Difference: PhysicsResultsSUS12024 (1 vs. 12)

Revision 122014-10-23 - KeithUlmer

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META TOPICPARENT name="PhysicsResultsSUS"

Search for gluino-mediated bottom- and top-squark production in pp collisions at 8 TeV

Line: 236 to 236
 
Added:
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Interpretation of the results with simplified models with Higgs

Schematic view of the simplified models

Figure Formats Caption
pdf, png Figure: Diagrams representing the T5Wh simplified model: Gluino pair production with , , and , .
pdf, png Figure: Diagrams representing the T5hh simplified model: Gluino pair production with , .

T5Wh

Figure Formats Caption
pdf, png Signal efficiency for the T5Wh simplified model, as a function of the mass of the gluino (x axis) and the mass of the neutralino 1 (y axis).
pdf, png The 95 % CL upper limits on the T5Wh simplified model cross sections (pb) derived using the toy CLs method. The solid (black) contours show the observed exclusions, along with the +/- 1 standard deviation theory uncertainties. The dashed (red) contours present the corresponding expected results, along with the +/- 1 standard deviation experimental uncertainties.

T5hh

Figure Formats Caption
pdf, png Signal efficiency for the T5hh simplified model, as a function of the mass of the gluino (x axis) and the mass of the neutralino 1 (y axis).
pdf, png The 95 % CL upper limits on the T5Wh simplified model cross sections (pb) derived using the toy CLs method. The solid (black) contours show the observed exclusions, along with the +/- 1 standard deviation theory uncertainties. The dashed (red) contours present the corresponding expected results, along with the +/- 1 standard deviation experimental uncertainties.

Additional plots

Figure Formats Caption
pdf, png Signal efficiency without the MET cut for the T5Wh simplified model, as a function of the mass of the gluino (x axis) and the mass of the neutralino 1 (y axis).
pdf, png Signal efficiency without the minDeltaPhiN cut for the T5Wh simplified model, as a function of the mass of the gluino (x axis) and the mass of the neutralino 1 (y axis).
pdf, png Signal efficiency without either the MET or the minDeltaPhiN cuts for the T5Wh simplified model, as a function of the mass of the gluino (x axis) and the mass of the neutralino 1 (y axis).
pdf, png Number of reconstructed jets of 50 GeV for the T5Wh signal with a gluino mass of 1 TeV and various LSP masses.
pdf, png MET distribution for the T5Wh signal with a gluino mass of 1 TeV and various LSP masses.
pdf, png minDeltaPhiN distribution for the T5Wh signal with a gluino mass of 1 TeV and various LSP masses.
pdf, png HT distribution for the T5hh signal with a gluino mass of 1 TeV and various LSP masses.
 
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Revision 112014-05-16 - AlessandroGaz

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META TOPICPARENT name="PhysicsResultsSUS"

Search for gluino-mediated bottom- and top-squark production in pp collisions at 8 TeV

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Changed:
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Revision 102013-09-09 - AlessandroGaz

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META TOPICPARENT name="PhysicsResultsSUS"

Search for gluino-mediated bottom- and top-squark production in pp collisions at 8 TeV

Line: 128 to 128
 
Figure Caption
Simplified model topology "T1bbbb".
Simplified model topology "T1tttt".
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Simplified model topologies "T5tttt" and "T1t1t".
Simplified model topology "T7btW".
 

Interpretation of the results with additional simplified models

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Revision 92013-09-07 - WilliamFord

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

Search for gluino-mediated bottom- and top-squark production in pp collisions at 8 TeV

Line: 129 to 129
 
Simplified model topology "T1bbbb".
Simplified model topology "T1tttt".
Added:
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Interpretation of the results with additional simplified models

T7btw, m(chi+) = 150 GeV

Figure Caption
Acceptance x selection efficiency (for the zero-lepton sample) on the T7btw simplified model, with m(chi+) = 150 GeV, as a function of the mass of the gluino (x axis) and the mass of the sbottom (y axis). The root macro that can be used to reproduce this plot is T7btwmChi150_eff_RA2bXSEC.C.
The 95 % CL upper limits on the T7btw simplified model (with m(chi+) = 150 GeV) cross sections (pb) derived using the CLs method. The solid (black) contours show the observed exclusions assuming the NLO+NLL cross sections, along with the +/- 1 standard deviation theory uncertainties. The dashed (red) contours present the corresponding expected results, along with the +/- 1 standard deviation experimental uncertainties. The root macro that can be used to reproduce this plot is T7btwmChi150RA2bXSEC.C.

