# Difference: PhysicsResultsSUS19006PAS (1 vs. 28)

#### Revision 282019-09-09 - RishiPatel

Line: 1 to 1

 META TOPICPARENT name="PhysicsResultsSUS"

# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

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Line: 258 to 257

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Changed:
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#### Revision 272019-09-09 - RishiPatel

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# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

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#### Revision 262019-09-06 - WilliamFord

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 META TOPICPARENT name="PhysicsResultsSUS"

# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

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 Figure phoF : Distribution of with baseline selection applied in the 46 search bins with . Because of limited statistical precision in the simulated event samples at large , the transfer factors determined for the region are also used for the region. Points with error bars show the computed value in each bin with statistical uncertainties.
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 Figure Z1a : Distribution in for . Data appear as points with error bars, simulation as stacked histograms, with the data over simulation ratio in the lower panel. The red dashed line in the ratio plot denotes the sample average. Baseline selection is applied.

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 Figure Z1 : Double ratio vs. (left), (center), and Events in the simulated +jets sample have been weighted by the reciprocal of the -dependent function represented by the green dot-dashed line in the left-hand panel. The average value of this function is 0.95. Points with error bars show the value of in each bin with statistical uncertainties. The solid and dashed blue lines show the straight-line fit and uncertainties propagated from the fit, respectively. The average value, 1.00, is drawn as a red dashed line on each plot.
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 Figure Z1b : Distribution in for . Data appear as points with error bars, simulation as stacked histograms, with the data over simulation ratio in the lower panel. The red dashed line in the ratio plot denotes the sample average. Baseline selection is applied.

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 Figure Z2a : Representative dilepton mass distributions from the +jets control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (a) with , .
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 Figure Z1c : Distribution in for . Data appear as points with error bars, simulation as stacked histograms, with the data over simulation ratio in the lower panel. The red dashed line in the ratio plot denotes the sample average. Baseline selection is applied, except for and the of the Z-boson candidate, which are subject only to trigger and preselection requirements.

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 Figure Z2b : Representative dilepton mass distributions from the +jets control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (b) with , .
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 Figure Z1d : Distribution in for . Data appear as points with error bars, simulation as stacked histograms, with the data over simulation ratio in the lower panel. The red dashed line in the ratio plot denotes the sample average. Baseline selection is applied. Baseline selection is applied, except for and the of the Z-boson candidate, which are subject only to trigger and preselection requirements.

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 Figure Z2c : Representative dilepton mass distributions from the +jets control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (c) with , .
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 Figure Z1e : Distribution in for . Data appear as points with error bars, simulation as stacked histograms, with the data over simulation ratio in the lower panel. The red dashed line in the ratio plot denotes the sample average. Baseline selection is applied.

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 Figure Z2d : Representative dilepton mass distributions from the +jets control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (d) with , .
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 Figure Z1f : Distribution in for . Data appear as points with error bars, simulation as stacked histograms, with the data over simulation ratio in the lower panel. The red dashed line in the ratio plot denotes the sample average. Baseline selection is applied.

 Figure Z1g : Distribution in for . Data appear as points with error bars, simulation as stacked histograms, with the data over simulation ratio in the lower panel. The red dashed line in the ratio plot denotes the sample average. Baseline selection is applied.

 Figure Z1h : Distribution in for . Data appear as points with error bars, simulation as stacked histograms, with the data over simulation ratio in the lower panel. The red dashed line in the ratio plot denotes the sample average. Baseline selection is applied.

 Figure Z2 : Double ratio vs. (left), (center), and Events in the simulated +jets sample have been weighted by the reciprocal of the -dependent function represented by the green dot-dashed line in the left-hand panel. The average value of this function is 0.95. Points with error bars show the value of in each bin with statistical uncertainties. The solid and dashed blue lines show the straight-line fit and uncertainties propagated from the fit, respectively. The average value, 1.00, is drawn as a red dashed line on each plot.

 Figure Z3a : Representative dilepton mass distributions from the +jets control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (a) with , .

 Figure Z3b : Representative dilepton mass distributions from the +jets control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (b) with , .

 Figure Z3c : Representative dilepton mass distributions from the +jets control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (c) with , .

 Figure Z3d : Representative dilepton mass distributions from the +jets control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (d) with , .

 Figure BKa : Data driven background composition in zero-lepton signal region projected onto different bins in search variables , number of jets () and number of b-tagged jets (). Each pie-chart for a given search variable is inclusive in other three search variables with baseline selections applied.
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# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

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 Figure BKc : Data driven background composition in zero-lepton signal region projected onto two dimensional bins in search variables number of jets () and number of b-tagged jets (). These pie-charts are inclusive in , after selection 600 GeV and 600 GeV applied.
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 Figure LLa : Lost lepton background in signal region decomposed as that from ttbar, W+jets and Single top in different bins of , , number of jets () and number of b-tagged jets (). Each pie-chart for a given search variable is inclusive in other three search variables with baseline selections applied.
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 Figure LLa : Lost lepton background in signal region decomposed as that from ttbar, W+jets and Single top in different bins of , , number of jets () and number of b-tagged jets (). Each pie-chart for a given search variable is inclusive in other three search variables with baseline selections applied.

 Figure LLb : (Top) Stacked distribution for W+jets showing relative fractions of “Single lepton” and three sub-categories of “Lost lepton” events (lost due to out of acceptance, failing ID/isolation requirement or having hadronically decaying tau) parameterized in bins of number of jets () and number of b-tagged jets (). Uncertainties are statistical only. (Bottom) Ratio of "Lost lepton" (combining three sub-categories) to "Single lepton" fraction parameterized in number of jets () and number of b-tagged jets (). Figure LLc : (Top) Stacked distribution for ttbar showing relative fractions of “Single lepton” and three sub-categories of “Lost lepton” events (lost due to out of acceptance, failing ID/isolation requirement or having hadronically decaying tau) parameterized in bins of number of jets () and number of b-tagged jets (). Uncertainties are statistical only. (Bottom) Ratio of "Lost lepton" (combining three sub-categories) to "Single lepton" fraction parameterized in number of jets () and number of b-tagged jets ().
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 META FILEATTACHMENT attachment="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" attr="" comment="Distribution of single photon event yields with baseline selection applied in the 46 search bins with $N_%7b\rm b-jet%7d=0$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1567586131" name="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" path="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" size="23517" user="trmishra" version="2" attachment="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" attr="" comment="Distribution of single photon event yields with baseline selection applied in the 46 search bins with $N_%7b\rm b-jet%7d=0$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1567586734" name="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" path="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" size="18462" user="trmishra" version="2" attachment="HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" attr="" comment="Distribution of single photon event yields with baseline selection applied and $N_%7b\rm b-jet%7d=0$ versus $H_%7b\rm T%7d$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1567586224" name="HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" path="HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" size="23351" user="trmishra" version="2"
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# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

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 Figure Z2d : Representative dilepton mass distributions from the +jets control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (d) with , .
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 Figure BKa : Data driven background composition in zero-lepton signal region projected onto different bins in search variables , number of jets () and number of b-tagged jets (). Each pie-chart for a given search variable is inclusive in other three search variables with baseline selections applied.
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 Figure BKa : Data driven background composition in zero-lepton signal region projected onto different bins in search variables , number of jets () and number of b-tagged jets (). Each pie-chart for a given search variable is inclusive in other three search variables with baseline selections applied.

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 Figure BKb : Data driven background composition in zero-lepton signal region projected onto two dimensional bins in search variables number of jets () and number of b-tagged jets (). These pie-charts are inclusive in , after selection 300 GeV and 300 GeV applied.
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 Figure BKb : Data driven background composition in zero-lepton signal region projected onto two dimensional bins in search variables number of jets () and number of b-tagged jets (). These pie-charts are inclusive in , after selection 300 GeV and 300 GeV applied.

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 Figure BKc : Data driven background composition in zero-lepton signal region projected onto two dimensional bins in search variables number of jets () and number of b-tagged jets (). These pie-charts are inclusive in , after selection 600 GeV and 600 GeV applied.
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 Figure BKc : Data driven background composition in zero-lepton signal region projected onto two dimensional bins in search variables number of jets () and number of b-tagged jets (). These pie-charts are inclusive in , after selection 600 GeV and 600 GeV applied.

 Figure LLa : Lost lepton background in signal region decomposed as that from ttbar, W+jets and Single top in different bins of , , number of jets () and number of b-tagged jets (). Each pie-chart for a given search variable is inclusive in other three search variables with baseline selections applied.
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 Figure LLb : (Top) Stacked distribution for W+jets showing relative fractions of “Single lepton” and three sub-categories of “Lost lepton” events (lost due to out of acceptance, failing ID/isolation requirement or having hadronically decaying tau) parameterized in bins of number of jets () and number of b-tagged jets (). Uncertainties are statistical only. (Bottom) Ratio of "Lost lepton" (combining three sub-categories) to "Single lepton" fraction parameterized in number of jets () and number of b-tagged jets (). Figure LLc : (Top) Stacked distribution for ttbar showing relative fractions of “Single lepton” and three sub-categories of “Lost lepton” events (lost due to out of acceptance, failing ID/isolation requirement or having hadronically decaying tau) parameterized in bins of number of jets () and number of b-tagged jets (). Uncertainties are statistical only. (Bottom) Ratio of "Lost lepton" (combining three sub-categories) to "Single lepton" fraction parameterized in number of jets () and number of b-tagged jets ().
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 Figure LLb : (Top) Stacked distribution for W+jets showing relative fractions of “Single lepton” and three sub-categories of “Lost lepton” events (lost due to out of acceptance, failing ID/isolation requirement or having hadronically decaying tau) parameterized in bins of number of jets () and number of b-tagged jets (). Uncertainties are statistical only. (Bottom) Ratio of "Lost lepton" (combining three sub-categories) to "Single lepton" fraction parameterized in number of jets () and number of b-tagged jets (). Figure LLc : (Top) Stacked distribution for ttbar showing relative fractions of “Single lepton” and three sub-categories of “Lost lepton” events (lost due to out of acceptance, failing ID/isolation requirement or having hadronically decaying tau) parameterized in bins of number of jets () and number of b-tagged jets (). Uncertainties are statistical only. (Bottom) Ratio of "Lost lepton" (combining three sub-categories) to "Single lepton" fraction parameterized in number of jets () and number of b-tagged jets ().

