceptance / {0:.1f} %".format(acc_qr.prec*100)
ut.put_yx_tit(frame, "Acceptance", "Electron polar angle #theta (rad)",
1.6, 1.3)
frame.Draw()
ut.set_margin_lbtr(gPad, 0.11, 0.1, 0.03, 0.02)
ut.set_graph(gThetaQr, rt.kRed)
gThetaQr.Draw("psame")
ut.set_graph(gThetaPy, rt.kBlue)
gThetaPy.Draw("psame")
gPad.SetGrid()
leg = ut.prepare_leg(0.15, 0.78, 0.24, 0.16, 0.035) # x, y, dx, dy, tsiz
leg.AddEntry(None, "Tagger 1", "")
leg.AddEntry(gThetaPy, "Pythia6", "l")
leg.AddEntry(gThetaQr, "QR", "l")
leg.Draw("same")
ut.invert_col(rt.gPad)
can.SaveAs("01fig.pdf")
def acc_lQ2_s2():
#Tagger 2 log_10(Q^2)
lQ2min = -10
lQ2max = 0
amax = 0.3
acc_qr = rt.acc_Q2_kine(tree_qr, "true_Q2", "lowQ2s2_IsHit")
acc_qr.modif = 1 # log_10(Q^2) from Q2
acc_qr.prec = 0.05
acc_qr.bmin = 0.1
#acc_qr.nev = int(1e5)
glQ2Qr = acc_qr.get()
acc_py = rt.acc_Q2_kine(tree_py, "true_Q2", "lowQ2s2_IsHit")
acc_py.modif = 1
acc_py.prec = 0.05
acc_py.bmin = 0.1
#acc_py.nev = int(1e5)
glQ2Py = acc_py.get()
can = ut.box_canvas()
frame = gPad.DrawFrame(lQ2min, 0, lQ2max, amax)
ut.put_yx_tit(frame, "Acceptance", "Virtuality log_{10}(#it{Q}^{2}) (GeV)",
1.6, 1.3)
frame.Draw()
ut.set_margin_lbtr(gPad, 0.11, 0.1, 0.03, 0.02)
ut.set_graph(glQ2Qr, rt.kRed)
glQ2Qr.Draw("psame")
ut.set_graph(glQ2Py, rt.kBlue)
glQ2Py.Draw("psame")
gPad.SetGrid()
leg = ut.prepare_leg(0.15, 0.78, 0.24, 0.16, 0.035) # x, y, dx, dy, tsiz
leg.AddEntry(None, "Tagger 2", "")
leg.AddEntry(glQ2Py, "Pythia6", "l")
leg.AddEntry(glQ2Qr, "QR", "l")
leg.Draw("same")
ut.invert_col(rt.gPad)
can.SaveAs("01fig.pdf")
def conv_phi():
#conversion probablity as a function of azimuthal angle phi
pbin = 0.4
pmin = -TMath.Pi() - 0.3
pmax = TMath.Pi() + 0.3
prec = 0.01
delt = 1e-6
gROOT.LoadMacro("get_ew_conv.C")
#hEffV1 = rt.get_ew_conv(tree_v1, "phot_phi", "ew_conv", prec, delt)
hEffV2 = rt.get_ew_conv(tree_v2, "phot_phi", "ew_conv", prec, delt)
#hEffV1 = get_eff(tree_v1, "phot_phi", "ew_conv", pbin, pmin, pmax)
#hEffV2 = get_eff(tree_v2, "phot_phi", "ew_conv", pbin, pmin, pmax)
#ut.set_graph(hEffV1, rt.kBlue)
#ut.set_graph(hEffV2, rt.kRed, rt.kFullTriangleUp)
#hEffV2.SetMarkerSize(1.5)
ut.set_graph(hEffV2)
#plot the probability
can = ut.box_canvas()
#frame = gPad.DrawFrame(pmin, 0.075, pmax, 0.087)
frame = gPad.DrawFrame(pmin, 0.065, pmax, 0.095)
frame.SetXTitle("Generated #phi (rad)")
frame.SetYTitle("Conversion probability")
frame.SetTitleOffset(2.1, "Y")