T7btw, m(chi+) = 300 GeV

Figure Caption
Acceptance x selection efficiency (for the zero-lepton sample) on the T7btw simplified model, with m(chi+) = 300 GeV, as a function of the mass of the gluino (x axis) and the mass of the sbottom (y axis). The root macro that can be used to reproduce this plot is T7btwmChi300_eff_RA2bXSEC.C.
The 95 % CL upper limits on the T7btw simplified model (with m(chi+) = 300 GeV) cross sections (pb) derived using the CLs method. The solid (black) contours show the observed exclusions assuming the NLO+NLL cross sections, along with the +/- 1 standard deviation theory uncertainties. The dashed (red) contours present the corresponding expected results, along with the +/- 1 standard deviation experimental uncertainties. The root macro that can be used to reproduce this plot is T7btwmChi300RA2bXSEC.C.

T5tttt

Figure Caption
Acceptance x selection efficiency (for the zero-lepton sample) on the T5tttt simplified model as a function of the mass of the gluino (x axis) and the mass of the stop (y axis). The mass of the neutralino is fixed to 50 GeV. The root macro that can be used to reproduce this plot is T5tttt_eff_RA2bXSEC.C.
The 95 % CL upper limits on the T5tttt simplified model cross sections (pb) derived using the CLs method. The solid (black) contours show the observed exclusions assuming the NLO+NLL cross sections, along with the +/- 1 standard deviation theory uncertainties. The dashed (red) contours present the corresponding expected results, along with the +/- 1 standard deviation experimental uncertainties. Cross section limits are presented for m(g ̃) - m(t ̃) > 200 GeV to ensure on-shell top quarks in the final state. As the t ̃ mass decreases with fixed χ ̃01 mass, the χ ̃01 momentum in the t ̃ rest frame decreases. This results in less MET in the event, and thus less sensitivity in this search. The root macro that can be used to reproduce this plot is T5ttttRA2bXSEC.C.

T1t1t

Figure Caption
Acceptance x selection efficiency (for the zero-lepton sample) on the T1t1t simplified model as a function of the mass of the stop (x axis) and the mass of the neutralino (y axis). The mass of the gluino is fixed to 1000 GeV. The root macro that can be used to reproduce this plot is T1t1t_eff_RA2bXSEC.C.
The 95 % CL upper limits on the T1t1t simplified model cross sections (pb) derived using the CLs method. The solid (black) contours show the observed exclusions assuming the NLO+NLL cross sections, along with the +/- 1 standard deviation theory uncertainties. The dashed (red) contours present the corresponding expected results, along with the +/- 1 standard deviation experimental uncertainties. Cross section limits are presented for m(t ̃) - m( χ ̃01) > 100 GeV to ensure on-shell W bosons from the top decay. As the stop mass decreases with fixed χ ̃01 mass, the χ ̃01 momentum in the t ̃ rest frame decreases. This results in less MET in the event, and thus less sensitivity in this search. The root macro that can be used to reproduce this plot is T1t1tRA2bXSEC.C.
 

Interpretation of the results within the pMSSM framework

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Revision 82013-08-27 - LukasVanelderen

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META TOPICPARENT name="PhysicsResultsSUS"

Search for gluino-mediated bottom- and top-squark production in pp collisions at 8 TeV

Line: 148 to 148
  The posterior distribution is obtained by weighting each of the 7300 pMSSM points with L(SUS-12-024|theta). Posterior and prior distribution are normalized to one.
  1. excluded vs not excluded: we compare the distribution of the 7300 pMSSM points to the distribution of those pMSSM points that are excluded by SUS-12-024 and the distribution of those points not excluded by SUS-12-024.
Changed:
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A pMSSM point is considered excluded if Z = sign(ln(B_10))sqrt(2*|ln B_10|) < -1.68, with B_10 = L(SUS-12-024|theta)/L(SUS-12-024|H_0), where L(SUS-12-024|H_0) is the likelihood for the background
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A pMSSM point is considered excluded if Z = sign(ln(B_10))sqrt(2*|ln B_10|) < -1.64, with B_10 = L(SUS-12-024|theta)/L(SUS-12-024|H_0), where L(SUS-12-024|H_0) is the likelihood for the background
  only hypothesis H_0. Z is a signed analog of the frequentist "n-sigma".

Fully Bayesian approach

Revision 72013-08-21 - LukasVanelderen

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META TOPICPARENT name="PhysicsResultsSUS"

Search for gluino-mediated bottom- and top-squark production in pp collisions at 8 TeV

Line: 130 to 130
 
Simplified model topology "T1tttt".
Changed:
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pMSSM interpretations

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Interpretation of the results within the pMSSM framework

 
Changed:
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For details on the definition and structure of the pMSSM model, and how the points to be tested by the analyses are generated, see the 7 TeV CMS pMSSM analysis documented on this twiki. The 8 TeV scan used here was generated using the same approach.
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Introduction

 
Changed:
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For each pMSSM point, we calculate the maximum likelihood value of the fit, fixing the SUSY signal yield to the expectations given by the selection efficiency and predicted cross-section. This value is compared to the maximum likelihood value of the background only hypothesis. The pMSSM points having a negative log-likelihood value which exceed 1.35 units the log-likelihood of the background only hypothesis are excluded at 95% CL (one sided).
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We show results of a phenomenological MSSM interpretation of the 8 TeV HT + MET + b-jets analysis SUS-12-024.
 