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## Results: yields vs. background prediction, select kinematic distributions

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 META FILEATTACHMENT attachment="fitZmass_5j2b_mm.png" attr="" comment="Zinv dilepton mass distn's with purity fits" date="1567619998" name="fitZmass_5j2b_mm.png" path="fitZmass_5j2b_mm.png" size="17843" user="wtford" version="3" attachment="PieChartHTWithSupplementary_137.pdf" attr="" comment="Lost lepton background in signal region decomposed as that from ttbar, W+jets and Single top" date="1564647072" name="PieChartHTWithSupplementary_137.pdf" path="PieChartHTWithSupplementary_137.pdf" size="43100" user="arane" version="1" attachment="PieChartHTWithSupplementary_137.png" attr="" comment="Lost lepton background in signal region decomposed as that from ttbar, W+jets and Single top" date="1564645983" name="PieChartHTWithSupplementary_137.png" path="PieChartHTWithSupplementary_137.png" size="16637" user="arane" version="1"
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 META FILEATTACHMENT attachment="1300_h_2017_CRSR_forSupplimentary_Exp_WJet.pdf" attr="" comment="Transfer Factor dependance on jet and b-jet multiplicity in W+jet event." date="1564651880" name="1300_h_2017_CRSR_forSupplimentary_Exp_WJet.pdf" path="1300_h_2017_CRSR_forSupplimentary_Exp_WJet.pdf" size="20030" user="arane" version="1" attachment="1300_h_2017_CRSR_forSupplimentary_Exp_WJet.png" attr="" comment="Transfer Factor dependance on jet and b-jet multiplicity in W+jet event." date="1564651880" name="1300_h_2017_CRSR_forSupplimentary_Exp_WJet.png" path="1300_h_2017_CRSR_forSupplimentary_Exp_WJet.png" size="25926" user="arane" version="1" attachment="1300_h_2017_CRSR_forSupplimentary_Exp_TTbar.pdf" attr="" comment="Transfer Factor dependance on jet and b-jet multiplicity in ttbar event." date="1564653596" name="1300_h_2017_CRSR_forSupplimentary_Exp_TTbar.pdf" path="1300_h_2017_CRSR_forSupplimentary_Exp_TTbar.pdf" size="20110" user="arane" version="1" attachment="1300_h_2017_CRSR_forSupplimentary_Exp_TTbar.png" attr="" comment="Transfer Factor dependance on jet and b-jet multiplicity in ttbar event." date="1564653596" name="1300_h_2017_CRSR_forSupplimentary_Exp_TTbar.png" path="1300_h_2017_CRSR_forSupplimentary_Exp_TTbar.png" size="24764" user="arane" version="1"

 META FILEATTACHMENT attachment="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" attr="" comment="Distribution of single photon event yields with baseline selection applied in the 46 search bins with $N_%7b\rm b-jet%7d=0$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1567586131" name="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" path="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" size="23517" user="trmishra" version="2" attachment="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" attr="" comment="Distribution of single photon event yields with baseline selection applied in the 46 search bins with $N_%7b\rm b-jet%7d=0$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1567586734" name="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" path="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" size="18462" user="trmishra" version="2" attachment="HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" attr="" comment="Distribution of single photon event yields with baseline selection applied and $N_%7b\rm b-jet%7d=0$ versus $H_%7b\rm T%7d$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1567586224" name="HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" path="HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" size="23351" user="trmishra" version="2"
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 META FILEATTACHMENT attachment="PieChartWithAllBkg_137.png" attr="" comment="Data driven background estimation projected in different search variables" date="1565710715" name="PieChartWithAllBkg_137.png" path="PieChartWithAllBkg_137.png" size="15452" user="arane" version="1" attachment="PieChart2DBaselineHTMHTAllBkg_137.pdf" attr="" comment="Data driven background composition in 2D Njet-Nbjet projection after HT300 and MHT300" date="1565712426" name="PieChart2DBaselineHTMHTAllBkg_137.pdf" path="PieChart2DBaselineHTMHTAllBkg_137.pdf" size="36248" user="arane" version="1" attachment="PieChart2DBaselineHTMHTAllBkg_137.png" attr="" comment="Data driven background composition in 2D Njet-Nbjet projection after HT300 and MHT300" date="1565712426" name="PieChart2DBaselineHTMHTAllBkg_137.png" path="PieChart2DBaselineHTMHTAllBkg_137.png" size="17016" user="arane" version="1"
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 META FILEATTACHMENT attachment="PieChart2DHigherHTMHTAllBkg_137.pdf" attr="" comment="Data driven background composition in 2D Njet-Nbjet projection after HT 600 GeV and MHT 600 GeV" date="1565713548" name="PieChart2DHigherHTMHTAllBkg_137.pdf" path="PieChart2DHigherHTMHTAllBkg_137.pdf" size="36613" user="arane" version="1" attachment="PieChart2DHigherHTMHTAllBkg_137.png" attr="" comment="Data driven background composition in 2D Njet-Nbjet projection after HT 600 GeV and MHT 600 GeV" date="1565713548" name="PieChart2DHigherHTMHTAllBkg_137.png" path="PieChart2DHigherHTMHTAllBkg_137.png" size="16767" user="arane" version="1"
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 META FILEATTACHMENT attachment="1300_withArxiv_h_2017_CRSR_forSupplimentary_Exp_ttbar.pdf" attr="" comment="Transfer Factor dependance on jet and b-jet multiplicity in ttbar event." date="1567667006" name="1300_withArxiv_h_2017_CRSR_forSupplimentary_Exp_ttbar.pdf" path="1300_withArxiv_h_2017_CRSR_forSupplimentary_Exp_ttbar.pdf" size="20163" user="arane" version="1" attachment="1300_withArxiv_h_2017_CRSR_forSupplimentary_Exp_ttbar.png" attr="" comment="Transfer Factor dependance on jet and b-jet multiplicity in ttbar event." date="1567667493" name="1300_withArxiv_h_2017_CRSR_forSupplimentary_Exp_ttbar.png" path="1300_withArxiv_h_2017_CRSR_forSupplimentary_Exp_ttbar.png" size="26032" user="arane" version="1" attachment="1300_withArxiv_h_2017_CRSR_forSupplimentary_Exp_Wjet.pdf" attr="" comment="Transfer Factor dependance on jet and b-jet multiplicity in W+jet event." date="1567667816" name="1300_withArxiv_h_2017_CRSR_forSupplimentary_Exp_Wjet.pdf" path="1300_withArxiv_h_2017_CRSR_forSupplimentary_Exp_Wjet.pdf" size="20081" user="arane" version="1" attachment="1300_withArxiv_h_2017_CRSR_forSupplimentary_Exp_Wjet.png" attr="" comment="Transfer Factor dependance on jet and b-jet multiplicity in W+jet event." date="1567667877" name="1300_withArxiv_h_2017_CRSR_forSupplimentary_Exp_Wjet.png" path="1300_withArxiv_h_2017_CRSR_forSupplimentary_Exp_Wjet.png" size="27191" user="arane" version="1" attachment="PieChart2DBaselineHTMHTAllBkg_withArxiv_137.pdf" attr="" comment="Data driven background composition in 2D Njet-Nbjet projection after HT300 and MHT300" date="1567671721" name="PieChart2DBaselineHTMHTAllBkg_withArxiv_137.pdf" path="PieChart2DBaselineHTMHTAllBkg_withArxiv_137.pdf" size="36296" user="arane" version="1" attachment="PieChart2DBaselineHTMHTAllBkg_withArxiv_137.png" attr="" comment="Data driven background composition in 2D Njet-Nbjet projection after HT300 and MHT300" date="1567671837" name="PieChart2DBaselineHTMHTAllBkg_withArxiv_137.png" path="PieChart2DBaselineHTMHTAllBkg_withArxiv_137.png" size="18002" user="arane" version="1" attachment="PieChart2DHigherHTMHTAllBkg_withArxiv_137.pdf" attr="" comment="Data driven background composition in 2D Njet-Nbjet projection after HT 600 GeV and MHT 600 GeV" date="1567673782" name="PieChart2DHigherHTMHTAllBkg_withArxiv_137.pdf" path="PieChart2DHigherHTMHTAllBkg_withArxiv_137.pdf" size="36656" user="arane" version="1" attachment="PieChart2DHigherHTMHTAllBkg_withArxiv_137.png" attr="" comment="Data driven background composition in 2D Njet-Nbjet projection after HT 600 GeV and MHT 600 GeV" date="1567673879" name="PieChart2DHigherHTMHTAllBkg_withArxiv_137.png" path="PieChart2DHigherHTMHTAllBkg_withArxiv_137.png" size="17734" user="arane" version="1" attachment="PieChartWithAllBkg_withArxiv_137.pdf" attr="" comment="Data driven background estimation projected in different search variables" date="1567674516" name="PieChartWithAllBkg_withArxiv_137.pdf" path="PieChartWithAllBkg_withArxiv_137.pdf" size="34186" user="arane" version="1" attachment="PieChartWithAllBkg_withArxiv_137.png" attr="" comment="Data driven background estimation projected in different search variables" date="1567674636" name="PieChartWithAllBkg_withArxiv_137.png" path="PieChartWithAllBkg_withArxiv_137.png" size="16418" user="arane" version="1"

#### Revision 232019-09-04 - WilliamFord

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 META TOPICPARENT name="PhysicsResultsSUS"

# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

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 META FILEATTACHMENT attachment="results-plot-prefit-137Paper_pre_app-QvalueGluino.pdf" attr="" comment="" date="1563537004" name="results-plot-prefit-137Paper_pre_app-QvalueGluino.pdf" path="results-plot-prefit-137Paper_pre_app-QvalueGluino.pdf" size="61779" user="rpatel" version="1" attachment="results-plot-prefit-137Paper_pre_app-QvalueSquark.png" attr="" comment="" date="1563538123" name="results-plot-prefit-137Paper_pre_app-QvalueSquark.png" path="results-plot-prefit-137Paper_pre_app-QvalueSquark.png" size="68356" user="rpatel" version="1" attachment="results-plot-prefit-137Paper_pre_app-QvalueSquark.pdf" attr="" comment="" date="1563538123" name="results-plot-prefit-137Paper_pre_app-QvalueSquark.pdf" path="results-plot-prefit-137Paper_pre_app-QvalueSquark.pdf" size="67499" user="rpatel" version="1"
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 META FILEATTACHMENT attachment="DRtriple_Run2v17_DRr2wt_sig.pdf" attr="" comment="Zinv double ratio vs HT, MHT, NJets" date="1564007223" name="DRtriple_Run2v17_DRr2wt_sig.pdf" path="DRtriple_Run2v17_DRr2wt_sig.pdf" size="21442" user="wtford" version="2" attachment="DRtriple_Run2v17_DRr2wt_sig.png" attr="" comment="Zinv double ratio vs HT, MHT, NJets" date="1564007223" name="DRtriple_Run2v17_DRr2wt_sig.png" path="DRtriple_Run2v17_DRr2wt_sig.png" size="31013" user="wtford" version="2" attachment="fitZmass_2j0b_ee.pdf" attr="" comment="Zinv dilepton mass distn's with purity fits" date="1564005164" name="fitZmass_2j0b_ee.pdf" path="fitZmass_2j0b_ee.pdf" size="20339" user="wtford" version="2" attachment="fitZmass_2j0b_mm.pdf" attr="" comment="Zinv dilepton mass distn's with purity fits" date="1564005384" name="fitZmass_2j0b_mm.pdf" path="fitZmass_2j0b_mm.pdf" size="20361" user="wtford" version="2" attachment="fitZmass_5j2b_ee.pdf" attr="" comment="Zinv dilepton mass distn's with purity fits" date="1564005298" name="fitZmass_5j2b_ee.pdf" path="fitZmass_5j2b_ee.pdf" size="20333" user="wtford" version="2" attachment="fitZmass_5j2b_mm.pdf" attr="" comment="Zinv dilepton mass distn's with purity fits" date="1564005298" name="fitZmass_5j2b_mm.pdf" path="fitZmass_5j2b_mm.pdf" size="20058" user="wtford" version="2" attachment="fitZmass_2j0b_ee.png" attr="" comment="Zinv dilepton mass distn's with purity fits" date="1564005164" name="fitZmass_2j0b_ee.png" path="fitZmass_2j0b_ee.png" size="16199" user="wtford" version="2" attachment="fitZmass_2j0b_mm.png" attr="" comment="Zinv dilepton mass distn's with purity fits" date="1564005509" name="fitZmass_2j0b_mm.png" path="fitZmass_2j0b_mm.png" size="16231" user="wtford" version="2" attachment="fitZmass_5j2b_ee.png" attr="" comment="Zinv dilepton mass distn's with purity fits" date="1564005298" name="fitZmass_5j2b_ee.png" path="fitZmass_5j2b_ee.png" size="16920" user="wtford" version="2" attachment="fitZmass_5j2b_mm.png" attr="" comment="Zinv dilepton mass distn's with purity fits" date="1564005298" name="fitZmass_5j2b_mm.png" path="fitZmass_5j2b_mm.png" size="17385" user="wtford" version="2"
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 META FILEATTACHMENT attachment="DRtriple_Run2v17_DRr2wt_sig.pdf" attr="" comment="Zinv double ratio vs HT, MHT, NJets" date="1567617721" name="DRtriple_Run2v17_DRr2wt_sig.pdf" path="DRtriple_Run2v17_DRr2wt_sig.pdf" size="21492" user="wtford" version="3" attachment="DRtriple_Run2v17_DRr2wt_sig.png" attr="" comment="Zinv double ratio vs HT, MHT, NJets" date="1567617857" name="DRtriple_Run2v17_DRr2wt_sig.png" path="DRtriple_Run2v17_DRr2wt_sig.png" size="32806" user="wtford" version="3" attachment="fitZmass_2j0b_ee.pdf" attr="" comment="Zinv dilepton mass distn's with purity fits" date="1567619667" name="fitZmass_2j0b_ee.pdf" path="fitZmass_2j0b_ee.pdf" size="20389" user="wtford" version="3" attachment="fitZmass_2j0b_mm.pdf" attr="" comment="Zinv dilepton mass distn's with purity fits" date="1567619780" name="fitZmass_2j0b_mm.pdf" path="fitZmass_2j0b_mm.pdf" size="20408" user="wtford" version="3" attachment="fitZmass_5j2b_ee.pdf" attr="" comment="Zinv dilepton mass distn's with purity fits" date="1567619874" name="fitZmass_5j2b_ee.pdf" path="fitZmass_5j2b_ee.pdf" size="20382" user="wtford" version="3" attachment="fitZmass_5j2b_mm.pdf" attr="" comment="Zinv dilepton mass distn's with purity fits" date="1567619960" name="fitZmass_5j2b_mm.pdf" path="fitZmass_5j2b_mm.pdf" size="20107" user="wtford" version="3" attachment="fitZmass_2j0b_ee.png" attr="" comment="Zinv dilepton mass distn's with purity fits" date="1567619726" name="fitZmass_2j0b_ee.png" path="fitZmass_2j0b_ee.png" size="16662" user="wtford" version="3" attachment="fitZmass_2j0b_mm.png" attr="" comment="Zinv dilepton mass distn's with purity fits" date="1567619829" name="fitZmass_2j0b_mm.png" path="fitZmass_2j0b_mm.png" size="16738" user="wtford" version="3" attachment="fitZmass_5j2b_ee.png" attr="" comment="Zinv dilepton mass distn's with purity fits" date="1567619927" name="fitZmass_5j2b_ee.png" path="fitZmass_5j2b_ee.png" size="17367" user="wtford" version="3" attachment="fitZmass_5j2b_mm.png" attr="" comment="Zinv dilepton mass distn's with purity fits" date="1567619998" name="fitZmass_5j2b_mm.png" path="fitZmass_5j2b_mm.png" size="17843" user="wtford" version="3"

