Search for supersymmetry using razor variables in events with b-tagged jets in pp collisions at $\sqrt{s}=8$ TeV

Abstract

An inclusive search for supersymmetry in events with at least one b-tagged jet is performed using proton-proton collision data collected by the CMS experiment in 2012 at a center-of-mass energy of 8 CMS.TeV. The data set size corresponds to an integrated luminosity of 19.3 fb$^{-1}$.The two-dimensional event distribution of the razor variables $\mathrm{R}^2$ and $M_{\mathrm{R}}$ is studied in events with and without leptons. The data are found to be consistent with the expected background, which is modeled with an empirical function. Exclusion limits on supersymmetric particle masses at a 95% confidence level are derived in several simplified supersymmetric scenarios for several choices of the branching fractions. By combining the likelihoods of a search in events without leptons and a search that requires a single lepton (electron or muon), an improved bound on the top-squark mass is obtained. Assuming the lightest supersymmetric particle to be stable, weakly interacting, and to have a mass of 100 CMS.GeV, the branching-fraction-dependent (-independent) production of gluinos is excluded for gluino masses up to 1310 (1175) CMS.GeV. The corresponding limit for top-squark pair production is 730 (645) CMS.GeV.

Link to paper on arXiv and PRD

CMS-SUS-13-004

Phys. Rev. D 91, 052018

Figures and tables from CMS-SUS-13-004

Simplified natural SUSY models Caption
naturalSpectrum.png Figure 1. The simplified natural SUSY spectrum considered in this paper, along with the assumed decay modes.
T1bbbb.pngT1tbbb.pngT1ttbb.pngT1tttb.pngT1tttt.pngT2bw.pngT2tb.pngT2tt.png Figure 2. Diagrams displaying the event topologies of gluino (upper 5 diagrams) and top-squark (lower 3 diagrams) pair production considered in this paper.
Box definitions Caption
boxTable.png Table 1. Kinematic and multiplicity requirements defining the nine razor boxes. Boxes are listed in order of event filling priority.
SidebandL_Mu.pngSidebandL_MultiJet.png Figure 3. Definition of the sideband and the signal-sensitive regions used in the analysis, for (left) the hadronic boxes and (right) the other boxes.
Modeling of the standard model backgrounds Caption
nSigmaLog_MuEle.pngnSigmaLog_MuMu.pngnSigmaLog_EleEle.png Figure 4. Comparison of the expected background and the observed yield in the (a) MuEle, (b) MuMu, and (c) EleEle boxes. A probability density function is derived for the bin-by-bin yield using pseudo-experiments, sampled from the output of the corresponding sideband fit. A two sided p-value is computed comparing the observed yield to the distribution of background yield from pseudo-experiments. The p-value is translated into the corresponding number of standard deviations, quoted in each bin and represented by the bin-filling color. Positive and negative significance correspond to regions where the observed yield is respectively larger and smaller than the predicted one. Gray areas correspond to empty bins with less than one background event expected on average. The dashed lines represent the boundaries between the sideband and the signal regions.
nSigmaLog_EleJet.pngnSigmaLog_EleMultiJet.pngnSigmaLog_MuJet.pngnSigmaLog_MuMultiJet.png Figure 5. Comparison of the expected background and the observed yield in (a) the EleJet, (b) the EleMultiJet, (c) the MuJet, and (d) the MuMultiJet boxes. A detailed explanation is given in the caption of Fig. 4.