Changed:
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The analysis has sensitivity to a large fraction of the model points with accessible masses for the gluino. In addition to the simplified topologies shown explicitly in the main results, gluino decays are flavor blind and often have b-quarks in their decay chains. In addition, many SUSY cascades contain Z or higgs bosons that often lead to b-enriched final states.
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We follow the approach of the phenomenological MSSM interpretation of 7 TeV CMS results, documented in the approved PAS SUS-12-030: About 7300 points in pMSSM parameter space are sampled from an evidence-based prior probability density, based on theoretical predictions and measurements of flavour observables, Higgs mass, top mass, bottom mass and anomalous magnetic moment of the muon. For each pMSSM point theta we calculate the likelihood L(SUS-12-024|theta).

Results are presented as distributions of pMSSM parameters, masses and other observables, in two ways:

  1. A fully Bayesian approach: the prior distribution is compared to the posterior distribution including the SUS-12-024 data. The prior distribution is simply the distribution of the 7300 pMSSM points. The posterior distribution is obtained by weighting each of the 7300 pMSSM points with L(SUS-12-024|theta). Posterior and prior distribution are normalized to one.
  2. excluded vs not excluded: we compare the distribution of the 7300 pMSSM points to the distribution of those pMSSM points that are excluded by SUS-12-024 and the distribution of those points not excluded by SUS-12-024. A pMSSM point is considered excluded if Z = sign(ln(B_10))sqrt(2*|ln B_10|) < -1.68, with B_10 = L(SUS-12-024|theta)/L(SUS-12-024|H_0), where L(SUS-12-024|H_0) is the likelihood for the background only hypothesis H_0. Z is a signed analog of the frequentist "n-sigma".

Fully Bayesian approach

 
Figure Caption
Changed:
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Distributions of the mass of the lightest sbottom. Each entry corresponds to a particular pMSSM point. The black histogram represents all the pMSSM points considered in the analysis, the red (blue) displays the points (not) excluded at 95% CL.

Distributions of the mass of the gluino. Each entry corresponds to a particular pMSSM point. The black histogram represents all the pMSSM points considered in the analysis, the red (blue) displays the points (not) excluded at 95% CL.
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Marginalized 1D probability distributions for ~g mass. The filled blue histogram shows the prior density. The line histograms show posterior densities after including the HT + MET + b-jets analysis. The solid curve shows the posterior density obtained from likelihoods calculated using the central values of estimated signal counts s, whereas the dashed and dotted lines show the posterior densities obtained from likelihoods calculated using s-0.5s and s+0.5s respectively.
   
Marginalized 1D probability distributions for ~b1 mass. The filled blue histogram shows the prior density. The line histograms show posterior densities after including the HT + MET + b-jets analysis. The solid curve shows the posterior density obtained from likelihoods calculated using the central values of estimated signal counts s, whereas the dashed and dotted lines show the posterior densities obtained from likelihoods calculated using s-0.5s and s+0.5s respectively.
   
Marginalized 1D probability distributions for the mass of the lightest colored sparticle. The filled blue histogram shows the prior density. The line histograms show posterior densities after including the HT + MET + b-jets analysis. The solid curve shows the posterior density obtained from likelihoods calculated using the central values of estimated signal counts s, whereas the dashed and dotted lines show the posterior densities obtained from likelihoods calculated using s-0.5s and s+0.5s respectively.
   
Marginalized 1D probability distributions for sparticle production cross section. The filled blue histogram shows the prior density. The line histograms show posterior densities after including the HT + MET + b-jets analysis. The solid curve shows the posterior density obtained from likelihoods calculated using the central values of estimated signal counts s, whereas the dashed and dotted lines show the posterior densities obtained from likelihoods calculated using s-0.5s and s+0.5s respectively.
   
Marginalized prior probability distribution for ~g mass versus ~χ10 mass. The grey and black contours enclose the 68% and 95% Bayesian credible regions respectively.
   
Marginalized posterior probability distribution for ~g mass versus ~χ10 mass after including the HT + MET + b-jets analysis. The grey and black contours enclose the 68% and 95% Bayesian credible regions respectively.
   
Marginalized prior probability distribution for ~b1 mass versus ~χ10 mass. The grey and black contours enclose the 68% and 95% Bayesian credible regions respectively.
   