 META FILEATTACHMENT attachment="PieChartHTWithSupplementary_137.pdf" attr="" comment="Lost lepton background in signal region decomposed as that from ttbar, W+jets and Single top" date="1564647072" name="PieChartHTWithSupplementary_137.pdf" path="PieChartHTWithSupplementary_137.pdf" size="43100" user="arane" version="1" attachment="PieChartHTWithSupplementary_137.png" attr="" comment="Lost lepton background in signal region decomposed as that from ttbar, W+jets and Single top" date="1564645983" name="PieChartHTWithSupplementary_137.png" path="PieChartHTWithSupplementary_137.png" size="16637" user="arane" version="1" attachment="1300_h_2017_CRSR_forSupplimentary_Exp_WJet.pdf" attr="" comment="Transfer Factor dependance on jet and b-jet multiplicity in W+jet event." date="1564651880" name="1300_h_2017_CRSR_forSupplimentary_Exp_WJet.pdf" path="1300_h_2017_CRSR_forSupplimentary_Exp_WJet.pdf" size="20030" user="arane" version="1"

#### Revision 222019-09-04 - TribeniMishra1

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 META TOPICPARENT name="PhysicsResultsSUS"

# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

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 META FILEATTACHMENT attachment="MHT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" attr="" comment="Distribution of single photon event yields with baseline selection applied and $N_%7b\rm b-jet%7d=0$ versus $H^%7b\rm miss%7d_%7b\rm T%7d$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1567586344" name="MHT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" path="MHT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" size="19119" user="trmishra" version="2" attachment="NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" attr="" comment="Distribution of single photon event yields with baseline selection applied and $N_%7b\rm b-jet%7d=0$ versus $N_%7b\rm jet%7d$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1567586016" name="NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" path="NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" size="17790" user="trmishra" version="2" attachment="NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" attr="" comment="Distribution of single photon event yields with baseline selection applied and $N_%7b\rm b-jet%7d=0$ versus $N_%7b\rm jet%7d$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1567586016" name="NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" path="NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" size="15147" user="trmishra" version="2"
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 META FILEATTACHMENT attachment="Purity_Run2_supplementary.pdf" attr="" comment="Measured photon purity versus $H^%7b\rm miss%7d_%7b\rm T%7d$. The solid points with errors show the purity for events with a photon reconstructed in the barrel; open points with errors show the purity for events with a photon reconstructed in the endcap." date="1565252683" name="Purity_Run2_supplementary.pdf" path="Purity_Run2_supplementary.pdf" size="14666" user="trmishra" version="1" attachment="Purity_Run2_supplementary.png" attr="" comment="Measured photon purity versus $H^%7b\rm miss%7d_%7b\rm T%7d$. The solid points with errors show the purity for events with a photon reconstructed in the barrel; open points with errors show the purity for events with a photon reconstructed in the endcap." date="1565252683" name="Purity_Run2_supplementary.png" path="Purity_Run2_supplementary.png" size="15909" user="trmishra" version="1" attachment="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.pdf" attr="" comment="Distribution of $R_%7b%7b\rm Z%7d/\gamma%7d$ with baseline selection applied in the 46 search bins with $N_%7b\rm b-jet%7d=0$. Because of limited statistical precision in the simulated event samples at large $N_%7b\rm jet%7d$, the transfer factors determined for the $8\leq$N_%7b\rm jet%7d$\leq 9$ region are also used for the $N_%7b\rm jet%7d10$ region. Points with error bars show the computed value in each bin with statistical uncertainties." date="1565253082" name="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.pdf" path="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.pdf" size="16980" user="trmishra" version="1" attachment="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.png" attr="" comment="Distribution of $R_%7b%7b\rm Z%7d/\gamma%7d$ with baseline selection applied in the 46 search bins with $N_%7b\rm b-jet%7d=0$. Because of limited statistical precision in the simulated event samples at large $N_%7b\rm jet%7d$, the transfer factors determined for the $8\leq$N_%7b\rm jet%7d$\leq 9$ region are also used for the $N_%7b\rm jet%7d10$ region. Points with error bars show the computed value in each bin with statistical uncertainties." date="1565253082" name="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.png" path="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.png" size="13866" user="trmishra" version="1"
>
>
 META FILEATTACHMENT attachment="Purity_Run2_supplementary.pdf" attr="" comment="Measured photon purity versus $H^%7b\rm miss%7d_%7b\rm T%7d$. The solid points with errors show the purity for events with a photon reconstructed in the barrel; open points with errors show the purity for events with a photon reconstructed in the endcap." date="1567593227" name="Purity_Run2_supplementary.pdf" path="Purity_Run2_supplementary.pdf" size="14697" user="trmishra" version="2" attachment="Purity_Run2_supplementary.png" attr="" comment="Measured photon purity versus $H^%7b\rm miss%7d_%7b\rm T%7d$. The solid points with errors show the purity for events with a photon reconstructed in the barrel; open points with errors show the purity for events with a photon reconstructed in the endcap." date="1567593262" name="Purity_Run2_supplementary.png" path="Purity_Run2_supplementary.png" size="17526" user="trmishra" version="2" attachment="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.pdf" attr="" comment="Distribution of $R_%7b%7b\rm Z%7d/\gamma%7d$ with baseline selection applied in the 46 search bins with $N_%7b\rm b-jet%7d=0$. Because of limited statistical precision in the simulated event samples at large $N_%7b\rm jet%7d$, the transfer factors determined for the $8\leq$N_%7b\rm jet%7d$\leq 9$ region are also used for the $N_%7b\rm jet%7d10$ region. Points with error bars show the computed value in each bin with statistical uncertainties." date="1567590779" name="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.pdf" path="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.pdf" size="17012" user="trmishra" version="2" attachment="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.png" attr="" comment="Distribution of $R_%7b%7b\rm Z%7d/\gamma%7d$ with baseline selection applied in the 46 search bins with $N_%7b\rm b-jet%7d=0$. Because of limited statistical precision in the simulated event samples at large $N_%7b\rm jet%7d$, the transfer factors determined for the $8\leq$N_%7b\rm jet%7d$\leq 9$ region are also used for the $N_%7b\rm jet%7d10$ region. Points with error bars show the computed value in each bin with statistical uncertainties." date="1567590747" name="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.png" path="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.png" size="14500" user="trmishra" version="2"

 META FILEATTACHMENT attachment="PieChartWithAllBkg_137.pdf" attr="" comment="Data driven background estimation projected in different search variables" date="1565710715" name="PieChartWithAllBkg_137.pdf" path="PieChartWithAllBkg_137.pdf" size="34128" user="arane" version="1" attachment="PieChartWithAllBkg_137.png" attr="" comment="Data driven background estimation projected in different search variables" date="1565710715" name="PieChartWithAllBkg_137.png" path="PieChartWithAllBkg_137.png" size="15452" user="arane" version="1" attachment="PieChart2DBaselineHTMHTAllBkg_137.pdf" attr="" comment="Data driven background composition in 2D Njet-Nbjet projection after HT300 and MHT300" date="1565712426" name="PieChart2DBaselineHTMHTAllBkg_137.pdf" path="PieChart2DBaselineHTMHTAllBkg_137.pdf" size="36248" user="arane" version="1"

#### Revision 212019-09-04 - TribeniMishra1

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 META TOPICPARENT name="PhysicsResultsSUS"

# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

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 META FILEATTACHMENT attachment="1300_h_2017_CRSR_forSupplimentary_Exp_WJet.png" attr="" comment="Transfer Factor dependance on jet and b-jet multiplicity in W+jet event." date="1564651880" name="1300_h_2017_CRSR_forSupplimentary_Exp_WJet.png" path="1300_h_2017_CRSR_forSupplimentary_Exp_WJet.png" size="25926" user="arane" version="1" attachment="1300_h_2017_CRSR_forSupplimentary_Exp_TTbar.pdf" attr="" comment="Transfer Factor dependance on jet and b-jet multiplicity in ttbar event." date="1564653596" name="1300_h_2017_CRSR_forSupplimentary_Exp_TTbar.pdf" path="1300_h_2017_CRSR_forSupplimentary_Exp_TTbar.pdf" size="20110" user="arane" version="1" attachment="1300_h_2017_CRSR_forSupplimentary_Exp_TTbar.png" attr="" comment="Transfer Factor dependance on jet and b-jet multiplicity in ttbar event." date="1564653596" name="1300_h_2017_CRSR_forSupplimentary_Exp_TTbar.png" path="1300_h_2017_CRSR_forSupplimentary_Exp_TTbar.png" size="24764" user="arane" version="1"
Changed:
<
<
 META FILEATTACHMENT attachment="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" attr="" comment="Distribution of single photon event yields with baseline selection applied in the 46 search bins with $N_%7b\rm b-jet%7d=0$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1565252261" name="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" path="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" size="23488" user="trmishra" version="1" attachment="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" attr="" comment="Distribution of single photon event yields with baseline selection applied in the 46 search bins with $N_%7b\rm b-jet%7d=0$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1565252290" name="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" path="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" size="17670" user="trmishra" version="1" attachment="HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" attr="" comment="Distribution of single photon event yields with baseline selection applied and $N_%7b\rm b-jet%7d=0$ versus $H_%7b\rm T%7d$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1565252393" name="HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" path="HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" size="23320" user="trmishra" version="1" attachment="HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" attr="" comment="Distribution of single photon event yields with baseline selection applied and $N_%7b\rm b-jet%7d=0$ versus $H_%7b\rm T%7d$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1565252393" name="HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" path="HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" size="16685" user="trmishra" version="1" attachment="MHT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" attr="" comment="Distribution of single photon event yields with baseline selection applied and $N_%7b\rm b-jet%7d=0$ versus $H^%7b\rm miss%7d_%7b\rm T%7d$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1565252493" name="MHT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" path="MHT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" size="24436" user="trmishra" version="1" attachment="MHT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" attr="" comment="Distribution of single photon event yields with baseline selection applied and $N_%7b\rm b-jet%7d=0$ versus $H^%7b\rm miss%7d_%7b\rm T%7d$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1565252525" name="MHT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" path="MHT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" size="18293" user="trmishra" version="1" attachment="NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" attr="" comment="Distribution of single photon event yields with baseline selection applied and $N_%7b\rm b-jet%7d=0$ versus $N_%7b\rm jet%7d$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1565252623" name="NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" path="NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" size="17759" user="trmishra" version="1" attachment="NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" attr="" comment="Distribution of single photon event yields with baseline selection applied and $N_%7b\rm b-jet%7d=0$ versus $N_%7b\rm jet%7d$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1565252623" name="NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" path="NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" size="14326" user="trmishra" version="1"
>
>
 META FILEATTACHMENT attachment="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" attr="" comment="Distribution of single photon event yields with baseline selection applied in the 46 search bins with $N_%7b\rm b-jet%7d=0$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1567586131" name="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" path="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" size="23517" user="trmishra" version="2" attachment="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" attr="" comment="Distribution of single photon event yields with baseline selection applied in the 46 search bins with $N_%7b\rm b-jet%7d=0$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1567586734" name="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" path="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" size="18462" user="trmishra" version="2" attachment="HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" attr="" comment="Distribution of single photon event yields with baseline selection applied and $N_%7b\rm b-jet%7d=0$ versus $H_%7b\rm T%7d$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1567586224" name="HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" path="HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" size="23351" user="trmishra" version="2" attachment="HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" attr="" comment="Distribution of single photon event yields with baseline selection applied and $N_%7b\rm b-jet%7d=0$ versus $H_%7b\rm T%7d$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1567586276" name="HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" path="HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" size="17481" user="trmishra" version="2" attachment="MHT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" attr="" comment="Distribution of single photon event yields with baseline selection applied and $N_%7b\rm b-jet%7d=0$ versus $H^%7b\rm miss%7d_%7b\rm T%7d$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1567586314" name="MHT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" path="MHT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" size="24467" user="trmishra" version="2" attachment="MHT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" attr="" comment="Distribution of single photon event yields with baseline selection applied and $N_%7b\rm b-jet%7d=0$ versus $H^%7b\rm miss%7d_%7b\rm T%7d$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1567586344" name="MHT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" path="MHT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" size="19119" user="trmishra" version="2" attachment="NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" attr="" comment="Distribution of single photon event yields with baseline selection applied and $N_%7b\rm b-jet%7d=0$ versus $N_%7b\rm jet%7d$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1567586016" name="NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" path="NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" size="17790" user="trmishra" version="2" attachment="NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" attr="" comment="Distribution of single photon event yields with baseline selection applied and $N_%7b\rm b-jet%7d=0$ versus $N_%7b\rm jet%7d$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1567586016" name="NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" path="NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" size="15147" user="trmishra" version="2"

 META FILEATTACHMENT attachment="Purity_Run2_supplementary.pdf" attr="" comment="Measured photon purity versus $H^%7b\rm miss%7d_%7b\rm T%7d$. The solid points with errors show the purity for events with a photon reconstructed in the barrel; open points with errors show the purity for events with a photon reconstructed in the endcap." date="1565252683" name="Purity_Run2_supplementary.pdf" path="Purity_Run2_supplementary.pdf" size="14666" user="trmishra" version="1" attachment="Purity_Run2_supplementary.png" attr="" comment="Measured photon purity versus $H^%7b\rm miss%7d_%7b\rm T%7d$. The solid points with errors show the purity for events with a photon reconstructed in the barrel; open points with errors show the purity for events with a photon reconstructed in the endcap." date="1565252683" name="Purity_Run2_supplementary.png" path="Purity_Run2_supplementary.png" size="15909" user="trmishra" version="1" attachment="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.pdf" attr="" comment="Distribution of $R_%7b%7b\rm Z%7d/\gamma%7d$ with baseline selection applied in the 46 search bins with $N_%7b\rm b-jet%7d=0$. Because of limited statistical precision in the simulated event samples at large $N_%7b\rm jet%7d$, the transfer factors determined for the $8\leq$N_%7b\rm jet%7d$\leq 9$ region are also used for the $N_%7b\rm jet%7d10$ region. Points with error bars show the computed value in each bin with statistical uncertainties." date="1565253082" name="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.pdf" path="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.pdf" size="16980" user="trmishra" version="1"

#### Revision 202019-08-26 - WilliamFord

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 META TOPICPARENT name="PhysicsResultsSUS"

# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

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 Figure phoE : Measured photon purity versus . The solid points with errors show the purity for events with a photon reconstructed in the barrel; open points with errors show the purity for events with a photon reconstructed in the endcap.
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| | Figure phoF : Distribution of with baseline selection applied in the 46 search bins with . Because of limited statistical precision in the simulated event samples at large , the transfer factors determined for the region are also used for the region. Points with error bars show the computed value in each bin with statistical uncertainties. |
Latex rendering error!! dvi file was not created.
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 Figure phoF : Distribution of with baseline selection applied in the 46 search bins with . Because of limited statistical precision in the simulated event samples at large , the transfer factors determined for the region are also used for the region. Points with error bars show the computed value in each bin with statistical uncertainties.

 Figure Z1 : Double ratio vs. (left), (center), and Events in the simulated +jets sample have been weighted by the reciprocal of the -dependent function represented by the green dot-dashed line in the left-hand panel. The average value of this function is 0.95. Points with error bars show the value of in each bin with statistical uncertainties. The solid and dashed blue lines show the straight-line fit and uncertainties propagated from the fit, respectively. The average value, 1.00, is drawn as a red dashed line on each plot.

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 META TOPICPARENT name="PhysicsResultsSUS"

# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

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 Figure Z2d : Representative dilepton mass distributions from the +jets control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (d) with , .
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 Figure LLa : Lost lepton background in signal region decomposed as that from ttbar, W+jets and Single top in different bins of , , number of jets () and number of b-tagged jets (). Each pie-chart for a given search variable is inclusive in other three search variables with baseline selections applied.
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 Figure BKa : Data driven background composition in zero-lepton signal region projected onto different bins in search variables , number of jets () and number of b-tagged jets (). Each pie-chart for a given search variable is inclusive in other three search variables with baseline selections applied.

 Figure BKb : Data driven background composition in zero-lepton signal region projected onto two dimensional bins in search variables number of jets () and number of b-tagged jets (). These pie-charts are inclusive in , after selection 300 GeV and 300 GeV applied.

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 Figure BKc : Data driven background composition in zero-lepton signal region projected onto two dimensional bins in search variables number of jets () and number of b-tagged jets (). These pie-charts are inclusive in , after selection 600 GeV and 600 GeV applied.

 Figure LLa : Lost lepton background in signal region decomposed as that from ttbar, W+jets and Single top in different bins of , , number of jets () and number of b-tagged jets (). Each pie-chart for a given search variable is inclusive in other three search variables with baseline selections applied.

 Figure LLb : (Top) Stacked distribution for W+jets showing relative fractions of “Single lepton” and three sub-categories of “Lost lepton” events (lost due to out of acceptance, failing ID/isolation requirement or having hadronically decaying tau) parameterized in bins of number of jets () and number of b-tagged jets (). Uncertainties are statistical only. (Bottom) Ratio of "Lost lepton" (combining three sub-categories) to "Single lepton" fraction parameterized in number of jets () and number of b-tagged jets (). Figure LLc : (Top) Stacked distribution for ttbar showing relative fractions of “Single lepton” and three sub-categories of “Lost lepton” events (lost due to out of acceptance, failing ID/isolation requirement or having hadronically decaying tau) parameterized in bins of number of jets () and number of b-tagged jets (). Uncertainties are statistical only. (Bottom) Ratio of "Lost lepton" (combining three sub-categories) to "Single lepton" fraction parameterized in number of jets () and number of b-tagged jets ().
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 META FILEATTACHMENT attachment="Purity_Run2_supplementary.png" attr="" comment="Measured photon purity versus $H^%7b\rm miss%7d_%7b\rm T%7d$. The solid points with errors show the purity for events with a photon reconstructed in the barrel; open points with errors show the purity for events with a photon reconstructed in the endcap." date="1565252683" name="Purity_Run2_supplementary.png" path="Purity_Run2_supplementary.png" size="15909" user="trmishra" version="1" attachment="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.pdf" attr="" comment="Distribution of $R_%7b%7b\rm Z%7d/\gamma%7d$ with baseline selection applied in the 46 search bins with $N_%7b\rm b-jet%7d=0$. Because of limited statistical precision in the simulated event samples at large $N_%7b\rm jet%7d$, the transfer factors determined for the $8\leq$N_%7b\rm jet%7d$\leq 9$ region are also used for the $N_%7b\rm jet%7d10$ region. Points with error bars show the computed value in each bin with statistical uncertainties." date="1565253082" name="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.pdf" path="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.pdf" size="16980" user="trmishra" version="1" attachment="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.png" attr="" comment="Distribution of $R_%7b%7b\rm Z%7d/\gamma%7d$ with baseline selection applied in the 46 search bins with $N_%7b\rm b-jet%7d=0$. Because of limited statistical precision in the simulated event samples at large $N_%7b\rm jet%7d$, the transfer factors determined for the $8\leq$N_%7b\rm jet%7d$\leq 9$ region are also used for the $N_%7b\rm jet%7d10$ region. Points with error bars show the computed value in each bin with statistical uncertainties." date="1565253082" name="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.png" path="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.png" size="13866" user="trmishra" version="1"
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 META FILEATTACHMENT attachment="PieChartWithAllBkg_137.pdf" attr="" comment="Data driven background estimation projected in different search variables" date="1565710715" name="PieChartWithAllBkg_137.pdf" path="PieChartWithAllBkg_137.pdf" size="34128" user="arane" version="1" attachment="PieChartWithAllBkg_137.png" attr="" comment="Data driven background estimation projected in different search variables" date="1565710715" name="PieChartWithAllBkg_137.png" path="PieChartWithAllBkg_137.png" size="15452" user="arane" version="1" attachment="PieChart2DBaselineHTMHTAllBkg_137.pdf" attr="" comment="Data driven background composition in 2D Njet-Nbjet projection after HT300 and MHT300" date="1565712426" name="PieChart2DBaselineHTMHTAllBkg_137.pdf" path="PieChart2DBaselineHTMHTAllBkg_137.pdf" size="36248" user="arane" version="1" attachment="PieChart2DBaselineHTMHTAllBkg_137.png" attr="" comment="Data driven background composition in 2D Njet-Nbjet projection after HT300 and MHT300" date="1565712426" name="PieChart2DBaselineHTMHTAllBkg_137.png" path="PieChart2DBaselineHTMHTAllBkg_137.png" size="17016" user="arane" version="1" attachment="PieChart2DHigherHTMHTAllBkg_137.pdf" attr="" comment="Data driven background composition in 2D Njet-Nbjet projection after HT 600 GeV and MHT 600 GeV" date="1565713548" name="PieChart2DHigherHTMHTAllBkg_137.pdf" path="PieChart2DHigherHTMHTAllBkg_137.pdf" size="36613" user="arane" version="1" attachment="PieChart2DHigherHTMHTAllBkg_137.png" attr="" comment="Data driven background composition in 2D Njet-Nbjet projection after HT 600 GeV and MHT 600 GeV" date="1565713548" name="PieChart2DHigherHTMHTAllBkg_137.png" path="PieChart2DHigherHTMHTAllBkg_137.png" size="16767" user="arane" version="1"

#### Revision 182019-08-11 - WilliamFord

Line: 1 to 1

 META TOPICPARENT name="PhysicsResultsSUS"

# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

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 Figure phoF : Distribution of with baseline selection applied in the 46 search bins with . Because of limited statistical precision in the simulated event samples at large , the transfer factors determined for the region are also used for the region. Points with error bars show the computed value in each bin with statistical uncertainties.