nSigmaLog_Jet2b.pngnSigmaLog_MultiJetFITS.png Figure 6. Comparison of the expected background and the observed yield in the $\geq2$ b-tagged jet box (left) and the MultiJet box (right). A detailed explanation is given in the caption of Fig. 4
MR_ElectronHad-Run2012ABCD_Sideband_MuEle.png RSQ_ElectronHad-Run2012ABCD_Sideband_MuEle.png MR_MuHad-Run2012ABCD_Sideband_MuMu.png RSQ_MuHad-Run2012ABCD_Sideband_MuMu.pngMR_ElectronHad-Run2012ABCD_Sideband_EleEle.png RSQ_ElectronHad-Run2012ABCD_Sideband_EleEle.png Figure 7. Projection of the sideband fit result in the (a-b) MuEle, (c-d) MuMu, and (e-f) EleEle boxes on $M_{\mathrm{R}}$ (left) and $\mathrm{R^2}$ (right), respectively. The fit is performed in the sideband regions and extrapolated to the signal-sensitive region. The solid line and the filled band represent the total background prediction and its uncertainty. The points and the band in the bottom panel represent the data-to-prediction ratio and the prediction uncertainty, respectively.
MR_MuHad-Run2012ABCD_Sideband_MuJet.png RSQ_MuHad-Run2012ABCD_Sideband_MuJet.pngMR_MuHad-Run2012ABCD_Sideband_MuMultiJet.png RSQ_MuHad-Run2012ABCD_Sideband_MuMultiJet.png Figure 8. Projection of the sideband fit result in the MuJet box on (a) $M_{\mathrm{R}}$ and (b) $\mathrm{R^2}$, and of the sideband fit result in the MuMultiJet box on (c) $M_{\mathrm{R}}$ and (d) $\mathrm{R^2}$. The fit is performed in the sideband regions and extrapolated to the signal-sensitive region. The solid line and the filled band represent the total background prediction and its uncertainty. The dashed and dot-dashed lines represent the background shape for $1$ b-tag and $\geq2$ b-tag events, respectively. The points and the band in the bottom panel represent the data-to-prediction ratio and the prediction uncertainty, respectively.
MR_ElectronHad-Run2012ABCD_Sideband_EleJet.png RSQ_ElectronHad-Run2012ABCD_Sideband_EleJet.png MR_ElectronHad-Run2012ABCD_Sideband_EleMultiJet.png RSQ_ElectronHad-Run2012ABCD_Sideband_EleMultiJet.png Figure 9. Projection of the sideband fit result in the EleJet box on (a) $M_{\mathrm{R}}$ and (b) $\mathrm{R^2}$, and projection of the sideband fit result in the EleMultiJet box on (c) $M_{\mathrm{R}}$ and (d) $\mathrm{R^2}$. A detailed explanation is given in the caption of Fig. 8
MR_HT-HTMHT-Run2012ABCD_Sideband_Jet2b.png RSQ_HT-HTMHT-Run2012ABCD_Sideband_Jet2b.png MR_HT-HTMHT-Run2012ABCD_Sideband_MultiJet.png RSQ_HT-HTMHT-Run2012ABCD_Sideband_MultiJet.png Figure 10. Projection of the sideband fit result in the $\geq2$ b-tagged jet box on (a) $M_{\mathrm{R}}$ and (b) $\mathrm{R^2}$, and projection of the sideband fit result in the MultiJet box on (c) $M_{\mathrm{R}}$ and (d) $\mathrm{R^2}$. A detailed explanation is given in the caption of Fig. 8.
T1bbbb_1325_50_FF.pngSMbkgd_FF.png Figure 11. Distribution of (a) simulated SM background events and (b) T1bbbb gluino-gluino events in the MultiJet box. Each $\tilde g$ is forced to decay to a $\mathrm{b \bar b}$ pair and a $\tilde\chi_1^0$, assumed to be the stable LSP. The $\tilde g$ and $\tilde\chi_1^0$ masses are fixed to 1325 CMS.GeV and 50 CMS.GeV, respectively.
MR_T1bbbb_0p02_MultiJet.pngRSQ_T1bbbb_0p02_MultiJet.pngnSigmaLog_MultiJet.png Figure 12. Result of the fit to the sideband events of a signal-plus-background MC sample, corresponding to the gluino model whose distribution is shown in Fig. 11. A gluino-gluino production cross section of $0.02$ pb is assumed. The one-dimensional projections on (a) $M_{\mathrm{R}}$ and (b) $\mathrm{R^2}$ are shown, together with (c) the agreement between the observed yield and the prediction from the sideband fit as a function of $\mathrm{R^2}$ and $M_{\mathrm{R}}$. This agreement is evaluated from a two-sided p-value using an ensemble of background-only pseudo-experiments as described in Section 6.