Marginalized posterior probability distribution for ~b1 mass versus ~χ10 mass after including the HT + MET + b-jets analysis. The grey and black contours enclose the 68% and 95% Bayesian credible regions respectively.
   
 
Changed:
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Distributions of the mass of the lightest colored sparticle. Each entry corresponds to a particular pMSSM point. The black histogram represents all the pMSSM points considered in the analysis, the red (blue) displays the points (not) excluded at 95% CL.
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Excluded vs not-excluded

 
Added:
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Figure Caption
Distributions of ~g mass. The filled blue histogram shows the distribution of pMSSM points samped from the prior density. The red (black) line histograms shows the distribution of pMSSM points not excluded (excluded) by the HT + MET + b-jets analysis. Solid curves show the posterior densities obtained from likelihoods calculated using the central values of estimated signal counts $s$, whereas the dashed and dotted lines show the posterior densities obtained from likelihoods calculated using s-0.5s and s+0.5s respectively.
   
Distributions of ~b1 mass. The filled blue histogram shows the distribution of pMSSM points samped from the prior density. The red (black) line histograms shows the distribution of pMSSM points not excluded (excluded) by the HT + MET + b-jets analysis. Solid curves show the posterior densities obtained from likelihoods calculated using the central values of estimated signal counts $s$, whereas the dashed and dotted lines show the posterior densities obtained from likelihoods calculated using s-0.5s and s+0.5s respectively.
   
Distributions of the mass of the lightest colored sparticle. The filled blue histogram shows the distribution of pMSSM points samped from the prior density. The red (black) line histograms shows the distribution of pMSSM points not excluded (excluded) by the HT + MET + b-jets analysis. Solid curves show the posterior densities obtained from likelihoods calculated using the central values of estimated signal counts $s$, whereas the dashed and dotted lines show the posterior densities obtained from likelihoods calculated using s-0.5s and s+0.5s respectively.
   
Distributions of the sparticle cross section. The filled blue histogram shows the posterior densities after preCMS measurements. The filled blue histogram shows the distribution of pMSSM points samped from the prior density. The red (black) line histograms shows the distribution of pMSSM points not excluded (excluded) by the HT + MET + b-jets analysis. Solid curves show the posterior densities obtained from likelihoods calculated using the central values of estimated signal counts $s$, whereas the dashed and dotted lines show the posterior densities obtained from likelihoods calculated using s-0.5s and s+0.5s respectively.
   
Distribution of ~g mass versus ~χ10 mass for the sampled pMSSM points excluded by the HT + MET + b-jets analysis. The grey and black contours enclose the 68% and 95% of the excluded points.
   
Distribution of ~g mass versus ~χ10 mass for the sampled pMSSM points non excluded by the HT + MET + b-jets analysis. The grey and black contours enclose 68% and 95% of the non-excluded points.
   
Distribution of ~b1 mass versus ~χ10 mass for the sampled pMSSM points excluded by the HT + MET + b-jets analysis. The grey and black contours enclose the 68% and 95% of the excluded points.
   
Distribution of ~b1 mass versus ~χ10 mass for the sampled pMSSM points not excluded by the HT + MET + b-jets analysis. The grey and black contours enclose the 68% and 95% of the non-excluded points.
   
 
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Simplified model topology "T1bbbb".
Simplified model topology "T1tttt".
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pMSSM interpretations

For details on the definition and structure of the pMSSM model, and how the points to be tested by the analyses are generated, see the 7 TeV CMS pMSSM analysis documented on this twiki. The 8 TeV scan used here was generated using the same approach.

For each pMSSM point, we calculate the maximum likelihood value of the fit, fixing the SUSY signal yield to the expectations given by the selection efficiency and predicted cross-section. This value is compared to the maximum likelihood value of the background only hypothesis. The pMSSM points having a negative log-likelihood value which exceed 1.35 units the log-likelihood of the background only hypothesis are excluded at 95% CL (one sided).

The analysis has sensitivity to a large fraction of the model points with accessible masses for the gluino. In addition to the simplified topologies shown explicitly in the main results, gluino decays are flavor blind and often have b-quarks in their decay chains. In addition, many SUSY cascades contain Z or higgs bosons that often lead to b-enriched final states.

Figure Caption
Distributions of the mass of the lightest sbottom. Each entry corresponds to a particular pMSSM point. The black histogram represents all the pMSSM points considered in the analysis, the red (blue) displays the points (not) excluded at 95% CL.

Distributions of the mass of the gluino. Each entry corresponds to a particular pMSSM point. The black histogram represents all the pMSSM points considered in the analysis, the red (blue) displays the points (not) excluded at 95% CL.

Distributions of the mass of the lightest colored sparticle. Each entry corresponds to a particular pMSSM point. The black histogram represents all the pMSSM points considered in the analysis, the red (blue) displays the points (not) excluded at 95% CL.