Latex rendering error!! dvi file was not created.

Changed:
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 Figure Zn : Double ratio vs. (left), (center), and Events in the simulated +jets sample have been weighted by the reciprocal of the -dependent function represented by the green dot-dashed line in the left-hand panel. The average value of this function is 0.95. Points with error bars show the value of in each bin with statistical uncertainties. The solid and dashed blue lines show the straight-line fit and uncertainties propagated from the fit, respectively. The average value, 1.00, is drawn as a red dashed line on each plot.
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 Figure Z1 : Double ratio vs. (left), (center), and Events in the simulated +jets sample have been weighted by the reciprocal of the -dependent function represented by the green dot-dashed line in the left-hand panel. The average value of this function is 0.95. Points with error bars show the value of in each bin with statistical uncertainties. The solid and dashed blue lines show the straight-line fit and uncertainties propagated from the fit, respectively. The average value, 1.00, is drawn as a red dashed line on each plot.

Changed:
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 Figure Zma : Representative dilepton mass distributions from the +jets control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (a) with , .
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 Figure Z2a : Representative dilepton mass distributions from the +jets control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (a) with , .

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 Figure Zmb : Representative dilepton mass distributions from the +jets control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (b) with , .
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 Figure Z2b : Representative dilepton mass distributions from the +jets control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (b) with , .

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 Figure Zmc : Representative dilepton mass distributions from the +jets control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (c) with , .
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 Figure Z2c : Representative dilepton mass distributions from the +jets control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (c) with , .

Changed:
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 Figure Zmd : Representative dilepton mass distributions from the +jets control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (d) with , .
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 Figure Z2d : Representative dilepton mass distributions from the +jets control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (d) with , .

 Figure LLa : Lost lepton background in signal region decomposed as that from ttbar, W+jets and Single top in different bins of , , number of jets () and number of b-tagged jets (). Each pie-chart for a given search variable is inclusive in other three search variables with baseline selections applied.

#### Revision 172019-08-08 - RishiPatel

Line: 1 to 1

 META TOPICPARENT name="PhysicsResultsSUS"

# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

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 Figure phoA : Distribution of single photon event yields with baseline selection applied in the 46 search bins with $N_{\rm b-jet}=0$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.

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 Figure phoA : Distribution of single photon event yields with baseline selection applied in the 46 search bins with . Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.

Changed:
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 Figure phoB : Distribution of single photon event yields with baseline selection applied and $N_{\rm b-jet}=0$ versus $H_{\rm T}$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.
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 Figure phoB : Distribution of single photon event yields with baseline selection applied and versus . Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.

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 Figure phoC : Distribution of single photon event yields with baseline selection applied and versus . Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.

Changed:
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 Figure phoC : Distribution of single photon event yields with baseline selection applied and $N_{\rm b-jet}=0$ versus $H^{\rm miss}_{\rm T}$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.
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 Figure phoD : Distribution of single photon event yields with baseline selection applied and versus . Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.

Changed:
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 Figure phoD : Distribution of single photon event yields with baseline selection applied and $N_{\rm b-jet}=0$ versus $N_{\rm jet}$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.
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 Figure phoE : Measured photon purity versus . The solid points with errors show the purity for events with a photon reconstructed in the barrel; open points with errors show the purity for events with a photon reconstructed in the endcap.

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| | Figure phoF : Distribution of with baseline selection applied in the 46 search bins with . Because of limited statistical precision in the simulated event samples at large , the transfer factors determined for the region are also used for the region. Points with error bars show the computed value in each bin with statistical uncertainties. |
Latex rendering error!! dvi file was not created.

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 Figure phoE : Measured photon purity versus $H^{\rm miss}_{\rm T}$. The solid points with errors show the purity for events with a photon reconstructed in the barrel; open points with errors show the purity for events with a photon reconstructed in the endcap.

Changed:
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 Figure phoF : Distribution of $R_{{\rm Z}/\gamma}$ with baseline selection applied in the 46 search bins with $N_{\rm b-jet}=0$. Because of limited statistical precision in the simulated event samples at large $N_{\rm jet}$, the transfer factors determined for the $8\leq$N_{\rm jet}$\leq 9$ region are also used for the $N_{\rm jet}>10$ region. Points with error bars show the computed value in each bin with statistical uncertainties.

 Figure Zn : Double ratio vs. (left), (center), and Events in the simulated +jets sample have been weighted by the reciprocal of the -dependent function represented by the green dot-dashed line in the left-hand panel. The average value of this function is 0.95. Points with error bars show the value of in each bin with statistical uncertainties. The solid and dashed blue lines show the straight-line fit and uncertainties propagated from the fit, respectively. The average value, 1.00, is drawn as a red dashed line on each plot.
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 Figure Zn : Double ratio vs. (left), (center), and Events in the simulated +jets sample have been weighted by the reciprocal of the -dependent function represented by the green dot-dashed line in the left-hand panel. The average value of this function is 0.95. Points with error bars show the value of in each bin with statistical uncertainties. The solid and dashed blue lines show the straight-line fit and uncertainties propagated from the fit, respectively. The average value, 1.00, is drawn as a red dashed line on each plot.

 Figure Zma : Representative dilepton mass distributions from the +jets control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (a) with , .

#### Revision 162019-08-08 - TribeniMishra1

Line: 1 to 1

 META TOPICPARENT name="PhysicsResultsSUS"

# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

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 Figure phoA : Distribution of single photon event yields with baseline selection applied in the 46 search bins with $N_{\rm b-jet}=0$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.

 Figure phoB : Distribution of single photon event yields with baseline selection applied and $N_{\rm b-jet}=0$ versus $H_{\rm T}$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.

 Figure phoC : Distribution of single photon event yields with baseline selection applied and $N_{\rm b-jet}=0$ versus $H^{\rm miss}_{\rm T}$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.

 Figure phoD : Distribution of single photon event yields with baseline selection applied and $N_{\rm b-jet}=0$ versus $N_{\rm jet}$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.

 Figure phoE : Measured photon purity versus $H^{\rm miss}_{\rm T}$. The solid points with errors show the purity for events with a photon reconstructed in the barrel; open points with errors show the purity for events with a photon reconstructed in the endcap.

 Figure phoF : Distribution of $R_{{\rm Z}/\gamma}$ with baseline selection applied in the 46 search bins with $N_{\rm b-jet}=0$. Because of limited statistical precision in the simulated event samples at large $N_{\rm jet}$, the transfer factors determined for the $8\leq$N_{\rm jet}$\leq 9$ region are also used for the $N_{\rm jet}>10$ region. Points with error bars show the computed value in each bin with statistical uncertainties.

 Figure Zn : Double ratio vs. (left), (center), and Events in the simulated +jets sample have been weighted by the reciprocal of the -dependent function represented by the green dot-dashed line in the left-hand panel. The average value of this function is 0.95. Points with error bars show the value of in each bin with statistical uncertainties. The solid and dashed blue lines show the straight-line fit and uncertainties propagated from the fit, respectively. The average value, 1.00, is drawn as a red dashed line on each plot.

 Figure Zma : Representative dilepton mass distributions from the +jets control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (a) with , .
Line: 132 to 150

Deleted:
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• AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf: Distribution of single photon event yields with baseline selection applied in the 46 search bins with $N_{\rm b-jet}=0$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.

• Distribution of single photon event yields with baseline selection applied in the 46 search bins with $N_{\rm b-jet}=0$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.:

• HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf: Distribution of single photon event yields with baseline selection applied and $N_{\rm b-jet}=0$ versus $H_{\rm T}$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.

• Distribution of single photon event yields with baseline selection applied and $N_{\rm b-jet}=0$ versus $H_{\rm T}$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.:

• MHT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf: Distribution of single photon event yields with baseline selection applied and $N_{\rm b-jet}=0$ versus $H^{\rm miss}_{\rm T}$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.

• Distribution of single photon event yields with baseline selection applied and $N_{\rm b-jet}=0$ versus $H^{\rm miss}_{\rm T}$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.:

• NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf: Distribution of single photon event yields with baseline selection applied and $N_{\rm b-jet}=0$ versus $N_{\rm jet}$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.

• Distribution of single photon event yields with baseline selection applied and $N_{\rm b-jet}=0$ versus $N_{\rm jet}$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.:

• Purity_Run2_supplementary.pdf: Measured photon purity versus $H^{\rm miss}_{\rm T}$. The solid points with errors show the purity for events with a photon reconstructed in the barrel; open points with errors show the purity for events with a photon reconstructed in the endcap.

• Measured photon purity versus $H^{\rm miss}_{\rm T}$. The solid points with errors show the purity for events with a photon reconstructed in the barrel; open points with errors show the purity for events with a photon reconstructed in the endcap.:

• AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.pdf: Distribution of $R_{{\rm Z}/\gamma}$ with baseline selection applied in the 46 search bins with $N_{\rm b-jet}=0$. Because of limited statistical precision in the simulated event samples at large $N_{\rm jet}$, the transfer factors determined for the $8\leq$N_{\rm jet}$\leq 9$ region are also used for the $N_{\rm jet}10$ region. Points with error bars show the computed value in each bin with statistical uncertainties.

Deleted:
<
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• Distribution of $R_{{\rm Z}/\gamma}$ with baseline selection applied in the 46 search bins with $N_{\rm b-jet}=0$. Because of limited statistical precision in the simulated event samples at large $N_{\rm jet}$, the transfer factors determined for the $8\leq$N_{\rm jet}$\leq 9$ region are also used for the $N_{\rm jet}10$ region. Points with error bars show the computed value in each bin with statistical uncertainties.:

 META FILEATTACHMENT attachment="njets-projection-pull.pdf" attr="" comment="" date="1562057157" name="njets-projection-pull.pdf" path="njets-projection-pull.pdf" size="17126" user="rpatel" version="1" attachment="nbjets-projection-pull.pdf" attr="" comment="" date="1562057157" name="nbjets-projection-pull.pdf" path="nbjets-projection-pull.pdf" size="17021" user="rpatel" version="1"

#### Revision 152019-08-08 - TribeniMishra1

Line: 1 to 1

 META TOPICPARENT name="PhysicsResultsSUS"

# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

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>
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• AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf: Distribution of single photon event yields with baseline selection applied in the 46 search bins with $N_{\rm b-jet}=0$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.

• Distribution of single photon event yields with baseline selection applied in the 46 search bins with $N_{\rm b-jet}=0$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.:

• HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf: Distribution of single photon event yields with baseline selection applied and $N_{\rm b-jet}=0$ versus $H_{\rm T}$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.