Interpretation Caption
Figure 13. Interpretation of the inclusive search with razor variables in the context of gluino pair production models: (a) T1bbbb, (b) T1tbbb, (c) T1ttbb, (d) T1tttb, and (e) T1tttt. The limit for T1bbbb is derived using only the hadronic boxes, while the limits for the remaining models are derived using all nine boxes. The color coding indicates the observed 95\% CL upper limit on the signal cross section. The dashed and solid lines represent the expected and observed exclusion contours at a 95% CL, respectively. The dashed contours around the expected limit and the solid contours around the observed one represent the one standard deviation theoretical uncertainties in the cross section and the combination of the statistical and experimental systematic uncertainties, respectively.
Figure 14. Gluino mass limit at a 95% CL, obtained for different gluino pair production models with the inclusive razor analysis in the context of the natural SUSY spectrum of Fig. 1
Figure 15. Interpretation of the inclusive search with razor variables in the context of top-squark pair production models: (a) T2bW$^{\ast}$, (b) T2tb, and (c) T2tt. The limit for T2bW$^{\ast}$ is derived using only the hadronic boxes, while the limits for the remaining models are derived using all nine boxes. The meaning of the color coding and the displayed contours is explained in the caption of Fig. 13.
Figure 16. Top-squark mass limit at a 95% CL, obtained for different squark pair production models with the inclusive razor analysis in the context of the natural SUSY spectrum of Fig 1.
Figure 17. Top-squark mass limit at a 95% CL, obtained combining the result of the hadronic razor boxes with the result of Ref. 19 for (a) T2tt and (b) independent of the branching fraction choice. The meaning of the color coding and the displayed contours is explained in the caption of Fig. 13
Additional Material Caption
Observed yields and expected yields plus-or-minus one standard deviation for each bin in the CMS-SUS-13-004 paper. The bin-by-bin yields can also be found in electronic format here. The expected yield histograms have the bin-by-bin systematic and statistical uncertainties saved as the bin-by-bin error.
eff_T1bbbb_Jet2b.pngeff_T1bbbb_MultiJet.png T1bbbb signal model selection efficiencies for the zero-lepton razor boxes used in the search.
eff_T1tbbb_MuEle.pngeff_T1tbbb_MuMu.pngeff_T1tbbb_EleEle.pngeff_T1tbbb_EleJet.pngeff_T1tbbb_EleMultiJet.pngeff_T1tbbb_MuJet.pngeff_T1tbbb_MuMultiJet.pngeff_T1tbbb_Jet2b.pngeff_T1tbbb_MultiJet.png T1tbbb signal model selection efficiencies for the zero-lepton, one-lepton, and two-lepton razor boxes used in the search.
eff_T1ttbb_MuEle.pngeff_T1ttbb_MuMu.pngeff_T1ttbb_EleEle.pngeff_T1ttbb_EleJet.pngeff_T1ttbb_EleMultiJet.pngeff_T1ttbb_MuJet.pngeff_T1ttbb_MuMultiJet.pngeff_T1ttbb_Jet2b.pngeff_T1ttbb_MultiJet.png T1ttbb signal model selection efficiencies for the zero-lepton, one-lepton, and two-lepton razor boxes used in the search.
eff_T1tttb_MuEle.pngeff_T1tttb_MuMu.pngeff_T1tttb_EleEle.pngeff_T1tttb_EleJet.pngeff_T1tttb_EleMultiJet.pngeff_T1tttb_MuJet.pngeff_T1tttb_MuMultiJet.pngeff_T1tttb_Jet2b.pngeff_T1tttb_MultiJet.png T1tttb signal model selection efficiencies for the zero-lepton, one-lepton, and two-lepton razor boxes used in the search.