 
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Table1.png Table 1. Observed numbers of events, SM background estimates from the fit, and SM expectations from Monte Carlo simulation, for the signal (ZL) regions with MET > 350 GeV and Nb-jet = 2. The labels HT2, HT3, and HT4 refer to the bins of HT indicated in the first figure on this twiki, while HT2-4 is the sum over the three bins. The bottom row presents the SM background estimates from the sideband fit described in the text. The uncertainties listed for the fit results include the statistical and systematic components, while those shown for the simulation are statistical only. For the fits, the SUSY signal strength is fixed to zero.
Table2.png Table 2. Observed numbers of events, SM background estimates from the fit, and SM expectations from Monte Carlo simulation, for the signal (ZL) regions with MET >150 GeV and Nb-jet >= 3. The labels HT1, HT2, MET2, etc., refer to the bins of HT and MET indicated in the first figure on this twiki, while HT1-4 (MET2-4) is the sum over the four HT (three MET) bins. The HT1-MET4 bin is excluded from the analysis, as explained in the text. The bottom section presents the SM background estimates from the sideband fit described in the text. The uncertainties listed for the fit results include the statistical and systematic components, while those shown for the simulation are statistical only. For the fits, the SUSY signal strength is fixed to zero.
fitresult-fullfit-hsbins-1sig-19fb_components.png Figure 6. Observed numbers of events (points with error bars) for the 14 bins with highest signal sensitivity in the analysis, in comparison with the standard model background predictions (with total uncertainties shown by the hatched bands) found in the fit with SUSY signal strength fixed to zero. The labels HT1, HT2, MET2, etc., refer to the bins of HT and MET indicated in the first figure on this twiki.
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T1bbbb_exclusions_corrected.png Figure 7 (left). The 95 % CL upper limits on the T1bbbb new-physics scenario cross sections (pb) derived using the CLs method. The solid (black) contours show the observed exclusions assuming the NLO+NLL cross sections, along with the +/- 1 standard deviation theory uncertainties. The dashed (red) contours present the corresponding expected results, along with the +/- 1 standard deviation experimental uncertainties. The root macro that can be used to reproduce the plot is T1bbbb_exclusion_corrected.C.
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T1bbbb_exclusions_corrected.png Figure 7 (left). The 95 % CL upper limits on the T1bbbb new-physics scenario cross sections (pb) derived using the CLs method. The solid (black) contours show the observed exclusions assuming the NLO+NLL cross sections, along with the +/- 1 standard deviation theory uncertainties. The dashed (red) contours present the corresponding expected results, along with the +/- 1 standard deviation experimental uncertainties. The root macro that can be used to reproduce the plot is T1bbbb_exclusions_corrected.C.
 
T1tttt_exclusions_corrected.png Figure 7 (right). The 95 % CL upper limits on the T1tttt new-physics scenario cross sections (pb) derived using the CLs method. The solid (black) contours show the observed exclusions assuming the NLO+NLL cross sections, along with the +/- 1 standard deviation theory uncertainties. The dashed (red) contours present the corresponding expected results, along with the +/- 1 standard deviation experimental uncertainties. The root macro that can be used to reproduce the plot is T1tttt_exclusion_corrected.C.

Comparisons of data and simulation

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Revision 22013-05-21 - EvaHalkiadakis

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Revision 12013-05-21 - EvaHalkiadakis

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Search for gluino-mediated bottom- and top-squark production in pp collisions at 8 TeV

Publication

The manuscript has been submitted to Physics Letters B as arXiv:1305.2390 for publication.

Abstract

A search for supersymmetry is presented based on events with large missing transverse energy, no isolated electron or muon, and at least three jets, with one or more identified as a bottom-quark jet. A simultaneous examination is performed of the numbers of events in exclusive bins of the scalar sum of jet transverse momentum values, missing transverse energy, and bottom-quark jet multiplicity. The sample, corresponding to an integrated luminosity of 19.4 $fb^{-1}$, consists of proton-proton collision data recorded at a center-of-mass energy of 8 TeV with the CMS detector at the LHC in 2012. The observed numbers of events are found to be consistent with the standard model expectation, which is evaluated with control samples in data. The results are interpreted in the context of two simplified supersymmetric scenarios in which gluino pair production is followed by the decay of each gluino to an undetected lightest supersymmetric particle and either a bottom or top quark-antiquark pair, characteristic of gluino mediated bottom- or top-squark production. Using the production cross section calculated to next-to-leading-order plus next-to-leading-logarithm accuracy, and in the limit of a massless lightest supersymmetric particle, we exclude gluinos with masses below 1170 GeV and 1020 GeV for the two scenarios, respectively.