• Distribution of single photon event yields with baseline selection applied and $N_{\rm b-jet}=0$ versus $H_{\rm T}$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.:

• MHT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf: Distribution of single photon event yields with baseline selection applied and $N_{\rm b-jet}=0$ versus $H^{\rm miss}_{\rm T}$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.

• Distribution of single photon event yields with baseline selection applied and $N_{\rm b-jet}=0$ versus $H^{\rm miss}_{\rm T}$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.:

• NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf: Distribution of single photon event yields with baseline selection applied and $N_{\rm b-jet}=0$ versus $N_{\rm jet}$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.

• Distribution of single photon event yields with baseline selection applied and $N_{\rm b-jet}=0$ versus $N_{\rm jet}$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel.:

• Purity_Run2_supplementary.pdf: Measured photon purity versus $H^{\rm miss}_{\rm T}$. The solid points with errors show the purity for events with a photon reconstructed in the barrel; open points with errors show the purity for events with a photon reconstructed in the endcap.

• Measured photon purity versus $H^{\rm miss}_{\rm T}$. The solid points with errors show the purity for events with a photon reconstructed in the barrel; open points with errors show the purity for events with a photon reconstructed in the endcap.:

• AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.pdf: Distribution of $R_{{\rm Z}/\gamma}$ with baseline selection applied in the 46 search bins with $N_{\rm b-jet}=0$. Because of limited statistical precision in the simulated event samples at large $N_{\rm jet}$, the transfer factors determined for the $8\leq$N_{\rm jet}$\leq 9$ region are also used for the $N_{\rm jet}10$ region. Points with error bars show the computed value in each bin with statistical uncertainties.

• Distribution of $R_{{\rm Z}/\gamma}$ with baseline selection applied in the 46 search bins with $N_{\rm b-jet}=0$. Because of limited statistical precision in the simulated event samples at large $N_{\rm jet}$, the transfer factors determined for the $8\leq$N_{\rm jet}$\leq 9$ region are also used for the $N_{\rm jet}10$ region. Points with error bars show the computed value in each bin with statistical uncertainties.:

 META FILEATTACHMENT attachment="njets-projection-pull.pdf" attr="" comment="" date="1562057157" name="njets-projection-pull.pdf" path="njets-projection-pull.pdf" size="17126" user="rpatel" version="1" attachment="nbjets-projection-pull.pdf" attr="" comment="" date="1562057157" name="nbjets-projection-pull.pdf" path="nbjets-projection-pull.pdf" size="17021" user="rpatel" version="1" attachment="mht-projection-pull.pdf" attr="" comment="" date="1562057157" name="mht-projection-pull.pdf" path="mht-projection-pull.pdf" size="17867" user="rpatel" version="1"
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 META FILEATTACHMENT attachment="1300_h_2017_CRSR_forSupplimentary_Exp_WJet.png" attr="" comment="Transfer Factor dependance on jet and b-jet multiplicity in W+jet event." date="1564651880" name="1300_h_2017_CRSR_forSupplimentary_Exp_WJet.png" path="1300_h_2017_CRSR_forSupplimentary_Exp_WJet.png" size="25926" user="arane" version="1" attachment="1300_h_2017_CRSR_forSupplimentary_Exp_TTbar.pdf" attr="" comment="Transfer Factor dependance on jet and b-jet multiplicity in ttbar event." date="1564653596" name="1300_h_2017_CRSR_forSupplimentary_Exp_TTbar.pdf" path="1300_h_2017_CRSR_forSupplimentary_Exp_TTbar.pdf" size="20110" user="arane" version="1" attachment="1300_h_2017_CRSR_forSupplimentary_Exp_TTbar.png" attr="" comment="Transfer Factor dependance on jet and b-jet multiplicity in ttbar event." date="1564653596" name="1300_h_2017_CRSR_forSupplimentary_Exp_TTbar.png" path="1300_h_2017_CRSR_forSupplimentary_Exp_TTbar.png" size="24764" user="arane" version="1"
>
>
 META FILEATTACHMENT attachment="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" attr="" comment="Distribution of single photon event yields with baseline selection applied in the 46 search bins with $N_%7b\rm b-jet%7d=0$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1565252261" name="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" path="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" size="23488" user="trmishra" version="1" attachment="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" attr="" comment="Distribution of single photon event yields with baseline selection applied in the 46 search bins with $N_%7b\rm b-jet%7d=0$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1565252290" name="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" path="AnalysisBins_BTag0_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" size="17670" user="trmishra" version="1" attachment="HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" attr="" comment="Distribution of single photon event yields with baseline selection applied and $N_%7b\rm b-jet%7d=0$ versus $H_%7b\rm T%7d$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1565252393" name="HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" path="HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" size="23320" user="trmishra" version="1" attachment="HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" attr="" comment="Distribution of single photon event yields with baseline selection applied and $N_%7b\rm b-jet%7d=0$ versus $H_%7b\rm T%7d$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1565252393" name="HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" path="HT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" size="16685" user="trmishra" version="1" attachment="MHT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" attr="" comment="Distribution of single photon event yields with baseline selection applied and $N_%7b\rm b-jet%7d=0$ versus $H^%7b\rm miss%7d_%7b\rm T%7d$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1565252493" name="MHT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" path="MHT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" size="24436" user="trmishra" version="1" attachment="MHT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" attr="" comment="Distribution of single photon event yields with baseline selection applied and $N_%7b\rm b-jet%7d=0$ versus $H^%7b\rm miss%7d_%7b\rm T%7d$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1565252525" name="MHT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" path="MHT_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" size="18293" user="trmishra" version="1" attachment="NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" attr="" comment="Distribution of single photon event yields with baseline selection applied and $N_%7b\rm b-jet%7d=0$ versus $N_%7b\rm jet%7d$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1565252623" name="NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" path="NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.pdf" size="17759" user="trmishra" version="1" attachment="NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" attr="" comment="Distribution of single photon event yields with baseline selection applied and $N_%7b\rm b-jet%7d=0$ versus $N_%7b\rm jet%7d$. Points with error bars show the observed event yields. Filled histograms show the predicted event yields from simulations, which is weighted with data/MC scale factors and measured trigger efficiencies. The ratio of observed data over simulations is shown in the lower panel." date="1565252623" name="NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" path="NJets_photon_baseline_Run2_LogY_supplementary-trig_eff-SF.png" size="14326" user="trmishra" version="1" attachment="Purity_Run2_supplementary.pdf" attr="" comment="Measured photon purity versus $H^%7b\rm miss%7d_%7b\rm T%7d$. The solid points with errors show the purity for events with a photon reconstructed in the barrel; open points with errors show the purity for events with a photon reconstructed in the endcap." date="1565252683" name="Purity_Run2_supplementary.pdf" path="Purity_Run2_supplementary.pdf" size="14666" user="trmishra" version="1" attachment="Purity_Run2_supplementary.png" attr="" comment="Measured photon purity versus $H^%7b\rm miss%7d_%7b\rm T%7d$. The solid points with errors show the purity for events with a photon reconstructed in the barrel; open points with errors show the purity for events with a photon reconstructed in the endcap." date="1565252683" name="Purity_Run2_supplementary.png" path="Purity_Run2_supplementary.png" size="15909" user="trmishra" version="1" attachment="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.pdf" attr="" comment="Distribution of $R_%7b%7b\rm Z%7d/\gamma%7d$ with baseline selection applied in the 46 search bins with $N_%7b\rm b-jet%7d=0$. Because of limited statistical precision in the simulated event samples at large $N_%7b\rm jet%7d$, the transfer factors determined for the $8\leq$N_%7b\rm jet%7d$\leq 9$ region are also used for the $N_%7b\rm jet%7d10$ region. Points with error bars show the computed value in each bin with statistical uncertainties." date="1565253082" name="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.pdf" path="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.pdf" size="16980" user="trmishra" version="1" attachment="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.png" attr="" comment="Distribution of $R_%7b%7b\rm Z%7d/\gamma%7d$ with baseline selection applied in the 46 search bins with $N_%7b\rm b-jet%7d=0$. Because of limited statistical precision in the simulated event samples at large $N_%7b\rm jet%7d$, the transfer factors determined for the $8\leq$N_%7b\rm jet%7d$\leq 9$ region are also used for the $N_%7b\rm jet%7d10$ region. Points with error bars show the computed value in each bin with statistical uncertainties." date="1565253082" name="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.png" path="AnalysisBins_BTag0_RzGamma_Run2_signal_ZJets_supplementary.png" size="13866" user="trmishra" version="1"

#### Revision 142019-08-08 - TribeniMishra1

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 META TOPICPARENT name="PhysicsResultsSUS"

# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

#### Revision 132019-08-07 - RishiPatel

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 META TOPICPARENT name="PhysicsResultsSUS"

# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

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| | Figure Zn : Double ratio vs. (left), (center), and (right). Events in the simulated +jets sample have been weighted by the reciprocal of the -dependent function represented by the green dot-dashed line in the left-hand panel. The average value of this function is 0.95. Points with error bars show the value of in each bin with statistical uncertainties. The solid and dashed blue lines show the straight-line fit and uncertainties propagated from the fit, respectively. The average value, 1.00, is drawn as a red dashed line on each plot. |
Latex rendering error!! dvi file was not created.
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 Figure Zn : Double ratio vs. (left), (center), and Events in the simulated +jets sample have been weighted by the reciprocal of the -dependent function represented by the green dot-dashed line in the left-hand panel. The average value of this function is 0.95. Points with error bars show the value of in each bin with statistical uncertainties. The solid and dashed blue lines show the straight-line fit and uncertainties propagated from the fit, respectively. The average value, 1.00, is drawn as a red dashed line on each plot.

 Figure Zma : Representative dilepton mass distributions from the +jets control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (a) with , .
Changed:
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 Figure Zmb : Representative dilepton mass distributions from the \!+jets\xspace control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (b) with , . Figure Zmc : Representative dilepton mass distributions from the \!+jets\xspace control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (c) with , .
| | Figure Zmd : Representative dilepton mass distributions from the \!+jets\xspace control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (d) with , . |
Latex rendering error!! dvi file was not created.
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 Figure Zmb : Representative dilepton mass distributions from the +jets control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (b) with , .

 Figure Zmc : Representative dilepton mass distributions from the +jets control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (c) with , .

 Figure Zmd : Representative dilepton mass distributions from the +jets control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (d) with , .

 Figure LLa : Lost lepton background in signal region decomposed as that from ttbar, W+jets and Single top in different bins of , , number of jets () and number of b-tagged jets (). Each pie-chart for a given search variable is inclusive in other three search variables with baseline selections applied.
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 Figure LLb : (Top) Stacked distribution for W+jets showing relative fractions of “Single lepton” and three sub-categories of “Lost lepton” events (lost due to out of acceptance, failing ID/isolation requirement or having hadronically decaying tau) parameterized in bins of number of jets () and number of b-tagged jets (). Uncertainties are statistical only. (Bottom) Ratio of "Lost lepton" (combining three sub-categories) to "Single lepton" fraction parameterized in number of jets () and number of b-tagged jets (). Figure LLc : (Top) Stacked distribution for ttbar showing relative fractions of “Single lepton” and three sub-categories of “Lost lepton” events (lost due to out of acceptance, failing ID/isolation requirement or having hadronically decaying tau) parameterized in bins of number of jets () and number of b-tagged jets (). Uncertainties are statistical only. (Bottom) Ratio of "Lost lepton" (combining three sub-categories) to "Single lepton" fraction parameterized in number of jets () and number of b-tagged jets ().
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## Results: yields vs. background prediction, select kinematic distributions

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# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

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 Figure Zmb : Representative dilepton mass distributions from the \!+jets\xspace control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (b) with , . Figure Zmc : Representative dilepton mass distributions from the \!+jets\xspace control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (c) with , .
| | Figure Zmd : Representative dilepton mass distributions from the \!+jets\xspace control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (d) with , . |
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 Figure LLa : Lost lepton background in signal region decomposed as that from ttbar, W+jets and Single top in different bins of , , number of jets () and number of b-tagged jets (). Each pie-chart for a given search variable is inclusive in other three search variables with baseline selections applied. Figure LLb : (Top) Stacked distribution for W+jets showing relative fractions of “Single lepton” and three sub-categories of “Lost lepton” events (lost due to out of acceptance, failing ID/isolation requirement or having hadronically decaying tau) parameterized in bins of number of jets () and number of b-tagged jets (). Uncertainties are statistical only. (Bottom) Ratio of "Lost lepton" (combining three sub-categories) to "Single lepton" fraction parameterized in number of jets () and number of b-tagged jets (). Figure LLc : (Top) Stacked distribution for ttbar showing relative fractions of “Single lepton” and three sub-categories of “Lost lepton” events (lost due to out of acceptance, failing ID/isolation requirement or having hadronically decaying tau) parameterized in bins of number of jets () and number of b-tagged jets (). Uncertainties are statistical only. (Bottom) Ratio of "Lost lepton" (combining three sub-categories) to "Single lepton" fraction parameterized in number of jets () and number of b-tagged jets ().