frame.SetTitleOffset(1.2, "X")
ut.set_margin_lbtr(gPad, 0.14, 0.09, 0.02, 0.01)
frame.Draw()
#hEffV1.Draw("psame")
hEffV2.Draw("psame")
leg = ut.prepare_leg(0.2, 0.84, 0.2, 0.1, 0.035)
#leg.AddEntry(hEffV1, "Tilted plane", "lp")
leg.AddEntry(hEffV2, "Half-cylinder", "lp")
#leg.Draw("same")
#ut.invert_col(rt.gPad)
can.SaveAs("01fig.pdf")
def sigma_en():
#cross section as a function of electron energy
emin = 0 # GeV
emax = 24
smin = 1e-4
smax = 1e3 # mb
ebin = 0.2
basedir = "/home/jaroslav/sim/GETaLM_data"
g1 = make_sigma(basedir+"/lumi/lumi_18x275_Lif_emin0p5_T3p3_10Mevt.root", "true_el_E", 0.1, emin, emax, 171.3)
g2 = make_sigma(basedir+"/qr/qr_18x275_T3p3_5Mevt.root", "true_el_E", ebin, emin, emax, 0.053)
g3 = make_sigma(basedir+"/py/pythia_ep_18x275_Q2all_beff2_5Mevt.root", "true_el_E", ebin, emin, emax, 0.055)
can = ut.box_canvas()
frame = gPad.DrawFrame(emin, smin, emax, smax)
frame.Draw()
xtit = "#it{E_{e}}' (GeV)"
ytit = "#frac{d#it{#sigma}}{d#it{E_{e}}'} (mb/GeV)"
ut.put_yx_tit(frame, ytit, xtit, 1.6, 1.3)
ut.set_margin_lbtr(gPad, 0.14, 0.1, 0.02, 0.02)
g1.SetLineColor(rt.kBlue)
g2.SetLineColor(rt.kRed)
g3.SetLineColor(rt.kGreen+1)
g3.SetLineStyle(rt.kDashed)
g1.Draw("lsame")
g2.Draw("lsame")
g3.Draw("lsame")
gPad.SetLogy()
gPad.SetGrid()
leg = ut.prepare_leg(0.2, 0.75, 0.24, 0.15, 0.035) # x, y, dx, dy, tsiz
leg.AddEntry(g1, "Bremsstrahlung", "l")
leg.AddEntry(g2, "Quasi-real", "l")
leg.AddEntry(g3, "Pythia6", "l")
leg.Draw("same")
#ut.invert_col(rt.gPad)
can.SaveAs("01fig.pdf")
def plot_dSigDe():
# dSigma / dEgamma according to ZEUS parametrization
parse = ConfigParser.RawConfigParser()
parse.add_section("main")
parse.set("main", "emin", "6")
parse.set("main", "Ee", "18")
parse.set("main", "Ep", "275")
gen = gen_zeus(parse)
sig = gen.dSigDe
gStyle.SetPadTickY(1)
can = ut.box_canvas()
#frame = gPad.DrawFrame(6, 0, 29, 6)
frame = gPad.DrawFrame(5, 0, 19, 7.2)
sig.SetLineWidth(3)
sig.SetNpx(1000)
sig.SetTitle("")
sig.Draw("same")
frame.GetXaxis().SetTitle("#it{E}_{#gamma} (GeV)")
frame.GetYaxis().SetTitle("d#sigma / d#it{E}_{#gamma} (mb/GeV)")
frame.GetYaxis().SetTitleOffset(1.1)
frame.GetXaxis().SetTitleOffset(1.3)
frame.SetTickLength(0.015, "X")
frame.SetTickLength(0.015, "Y")
gPad.SetTopMargin(0.02)
gPad.SetRightMargin(0.01)
gPad.SetLeftMargin(0.09)
leg = ut.prepare_leg(0.65, 0.73, 0.24, 0.2, 0.035) # x, y, dx, dy, tsiz