Tables and Plots from the paper

  • Click on plot to get .pdf
  • "right click->save image as" to get .png

Likelihood fit schematic diagram

Figure Caption
Figure 2. Schematic diagram illustrating the 176 mutually exclusive bins in the analysis. The MET and HT distributions are divided into four bins each; the table gives the bin definitions. The designations HT$i$ and MET$i$ ($i=1-4$) are used to label the individual HT and MET bins. The Nb-jet distributions of the signal sample (ZL), top-quark and W+jets control sample (SL), and QCD multijet control sample (LDP), contain three bins each, corresponding to exactly one, exactly two, and three or more identified b jets.

Results and interpretation

Table1.png Table 1. Observed numbers of events, SM background estimates from the fit, and SM expectations from Monte Carlo simulation, for the signal (ZL) regions with MET > 350 GeV and Nb-jet = 2. The labels HT2, HT3, and HT4 refer to the bins of HT indicated in the first figure on this twiki, while HT2-4 is the sum over the three bins. The bottom row presents the SM background estimates from the sideband fit described in the text. The uncertainties listed for the fit results include the statistical and systematic components, while those shown for the simulation are statistical only. For the fits, the SUSY signal strength is fixed to zero.
Table2.png Table 2. Observed numbers of events, SM background estimates from the fit, and SM expectations from Monte Carlo simulation, for the signal (ZL) regions with MET >150 GeV and Nb-jet >= 3. The labels HT1, HT2, MET2, etc., refer to the bins of HT and MET indicated in the first figure on this twiki, while HT1-4 (MET2-4) is the sum over the four HT (three MET) bins. The HT1-MET4 bin is excluded from the analysis, as explained in the text. The bottom section presents the SM background estimates from the sideband fit described in the text. The uncertainties listed for the fit results include the statistical and systematic components, while those shown for the simulation are statistical only. For the fits, the SUSY signal strength is fixed to zero.
fitresult-fullfit-hsbins-1sig-19fb_components.png Figure 6. Observed numbers of events (points with error bars) for the 14 bins with highest signal sensitivity in the analysis, in comparison with the standard model background predictions (with total uncertainties shown by the hatched bands) found in the fit with SUSY signal strength fixed to zero. The labels HT1, HT2, MET2, etc., refer to the bins of HT and MET indicated in the first figure on this twiki.
T1bbbb_exclusions_corrected.png Figure 7 (left). The 95 % CL upper limits on the T1bbbb new-physics scenario cross sections (pb) derived using the CLs method. The solid (black) contours show the observed exclusions assuming the NLO+NLL cross sections, along with the +/- 1 standard deviation theory uncertainties. The dashed (red) contours present the corresponding expected results, along with the +/- 1 standard deviation experimental uncertainties. The root macro that can be used to reproduce the plot is T1bbbb_exclusion_corrected.C.
T1tttt_exclusions_corrected.png Figure 7 (right). The 95 % CL upper limits on the T1tttt new-physics scenario cross sections (pb) derived using the CLs method. The solid (black) contours show the observed exclusions assuming the NLO+NLL cross sections, along with the +/- 1 standard deviation theory uncertainties. The dashed (red) contours present the corresponding expected results, along with the +/- 1 standard deviation experimental uncertainties. The root macro that can be used to reproduce the plot is T1tttt_exclusion_corrected.C.