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#### Revision 112019-07-27 - WilliamFord

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 META TOPICPARENT name="PhysicsResultsSUS"

# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

#### Revision 102019-07-26 - WilliamFord

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 META TOPICPARENT name="PhysicsResultsSUS"

# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

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| | Figure Zn : Double ratio vs. (left), (center), and (right). Events in the simulated +jets sample have been weighted by the reciprocal of the -dependent function represented by the green dot-dashed line in the left-hand panel. The average value of this function is 0.95. Points with error bars show the value of in each bin with statistical uncertainties. The solid and dashed blue lines show the straight-line fit and uncertainties propagated from the fit, respectively. The average value, 1.00, is drawn as a red dashed line on each plot. |
Latex rendering error!! dvi file was not created.
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| | Figure Zma : Representative dilepton mass distributions from the \!+jets\xspace control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (a) with , . |
Latex rendering error!! dvi file was not created.
>
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 Figure Zma : Representative dilepton mass distributions from the +jets control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (a) with , .

 Figure Zmb : Representative dilepton mass distributions from the \!+jets\xspace control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (b) with , .
| | Figure Zmc : Representative dilepton mass distributions from the \!+jets\xspace control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (c) with , . |
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| | Figure Zmd : Representative dilepton mass distributions from the \!+jets\xspace control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within with , . |
Latex rendering error!! dvi file was not created.
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| | Figure Zmd : Representative dilepton mass distributions from the \!+jets\xspace control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (d) with , . |
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#### Revision 92019-07-25 - WilliamFord

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 META TOPICPARENT name="PhysicsResultsSUS"

# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

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| | Figure Zn : Double ratio vs. (left), (center), and (right). Events in the simulated +jets sample have been weighted by the reciprocal of the -dependent function represented by the green dot-dashed line in the left-hand panel. The average value of this function is 0.95. Points with error bars show the value of in each bin with statistical uncertainties. The solid and dashed blue lines show the straight-line fit and uncertainties propagated from the fit, respectively. The average value, 1.00, is drawn as a red dashed line on each plot. |
Latex rendering error!! dvi file was not created.
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 Figure Zma : Representative dilepton mass distributions from the \!+jets\xspace control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (a) with , . Figure Zmb : Representative dilepton mass distributions from the \!+jets\xspace control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (b) with , . Figure Zmc : Representative dilepton mass distributions from the \!+jets\xspace control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within GeV of the Z boson mass. The stacked distributions from simulation serve to show the approximate composition of the sample, but play no role in the fit or purity measurement. (c) with , .
| | Figure Zmd : Representative dilepton mass distributions from the \!+jets\xspace control sample. The solid blue curve is the result of a fit to the data of a function with peaking signal and continuum background components; the dashed line represents the background. The purity of the sample is given by the ratio of signal to total areas within with , . |
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#### Revision 82019-07-23 - WilliamFord

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# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

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 Figure Zn : (Under construction)
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| | Figure Zn : Double ratio vs. (left), (center), and (right). Events in the simulated +jets sample have been weighted by the reciprocal of the -dependent function represented by the green dot-dashed line in the left-hand panel. The average value of this function is 0.95. Points with error bars show the value of in each bin with statistical uncertainties. The solid and dashed blue lines show the straight-line fit and uncertainties propagated from the fit, respectively. The average value, 1.00, is drawn as a red dashed line on each plot. |
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#### Revision 72019-07-23 - WilliamFord

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# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

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Figure Caption
Figure Zn : (Under construction)

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#### Revision 62019-07-19 - RishiPatel

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# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

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Figure Caption
Figure 5 : The same distributions shown in Fig. 10 in the body of the paper, with the pull for each bin, defined as , shown in the lower panel of the plot.
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 Figure 6a : The sensitivity of the analysis to different direct gluino production signal models as a function of the analysis binning. The upper panel shows the total predicted SM backgrounds and the expected number of signal events in 137 of data for six representative model points per analysis bin. The bottom panel shows the expected sensitivity, expressed in terms of the figure of merit Q, per analysis bin.

 Figure 6b : The sensitivity of the analysis to different direct squark production signal models as a function of the analysis binning. The upper panel shows the total predicted SM backgrounds and the expected number of signal events in 137 of data for six representative model points per analysis bin. The bottom panel shows the expected sensitivity, expressed in terms of the figure of merit Q, per analysis bin.

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#### Revision 52019-07-19 - RishiPatel

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 META TOPICPARENT name="PhysicsResultsSUS"

# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

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This analysis is documented in arxiv:1704.07781 and the public webpage for this analysis is http://cms-results.web.cern.ch/cms-results/public-results/publications/SUS-16-033/

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This analysis is documented in http://cds.cern.ch/record/2682103 and the public webpage for this analysis is http://cms-results.web.cern.ch/cms-results/public-results/preliminary-results/SUS-19-006/index.html/

# Technical plots for CMS speakers (click on plots to get larger pdf versions)

#### Revision 42019-07-04 - AlexxPerloff

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 META TOPICPARENT name="PhysicsResultsSUS"

# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

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 Figure 24a : Event displays for a SUSY candidate event with 12 jets in the search region, 273447:179:291867669 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the non b-tagged jets are marked and labeled in orange and the momenta of the b-tagged jets are marked in green. Figure 24b : Event displays for a SUSY candidate event with 12 jets in the search region, 273447:179:291867669 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the non b-tagged jets are marked and labeled in orange and the momenta of the b-tagged jets are marked in green. Figure 24c : Event displays for a SUSY candidate event with 12 jets in the search region, 273447:179:291867669 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the non b-tagged jets are marked and labeled in orange and the momenta of the b-tagged jets are marked in green. Figure 24d : Event displays for a SUSY candidate event with 12 jets in the search region, 273447:179:291867669 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the non b-tagged jets are marked and labeled in orange and the momenta of the b-tagged jets are marked in green.
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 Figure 8a : Event displays for a SUSY candidate event with 12 jets in the search region, 273447:179:291867669 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the non b-tagged jets are marked and labeled in orange and the momenta of the b-tagged jets are marked in green. Figure 8b : Event displays for a SUSY candidate event with 12 jets in the search region, 273447:179:291867669 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the non b-tagged jets are marked and labeled in orange and the momenta of the b-tagged jets are marked in green. Figure 8c : Event displays for a SUSY candidate event with 12 jets in the search region, 273447:179:291867669 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the non b-tagged jets are marked and labeled in orange and the momenta of the b-tagged jets are marked in green. Figure 8d : Event displays for a SUSY candidate event with 12 jets in the search region, 273447:179:291867669 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the non b-tagged jets are marked and labeled in orange and the momenta of the b-tagged jets are marked in green.

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 Figure 25a : Event displays for a SUSY candidate event with very high in the search region, 321219:344:504952772 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the two jets are marked and labeled in orange. Figure 25b : Event displays for a SUSY candidate event with very high in the search region, 321219:344:504952772 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the two jets are marked and labeled in orange. Figure 25c : Event displays for a SUSY candidate event with very high in the search region, 321219:344:504952772 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the two jets are marked and labeled in orange. Figure 25d : Event displays for a SUSY candidate event with very high in the search region, 321219:344:504952772 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the two jets are marked and labeled in orange.
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 Figure 9a : Event displays for a SUSY candidate event with very high in the search region, 321219:344:504952772 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the two jets are marked and labeled in orange. Figure 9b : Event displays for a SUSY candidate event with very high in the search region, 321219:344:504952772 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the two jets are marked and labeled in orange. Figure 9c : Event displays for a SUSY candidate event with very high in the search region, 321219:344:504952772 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the two jets are marked and labeled in orange. Figure 9d : Event displays for a SUSY candidate event with very high in the search region, 321219:344:504952772 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the two jets are marked and labeled in orange.

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 Figure 26a : Event displays for a T1bbbb-like candidate in the search region with exactly 4 jets, all of which are b-tagged, 321295:60:95701713 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the four b-tagged jets are marked and labeled in green. Figure 26b : Event displays for a T1bbbb-like candidate in the search region with exactly 4 jets, all of which are b-tagged, 321295:60:95701713 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the four b-tagged jets are marked and labeled in green. Figure 26c : Event displays for a T1bbbb-like candidate in the search region with exactly 4 jets, all of which are b-tagged, 321295:60:95701713 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the four b-tagged jets are marked and labeled in green. Figure 26d : Event displays for a T1bbbb-like candidate in the search region with exactly 4 jets, all of which are b-tagged, 321295:60:95701713 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the four b-tagged jets are marked and labeled in green.
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 Figure 10a : Event displays for a T1bbbb-like candidate in the search region with exactly 4 jets, all of which are b-tagged, 321295:60:95701713 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the four b-tagged jets are marked and labeled in green. Figure 10b : Event displays for a T1bbbb-like candidate in the search region with exactly 4 jets, all of which are b-tagged, 321295:60:95701713 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the four b-tagged jets are marked and labeled in green. Figure 10c : Event displays for a T1bbbb-like candidate in the search region with exactly 4 jets, all of which are b-tagged, 321295:60:95701713 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the four b-tagged jets are marked and labeled in green. Figure 10d : Event displays for a T1bbbb-like candidate in the search region with exactly 4 jets, all of which are b-tagged, 321295:60:95701713 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the four b-tagged jets are marked and labeled in green.

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#### Revision 32019-07-03 - AlexxPerloff

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 META TOPICPARENT name="PhysicsResultsSUS"

# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

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Figure Caption
Figure 24a : Event displays for a SUSY candidate event with 12 jets in the search region, 273447:179:291867669 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the non b-tagged jets are marked and labeled in orange and the momenta of the b-tagged jets are marked in green.
Figure 24b : Event displays for a SUSY candidate event with 12 jets in the search region, 273447:179:291867669 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the non b-tagged jets are marked and labeled in orange and the momenta of the b-tagged jets are marked in green.
Figure 24c : Event displays for a SUSY candidate event with 12 jets in the search region, 273447:179:291867669 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the non b-tagged jets are marked and labeled in orange and the momenta of the b-tagged jets are marked in green.
Figure 24d : Event displays for a SUSY candidate event with 12 jets in the search region, 273447:179:291867669 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the non b-tagged jets are marked and labeled in orange and the momenta of the b-tagged jets are marked in green.

Figure Caption
Figure 25a : Event displays for a SUSY candidate event with very high in the search region, 321219:344:504952772 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the two jets are marked and labeled in orange.
Figure 25b : Event displays for a SUSY candidate event with very high in the search region, 321219:344:504952772 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the two jets are marked and labeled in orange.
Figure 25c : Event displays for a SUSY candidate event with very high in the search region, 321219:344:504952772 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the two jets are marked and labeled in orange.
Figure 25d : Event displays for a SUSY candidate event with very high in the search region, 321219:344:504952772 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the two jets are marked and labeled in orange.