eff_T1tttt_MuEle.pngeff_T1tttt_MuMu.pngeff_T1tttt_EleEle.pngeff_T1tttt_EleJet.pngeff_T1tttt_EleMultiJet.pngeff_T1tttt_MuJet.pngeff_T1tttt_MuMultiJet.pngeff_T1tttt_Jet2b.pngeff_T1tttt_MultiJet.png T1tttt signal model selection efficiencies for the zero-lepton, one-lepton, and two-lepton razor boxes used in the search.
eff_T2bw_Jet2b.pngeff_T2bw_MultiJet.png T2bW$^{\ast}$ signal model selection efficiencies for the zero-lepton razor boxes used in the search.
eff_T2tb_MuEle.pngeff_T2tb_MuMu.pngeff_T2tb_EleEle.pngeff_T2tb_EleJet.pngeff_T2tb_EleMultiJet.pngeff_T2tb_MuJet.pngeff_T2tb_MuMultiJet.pngeff_T2tb_Jet2b.pngeff_T2tb_MultiJet.png T2tb signal model selection efficiencies for the zero-lepton, one-lepton, and two-lepton razor boxes used in the search.
eff_T2tt_MuEle.pngeff_T2tt_MuMu.pngeff_T2tt_EleEle.pngeff_T2tt_EleJet.pngeff_T2tt_EleMultiJet.pngeff_T2tt_MuJet.pngeff_T2tt_MuMultiJet.pngeff_T2tt_Jet2b.pngeff_T2tt_MultiJet.png T2tt signal model selection efficiencies for the zero-lepton, one-lepton, and two-lepton razor boxes used in the search.
razor_8TeV_sms_results.png The observed 95% CL upper limit on the signal cross section in electronic ROOT format for all signal models for both razor and combined searches.
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PNGpng eff_T1ttbb_EleEle.png r1 manage 154.6 K 2015-06-03 - 00:39 JavierDuarte  
PDFpdf eff_T1ttbb_EleJet.pdf r1 manage 21.6 K 2015-06-03 - 00:39 JavierDuarte  
PNGpng eff_T1ttbb_EleJet.png r1 manage 151.5 K 2015-06-03 - 00:39 JavierDuarte  
PDFpdf eff_T1ttbb_EleMultiJet.pdf r1 manage 21.6 K 2015-06-03 - 00:39 JavierDuarte  
PNGpng eff_T1ttbb_EleMultiJet.png r1 manage 153.2 K 2015-06-03 - 00:39 JavierDuarte  
PDFpdf eff_T1ttbb_Jet2b.pdf r1 manage 21.5 K 2015-06-03 - 00:39 JavierDuarte  
PNGpng eff_T1ttbb_Jet2b.png r1 manage 153.8 K 2015-06-03 - 00:39 JavierDuarte  
PDFpdf eff_T1ttbb_MuEle.pdf r1 manage 21.7 K 2015-06-03 - 00:39 JavierDuarte  
PNGpng eff_T1ttbb_MuEle.png r1 manage 158.4 K 2015-06-03 - 00:39 JavierDuarte  
PDFpdf eff_T1ttbb_MuJet.pdf r1 manage 21.7 K 2015-06-03 - 00:39 JavierDuarte  
PNGpng eff_T1ttbb_MuJet.png r1 manage 158.7 K 2015-06-03 - 00:39 JavierDuarte  
PDFpdf eff_T1ttbb_MuMu.pdf r1 manage 21.7 K 2015-06-03 - 00:39 JavierDuarte  
PNGpng eff_T1ttbb_MuMu.png r1 manage 155.4 K 2015-06-03 - 00:39 JavierDuarte  