Comparisons of data and simulation

h_nb_zl_all_btw_logy.png Figure 3 (top left). Data and Monte Carlo distributions of the number Nb-jet of b-tagged jets for the signal (ZL) sample. The lower panes show the ratio of the measured to the simulated events. The simulated results are intended for guidance and are not used in the analysis. Results for the T1bbbb scenario with (m$\tilde{g}$, m$\tilde{\chi}^0_1$)=(600 GeV, 500 GeV) and (1225 GeV, 150 GeV) are shown as unstacked distributions. The uncertainties are statistical only. The normalization of the simulated curves is based on the absolute cross sections, as described in the text.
h_nb_sl_all_btw_logy.png Figure 3 (top middle). Data and Monte Carlo distributions of the number Nb-jet of b-tagged jets for the top-quark and W+jets (SL) control sample. The lower panes show the ratio of the measured to the simulated events. The simulated results are intended for guidance and are not used in the analysis. Results for the T1bbbb scenario with (m$\tilde{g}$, m$\tilde{\chi}^0_1$)=(600 GeV, 500 GeV) and (1225 GeV, 150 GeV) are shown as unstacked distributions. The uncertainties are statistical only. The normalization of the simulated curves is based on the absolute cross sections, as described in the text.
h_nb_ldp_all_btw_logy.png Figure 3 (top right). Data and Monte Carlo distributions of the number Nb-jet of b-tagged jets for the QCD multijet (LDP) control sample. The lower panes show the ratio of the measured to the simulated events. The simulated results are intended for guidance and are not used in the analysis. Results for the T1bbbb scenario with (m$\tilde{g}$, m$\tilde{\chi}^0_1$)=(600 GeV, 500 GeV) and (1225 GeV, 150 GeV) are shown as unstacked distributions. The uncertainties are statistical only. The normalization of the simulated curves is based on the absolute cross sections, as described in the text.
h_met_zl_nb3_btw_logy.png Figure 3 (center left). Data and Monte Carlo distributions of MET for the signal (ZL) sample for events with Nb-jet >= 3. The lower panes show the ratio of the measured to the simulated events. The dashed vertical lines indicate the divisions between the four bins of MET. The simulated results are intended for guidance and are not used in the analysis. Results for the T1bbbb scenario with (m$\tilde{g}$, m$\tilde{\chi}^0_1$)=(600 GeV, 500 GeV) and (1225 GeV, 150 GeV) are shown as unstacked distributions. The uncertainties are statistical only. The normalization of the simulated curves is based on the absolute cross sections, as described in the text.
h_met_sl_nb3_btw_logy.png Figure 3 (center center). Data and Monte Carlo distributions of MET for the top-quark and W+jets (SL) control sample for events with Nb-jet >= 3. The lower panes show the ratio of the measured to the simulated events. The dashed vertical lines indicate the divisions between the four bins of MET. The simulated results are intended for guidance and are not used in the analysis. Results for the T1bbbb scenario with (m$\tilde{g}$, m$\tilde{\chi}^0_1$)=(600 GeV, 500 GeV) and (1225 GeV, 150 GeV) are shown as unstacked distributions. The uncertainties are statistical only. The normalization of the simulated curves is based on the absolute cross sections, as described in the text.
h_met_ldp_nb3_btw_logy.png Figure 3 (center right). Data and Monte Carlo distributions of MET for the QCD multijet (LDP) control sample for events with Nb-jet >= 3. The lower panes show the ratio of the measured to the simulated events. The dashed vertical lines indicate the divisions between the four bins of MET. The simulated results are intended for guidance and are not used in the analysis. Results for the T1bbbb scenario with (m$\tilde{g}$, m$\tilde{\chi}^0_1$)=(600 GeV, 500 GeV) and (1225 GeV, 150 GeV) are shown as unstacked distributions. The uncertainties are statistical only. The normalization of the simulated curves is based on the absolute cross sections, as described in the text.
h_ht_zl_nb3_btw_logy.png Figure 3 (bottom left). Data and Monte Carlo distributions of HT for the signal (ZL) sample for events with Nb-jet >= 3. The lower panes show the ratio of the measured to the simulated events. The dashed vertical lines indicate the divisions between the four bins of HT. The simulated results are intended for guidance and are not used in the analysis. Results for the T1bbbb scenario with (m$\tilde{g}$, m$\tilde{\chi}^0_1$)=(600 GeV, 500 GeV) and (1225 GeV, 150 GeV) are shown as unstacked distributions. The uncertainties are statistical only. The normalization of the simulated curves is based on the absolute cross sections, as described in the text.
h_ht_sl_nb3_btw_logy.png Figure 3 (bottom center). Data and Monte Carlo distributions of HT for the top-quark and W+jets (SL) control sample for events with Nb-jet >= 3. The lower panes show the ratio of the measured to the simulated events. The dashed vertical lines indicate the divisions between the four bins of HT. The simulated results are intended for guidance and are not used in the analysis. Results for the T1bbbb scenario with (m$\tilde{g}$, m$\tilde{\chi}^0_1$)=(600 GeV, 500 GeV) and (1225 GeV, 150 GeV) are shown as unstacked distributions. The uncertainties are statistical only. The normalization of the simulated curves is based on the absolute cross sections, as described in the text.
h_ht_ldp_nb3_btw_logy.png Figure 3 (bottom right). Data and Monte Carlo distributions of HT for the QCD multijet (LDP) control sample for events with Nb-jet >= 3. The lower panes show the ratio of the measured to the simulated events. The dashed vertical lines indicate the divisions between the four bins of HT. The simulated results are intended for guidance and are not used in the analysis. Results for the T1bbbb scenario with (m$\tilde{g}$, m$\tilde{\chi}^0_1$)=(600 GeV, 500 GeV) and (1225 GeV, 150 GeV) are shown as unstacked distributions. The uncertainties are statistical only. The normalization of the simulated curves is based on the absolute cross sections, as described in the text.

Estimate of top+W background

gi-plots-met4-ht4-v15-mcclosure-ttwj3.png Figure 4. [left] Ratio of the number of events in the zero-lepton (ZL) sample to that in the single-lepton (SL) sample for simulated top-quark and W+jets events in the 16 HT-MET bins with Nb-jet = 1, divided by the average ratio value over the 16 bins. The leftmost group of four consecutive points corresponds to MET bin 1 (MET1) of the table in the first figure on this twiki, the next-leftmost group to MET bin 2 (MET2), etc. The four points within each group correspond to the four HT bins in the table, increasing in HT value from left to right (HT1 to HT4). The inner (outer) error bars show the statistical (combined statistical and systematic) uncertainties. [center and right] The corresponding results for Nb-jet = 2 and Nb-jet >= 3.