Figure Caption
Figure 26a : Event displays for a T1bbbb-like candidate in the search region with exactly 4 jets, all of which are b-tagged, 321295:60:95701713 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the four b-tagged jets are marked and labeled in green.
Figure 26b : Event displays for a T1bbbb-like candidate in the search region with exactly 4 jets, all of which are b-tagged, 321295:60:95701713 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the four b-tagged jets are marked and labeled in green.
Figure 26c : Event displays for a T1bbbb-like candidate in the search region with exactly 4 jets, all of which are b-tagged, 321295:60:95701713 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the four b-tagged jets are marked and labeled in green.
Figure 26d : Event displays for a T1bbbb-like candidate in the search region with exactly 4 jets, all of which are b-tagged, 321295:60:95701713 in (a) view, (b) view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the four b-tagged jets are marked and labeled in green.

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The momenta of the two jets are marked and labeled in orange." date="1562173003" name="321219_344_504952772_3DTower_BlackBackground.png" path="321219_344_504952772_3DTower_BlackBackground.png" size="7770427" user="aperloff" version="1" attachment="321219_344_504952772_3DTower_WhiteBackground.png" attr="" comment="Event displays for a SUSY candidate event with very high %25$H_%7b\rm T%7d^%7b\rm miss%7d$%25 in the search region, 321219:344:504952772 in (a) %25$r-\phi$%25 view, (b) %25$r-\phi$%25 view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the two jets are marked and labeled in orange." date="1562173024" name="321219_344_504952772_3DTower_WhiteBackground.png" path="321219_344_504952772_3DTower_WhiteBackground.png" size="9495912" user="aperloff" version="1" attachment="321219_344_504952772_RhoPhi_BlackBackground.png" attr="" comment="Event displays for a SUSY candidate event with very high %25$H_%7b\rm T%7d^%7b\rm miss%7d$%25 in the search region, 321219:344:504952772 in (a) %25$r-\phi$%25 view, (b) %25$r-\phi$%25 view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the two jets are marked and labeled in orange." date="1562173032" name="321219_344_504952772_RhoPhi_BlackBackground.png" path="321219_344_504952772_RhoPhi_BlackBackground.png" size="2515339" user="aperloff" version="1" attachment="321219_344_504952772_RhoPhi_WhiteBackground.png" attr="" comment="Event displays for a SUSY candidate event with very high %25$H_%7b\rm T%7d^%7b\rm miss%7d$%25 in the search region, 321219:344:504952772 in (a) %25$r-\phi$%25 view, (b) %25$r-\phi$%25 view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the two jets are marked and labeled in orange." date="1562173039" name="321219_344_504952772_RhoPhi_WhiteBackground.png" path="321219_344_504952772_RhoPhi_WhiteBackground.png" size="2675119" user="aperloff" version="1" attachment="321295_60_95701713_3DTower_BlackBackground.pdf" attr="" comment="Event displays for a T1bbbb-like candidate in the search region with exactly 4 jets, all of which are b-tagged, 321295:60:95701713 in (a) %25$r-\phi$%25 view, (b) %25$r-\phi$%25 view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the four b-tagged jets are marked and labeled in green." date="1562173099" name="321295_60_95701713_3DTower_BlackBackground.pdf" path="321295_60_95701713_3DTower_BlackBackground.pdf" size="1594465" user="aperloff" version="1" attachment="321295_60_95701713_3DTower_WhiteBackground.pdf" attr="" comment="Event displays for a T1bbbb-like candidate in the search region with exactly 4 jets, all of which are b-tagged, 321295:60:95701713 in (a) %25$r-\phi$%25 view, (b) %25$r-\phi$%25 view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the four b-tagged jets are marked and labeled in green." date="1562173101" name="321295_60_95701713_3DTower_WhiteBackground.pdf" path="321295_60_95701713_3DTower_WhiteBackground.pdf" size="1800369" user="aperloff" version="1" attachment="321295_60_95701713_RhoPhi_BlackBackground.pdf" attr="" comment="Event displays for a T1bbbb-like candidate in the search region with exactly 4 jets, all of which are b-tagged, 321295:60:95701713 in (a) %25$r-\phi$%25 view, (b) %25$r-\phi$%25 view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the four b-tagged jets are marked and labeled in green." date="1562173103" name="321295_60_95701713_RhoPhi_BlackBackground.pdf" path="321295_60_95701713_RhoPhi_BlackBackground.pdf" size="983939" user="aperloff" version="1" attachment="321295_60_95701713_RhoPhi_WhiteBackground.pdf" attr="" comment="Event displays for a T1bbbb-like candidate in the search region with exactly 4 jets, all of which are b-tagged, 321295:60:95701713 in (a) %25$r-\phi$%25 view, (b) %25$r-\phi$%25 view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the four b-tagged jets are marked and labeled in green." date="1562173104" name="321295_60_95701713_RhoPhi_WhiteBackground.pdf" path="321295_60_95701713_RhoPhi_WhiteBackground.pdf" size="962950" user="aperloff" version="1" attachment="321295_60_95701713_3DTower_BlackBackground.png" attr="" comment="Event displays for a T1bbbb-like candidate in the search region with exactly 4 jets, all of which are b-tagged, 321295:60:95701713 in (a) %25$r-\phi$%25 view, (b) %25$r-\phi$%25 view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the four b-tagged jets are marked and labeled in green." date="1562173110" name="321295_60_95701713_3DTower_BlackBackground.png" path="321295_60_95701713_3DTower_BlackBackground.png" size="7921993" user="aperloff" version="1" attachment="321295_60_95701713_3DTower_WhiteBackground.png" attr="" comment="Event displays for a T1bbbb-like candidate in the search region with exactly 4 jets, all of which are b-tagged, 321295:60:95701713 in (a) %25$r-\phi$%25 view, (b) %25$r-\phi$%25 view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the four b-tagged jets are marked and labeled in green." date="1562173116" name="321295_60_95701713_3DTower_WhiteBackground.png" path="321295_60_95701713_3DTower_WhiteBackground.png" size="9644098" user="aperloff" version="1" attachment="321295_60_95701713_RhoPhi_BlackBackground.png" attr="" comment="Event displays for a T1bbbb-like candidate in the search region with exactly 4 jets, all of which are b-tagged, 321295:60:95701713 in (a) %25$r-\phi$%25 view, (b) %25$r-\phi$%25 view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the four b-tagged jets are marked and labeled in green." date="1562173118" name="321295_60_95701713_RhoPhi_BlackBackground.png" path="321295_60_95701713_RhoPhi_BlackBackground.png" size="2766722" user="aperloff" version="1" attachment="321295_60_95701713_RhoPhi_WhiteBackground.png" attr="" comment="Event displays for a T1bbbb-like candidate in the search region with exactly 4 jets, all of which are b-tagged, 321295:60:95701713 in (a) %25$r-\phi$%25 view, (b) %25$r-\phi$%25 view with a white background, (c) 3D view, and (d) 3D view with a white background. The momenta of the four b-tagged jets are marked and labeled in green." date="1562173120" name="321295_60_95701713_RhoPhi_WhiteBackground.png" path="321295_60_95701713_RhoPhi_WhiteBackground.png" size="2864349" user="aperloff" version="1"

#### Revision 22019-07-02 - AlexxPerloff

Line: 1 to 1

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# Search for supersymmetry in proton-proton collisions at 13TeV using 137\fbinv of data in final states with jets and missing transverse momentum (SUS-19-006)

#### Revision 12019-07-02 - RishiPatel

Line: 1 to 1
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 META TOPICPARENT name="PhysicsResultsSUS"

# Further information

This analysis is documented in arxiv:1704.07781 and the public webpage for this analysis is http://cms-results.web.cern.ch/cms-results/public-results/publications/SUS-16-033/

# Technical plots for CMS speakers (click on plots to get larger pdf versions)

## SM Backgrounds

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## Results: yields vs. background prediction, select kinematic distributions

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Figure Caption
Figure 1a : One-dimensional projection of observed number of events and pre-fit background predictions in the search region in with the pull for each bin, defined as , shown in the lower panel of the plot.
Figure 1b : One-dimensional projection of observed number of events and pre-fit background predictions in the search region in .
Figure 1c: One-dimensional projection of observed number of events and pre-fit background predictions in the search region in .

| | Figure 2a : The same distributions shown in Fig. 11a in the body of the paper, with the pull for each bin, defined as , shown in the lower panel of the plot.
 Figure 2b : The same distributions shown in Fig. 11b in the body of the paper, with the pull for each bin, defined as , shown in the lower panel of the plot. Figure 2c : The same distributions shown in Fig. 11c in the body of the paper, with the pull for each bin, defined as , shown in the lower panel of the plot. Figure 2d : The same distributions shown in Fig. 11d in the body of the paper, with the pull for each bin, defined as , shown in the lower panel of the plot. Figure 2e : The same distributions shown in Fig. 11e in the body of the paper, with the pull for each bin, defined as , shown in the lower panel of the plot. Figure 2f : The same distributions shown in Fig. 11f in the body of the paper, with the pull for each bin, defined as , shown in the lower panel of the plot.

Figure Caption
Figure 3a : Observed numbers of events and corresponding SM background predictions in intervals of and , integrated over search regions with GeV and GeV. An example T1tttt signal scenario with GeV and GeV is shown by the (stacked) purple histogram.
Figure 3b : The same distributions shown in Add. Fig. 21a, with the pull for each bin, defined as , shown in the lower panel of the plot.
Figure 3c : Observed numbers of events and corresponding SM background predictions in intervals of and , integrated over search regions with GeV and GeV. An example T1bbbb signal scenario with GeV and GeV is shown by the (stacked) purple histogram.
Figure 3d : The same distributions shown in Add. Fig. 21c, with the pull for each bin, defined as , shown in the lower panel of the plot.
Figure 3e : Observed numbers of events and corresponding SM background predictions in intervals of and , integrated over search regions with GeV and GeV. An example T1qqqq signal scenario with GeV and GeV is shown by the (stacked) purple histogram.
Figure 3f : The same distributions shown in Add. Fig. 21e, with the pull for each bin, defined as , shown in the lower panel of the plot.
Figure 3g : Observed numbers of events and corresponding SM background predictions in intervals of and , integrated over search regions with GeV and GeV. An example T2tt signal scenario with GeV and GeV is shown by the (stacked) purple histogram.
Figure 3h : The same distributions shown in Add. Fig. 21g, with the pull for each bin, defined as , shown in the lower panel of the plot.
Figure 3i : Observed numbers of events and corresponding SM background predictions in intervals of and , integrated over search regions with GeV and GeV. An example T2bb signal scenario with GeV and GeV is shown by the (stacked) purple histogram.
Figure 3j : The same distributions shown in Add. Fig. 21i, with the pull for each bin, defined as , shown in the lower panel of the plot.
Figure 3k : Observed numbers of events and corresponding SM background predictions in intervals of and , integrated over search regions with GeV and GeV. An example T2qq signal scenario with GeV and GeV is shown by the (stacked) purple histogram.
Figure 3l : The same distributions shown in Add. Fig. 21k, with the pull for each bin, defined as , shown in the lower panel of the plot.

Figure Caption
Figure 4 : The same distributions shown in Fig. 9 in the body of the paper, with the pull for each bin, defined as , shown in the lower panel of the plot.

Figure Caption
Figure 5 : The same distributions shown in Fig. 10 in the body of the paper, with the pull for each bin, defined as , shown in the lower panel of the plot.

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## Event displays

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-- RishiPatel - 2019-07-02

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