leg.AddEntry(sig, "#frac{d#sigma}{d#it{E}_{#gamma}}", "l")
leg.AddEntry(None, "", "")
#leg.AddEntry(None, "#it{E}_{e} = 27.6 GeV", "")
#leg.AddEntry(None, "#it{E}_{p} = 920 GeV", "")
leg.AddEntry(None, "#it{E}_{e} = 18 GeV", "")
leg.AddEntry(None, "#it{E}_{p} = 275 GeV", "")
leg.Draw("same")
ut.invert_col(gPad)
can.SaveAs("01fig.pdf")
def sigma_pitheta():
#cross section as a function of electron scattering angle as pi - theta in mrad
tmin = 0 # mrad
tmax = 25
smin = 1e-4
smax = 2e3 # mb
basedir = "/home/jaroslav/sim/GETaLM_data"
form = "(TMath::Pi()-true_el_theta)*1e3"
g1 = make_sigma_2(basedir+"/lumi/lumi_18x275_Lif_emin0p5_T3p3_10Mevt.root", form, 0.2, tmin, tmax, 171.3, 5, 1.2)
g2 = make_sigma(basedir+"/qr/qr_18x275_T3p3_5Mevt.root", form, 0.2, tmin, tmax, 0.053)
g3 = make_sigma(basedir+"/py/pythia_ep_18x275_Q2all_beff2_5Mevt.root", form, 0.2, tmin, tmax, 0.055)
can = ut.box_canvas()
frame = gPad.DrawFrame(tmin, smin, tmax, smax)
frame.Draw()
xtit = "#it{#pi - #theta_{e}}' (mrad)"
ytit = "#frac{d#it{#sigma}}{d#it{#theta_{e}}'} (mb/mrad)"
ut.put_yx_tit(frame, ytit, xtit, 1.6, 1.3)
ut.set_margin_lbtr(gPad, 0.14, 0.1, 0.02, 0.02)
g1.SetLineColor(rt.kBlue)
g2.SetLineColor(rt.kRed)
g3.SetLineColor(rt.kGreen+1)
g3.SetLineStyle(rt.kDashed)
g1.Draw("lsame")
g2.Draw("lsame")
g3.Draw("lsame")
leg = ut.prepare_leg(0.6, 0.75, 0.24, 0.15, 0.035) # x, y, dx, dy, tsiz
leg.AddEntry(g1, "Bremsstrahlung", "l")
leg.AddEntry(g2, "Quasi-real", "l")
leg.AddEntry(g3, "Pythia6", "l")
leg.Draw("same")
gPad.SetLogy()
gPad.SetGrid()
#ut.invert_col(rt.gPad)
can.SaveAs("01fig.pdf")
def make_all_E():
lqmin = -11
lqmax = 5
smax = 7.5
basedir = "/home/jaroslav/sim/lgen/data"
#sigma in micro barn
#g18x275 = make_sigma(basedir+"/lgen_18x275_qr_Qe_beff2_5Mevt.root", 55.1)
#g10x100 = make_sigma(basedir+"/lgen_10x100_qr_5Mevt.root", 44.8)
#g5x41 = make_sigma(basedir+"/lgen_5x41_qr_5Mevt.root", 33.4)
g18x275 = make_sigma(basedir+"/lgen_py_18x275_Q2all_5Mevt.root", 54.7)
g10x100 = make_sigma(basedir+"/lgen_py_10x100_Q2all_5Mevt.root", 40.9)
g5x41 = make_sigma(basedir+"/lgen_py_5x41_Q2all_5Mevt.root", 28.4)
can = ut.box_canvas()
frame = gPad.DrawFrame(lqmin, 0, lqmax, smax)
frame.Draw()
xtit = "log_{10}(#it{Q}^{2})"
ytit = "#frac{d#it{#sigma}}{d("+xtit+")} (#mub/GeV^{2})"
ut.put_yx_tit(frame, ytit, xtit, 1.6, 1.3)
ut.set_margin_lbtr(gPad, 0.14, 0.1, 0.01, 0.01)
g18x275.SetLineColor(rt.kRed)