Estimate of QCD background

mcclosure4-qcd-averatio.png Figure 5. Ratio of the number of events in the zero-lepton (ZL) sample to that in the low-$\Delta \hat{\phi}_{min}$ (LDP) sample for simulated QCD multijet events. The definitions of the bins are the same as in the above figure. Various QCD multijet samples, with different choices for the hardness scale ($\hat{p}_T$) of the interaction, are combined. The points show the averages over those samples. The inner error bars indicate the statistical uncertainties. The outer error bars indicate the statistical uncertainties added in quadrature with the root-mean-squared values over the different $\hat{p}_T$ samples. The histogram shows the results of the fitted parameterization described in the text.
mcclosure4-qcd-scalefactor-model4.png The corresponding ratio divided by the parameterization from the top row. The inner (black) and outer (blue) error bars indicate the statistical and combined statistical-and-systematic uncertainties, respectively.

Additional material

  • Click on plot to get .pdf
  • "right click->save image as" to get .png

Results of sideband fit

In addition to the full fit, it is interesting to perform the likelihood fit with the Poisson PDF terms for the 14 bins with the highest signal sensitivity removed, in order to ascertain the data-based SM background prediction when the data in these bins do not affect the result. We call such a fit the ``sideband'' fit.

Table3.png SM background estimates from the sideband fit for events with MET > 350 GeV and number of b jets = 2. The labels HT2, HT3, and HT4 refer to the bins of HT indicated in the schematic above (first figure on this twiki), while HT2-4 is the sum over the three bins

Table4.png SM background estimates from the sideband fit for events with MET > 150 GeV and number of b jets ≥ 3. The labels HT1, HT2, MET2, etc., refer to the bins of HT and MET indicated in the schematic above (first figure on this twiki). HT1-4 (MET2-4) refers to the sum over the four HT (three MET) bins. The HT1-MET4 bin is excluded from the analysis. Please see Section 5.6 of our PAS for more details

fitresult-unbiased-hsbins-2sig-19fb.png Observed number of events (points with error bars) for the 14 bins with highest signal sensitivity in the analysis. The dark- and light-shaded bands indicate the 1 and 2 standard deviation intervals, respectively, for the SM background estimates from the sideband fit.

Efficiencies

T1bbbb_efficiency.png T1bbbb selection efficiencies. In the root file efficiency_T1bbbb_multi.root we provide not only the histogram for the total 0-lepton efficiency ("heff_tot"), but also the histograms of the efficiency in every 0-lepton bin of the analysis ("heff_METx_HTy_nBz" - the boundaries of the (MET,HT,nB) bins are specified in the title of the root histogram). The plotted points reflect the density of the scan used to determine the efficiencies.
T1tttt_efficiency.png T1tttt selection efficiencies. In the root file efficiency_T1tttt_multi.root we provide not only the histogram for the total 0-lepton efficiency ("heff_tot"), but also the histograms of the efficiency in every 0-lepton bin of the analysis ("heff_METx_HTy_nBz" - the boundaries of the (MET,HT,nB) bins are specified in the title of the root histogram). The plotted points reflect the density of the scan used to determine the efficiencies.

Event Displays

Event displays are included for a couple events, each presented in a rho-phi and 3D view, and with black and white background.

615309469_rhophi_black.png Event 61509469, rho-phi view, black background

615309469_rhophi_newScheme.png Event 61509469, rho-phi view, black background, alternative color scheme

615309469_rhophi_white.png Event 61509469, rho-phi view, white background

615309469_3D_black.png Event 61509469, 3D view, black background

615309469_3D_newScheme.png Event 61509469, 3D view, black background, alternative color scheme

615309469_3D_white.png Event 61509469, 3D view, white background

94548608_rhophi_black.png Event 94548608, rho-phi view, black background

94548608_rhophi_newScheme.png Event 94548608, rho-phi view, black background, alternative color scheme

94548608_rhophi_white.png Event 94548608, rho-phi view, white background

94548608_3D_black.png Event 94548608, 3D view, black background

94548608_3D_newScheme.png Event 94548608, 3D view, black background, alternative color scheme

94548608_3D_white.png Event 94548608, 3D view, white background

Simplified models

The concept of "simplified models" is described here and here. The purpose is to link the LHC experiments and the theory communities interested in interpreting LHC data.

Figure Caption
Simplified model topology "T1bbbb".
Simplified model topology "T1tttt".

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