g10x100.SetLineColor(rt.kYellow+1)
g5x41.SetLineColor(rt.kBlue)
g18x275.Draw("lsame")
g10x100.Draw("lsame")
g5x41.Draw("lsame")
leg = ut.prepare_leg(0.72, 0.8, 0.24, 0.16, 0.035) # x, y, dx, dy, tsiz
leg.AddEntry(g18x275, "18 #times 275 GeV", "l")
leg.AddEntry(g10x100, "10 #times 100 GeV", "l")
leg.AddEntry(g5x41, "5 #times 41 GeV", "l")
leg.Draw("same")
gPad.SetGrid()
ut.invert_col(rt.gPad)
can.SaveAs("01fig.pdf")
def acc_pT_s2():
ptmin = 0
ptmax = 0.25
amax = 0.25
acc_qr = rt.acc_Q2_kine(tree_qr, "true_el_pT", "lowQ2s2_IsHit")
acc_qr.prec = 0.05
acc_qr.bmin = 0.003
#acc_qr.nev = int(1e5)
gPtQr = acc_qr.get()
acc_py = rt.acc_Q2_kine(tree_py, "true_el_pT", "lowQ2s2_IsHit")
acc_py.prec = 0.05
acc_py.bmin = 0.003
#acc_py.nev = int(1e4)
gPtPy = acc_py.get()
can = ut.box_canvas()
frame = gPad.DrawFrame(ptmin, 0, ptmax, amax)
#ytit = "Acceptance / {0:.1f} %".format(acc_qr.prec*100)
ut.put_yx_tit(frame, "Acceptance", "Electron #it{p}_{T} (GeV)", 1.6, 1.3)
frame.Draw()
ut.set_margin_lbtr(gPad, 0.11, 0.1, 0.03, 0.05)
ut.set_graph(gPtQr, rt.kRed)
gPtQr.Draw("psame")
ut.set_graph(gPtPy, rt.kBlue)
gPtPy.Draw("psame")
gPad.SetGrid()
leg = ut.prepare_leg(0.72, 0.78, 0.24, 0.16, 0.035) # x, y, dx, dy, tsiz
leg.AddEntry(None, "Tagger 2", "")
leg.AddEntry(gPtPy, "Pythia6", "l")
leg.AddEntry(gPtQr, "QR", "l")
leg.Draw("same")
#ut.invert_col(rt.gPad)
can.SaveAs("01fig.pdf")
def conv_prob_en():
#conversion probability as a function of photon energy
#plot range
emin = 0
emax = 19
pmin = 0.05
pmax = 0.1
#pmax = 1
inp = TFile.Open("ew.root")
tree = inp.Get("conv_tree")
prec = 0.01
calc = rt.conv_calc(prec, 1e-6)
calc.set_tree(tree)
#calc.nev = 300000
conv = calc.get_conv()
calc.release_tree()
#calc.conv_in_all = True
#calc.clean_in_sel = True
#clean = calc.get_conv()
can = ut.box_canvas()
frame = gPad.DrawFrame(emin, pmin, emax, pmax)
ut.put_yx_tit(frame, "Conversion probability", "#it{E}_{#gamma} (GeV)",
1.8)
ut.set_margin_lbtr(gPad, 0.12, 0.09, 0.02, 0.01)
frame.Draw()
gPad.SetGrid()
ut.set_graph(conv, rt.kBlue)
conv.Draw("psame")
#ut.set_graph(clean, rt.kRed)
#clean.Draw("psame")
ut.invert_col(rt.gPad)
can.SaveAs("01fig.pdf")
def pressure_func():
gen = make_gen()
#pressure function
pf = gen.pressure_func
ut.set_F1(pf, rt.kBlue)
can = ut.box_canvas()
frame = gPad.DrawFrame(-5.5e3, 0, 15.5e3, 7e-9)
pf.Draw("same")
gPad.SetGrid()
ut.invert_col(gPad)
can.SaveAs("01fig.pdf")