PDFpdf eff_T1ttbb_MuMultiJet.pdf r1 manage 21.7 K 2015-06-03 - 00:40 JavierDuarte  
PNGpng eff_T1ttbb_MuMultiJet.png r1 manage 155.5 K 2015-06-03 - 00:40 JavierDuarte  
PDFpdf eff_T1ttbb_MultiJet.pdf r1 manage 21.6 K 2015-06-03 - 00:39 JavierDuarte  
PNGpng eff_T1ttbb_MultiJet.png r1 manage 154.4 K 2015-06-03 - 00:39 JavierDuarte  
PDFpdf eff_T1tttb_EleEle.pdf r1 manage 21.6 K 2015-06-03 - 01:06 JavierDuarte  
PNGpng eff_T1tttb_EleEle.png r1 manage 171.2 K 2015-06-03 - 01:10 JavierDuarte  
PDFpdf eff_T1tttb_EleJet.pdf r1 manage 21.6 K 2015-06-03 - 01:06 JavierDuarte  
PNGpng eff_T1tttb_EleJet.png r1 manage 167.5 K 2015-06-03 - 01:10 JavierDuarte  
PDFpdf eff_T1tttb_EleMultiJet.pdf r1 manage 21.7 K 2015-06-03 - 01:06 JavierDuarte  
PNGpng eff_T1tttb_EleMultiJet.png r1 manage 169.5 K 2015-06-03 - 01:10 JavierDuarte  
PDFpdf eff_T1tttb_Jet2b.pdf r1 manage 21.6 K 2015-06-03 - 01:06 JavierDuarte  
PNGpng eff_T1tttb_Jet2b.png r1 manage 167.1 K 2015-06-03 - 01:10 JavierDuarte  
PDFpdf eff_T1tttb_MuEle.pdf r1 manage 21.8 K 2015-06-03 - 01:06 JavierDuarte  
PNGpng eff_T1tttb_MuEle.png r1 manage 173.4 K 2015-06-03 - 01:10 JavierDuarte  
PDFpdf eff_T1tttb_MuJet.pdf r1 manage 21.6 K 2015-06-03 - 01:06 JavierDuarte  
PNGpng eff_T1tttb_MuJet.png r1 manage 168.6 K 2015-06-03 - 01:10 JavierDuarte  
PDFpdf eff_T1tttb_MuMu.pdf r1 manage 21.7 K 2015-06-03 - 01:06 JavierDuarte  
PNGpng eff_T1tttb_MuMu.png r1 manage 171.7 K 2015-06-03 - 01:10 JavierDuarte  
PDFpdf eff_T1tttb_MuMultiJet.pdf r1 manage 21.8 K 2015-06-03 - 01:06 JavierDuarte  
PNGpng eff_T1tttb_MuMultiJet.png r1 manage 168.3 K 2015-06-03 - 01:10 JavierDuarte  
PDFpdf eff_T1tttb_MultiJet.pdf r1 manage 21.8 K 2015-06-03 - 01:06 JavierDuarte  
PNGpng eff_T1tttb_MultiJet.png r1 manage 167.2 K 2015-06-03 - 01:10 JavierDuarte  
PDFpdf eff_T1tttt_EleEle.pdf r1 manage 26.3 K 2015-06-03 - 01:06 JavierDuarte  
PNGpng eff_T1tttt_EleEle.png r1 manage 154.3 K 2015-06-03 - 00:40 JavierDuarte  
PDFpdf eff_T1tttt_EleJet.pdf r1 manage 26.0 K 2015-06-03 - 00:40 JavierDuarte  
PNGpng eff_T1tttt_EleJet.png r1 manage 160.5 K 2015-06-03 - 00:40 JavierDuarte  
PDFpdf eff_T1tttt_EleMultiJet.pdf r1 manage 26.3 K 2015-06-03 - 00:40 JavierDuarte  
PNGpng eff_T1tttt_EleMultiJet.png r1 manage 156.1 K 2015-06-03 - 00:40 JavierDuarte  
PDFpdf eff_T1tttt_Jet2b.pdf r1 manage 25.6 K 2015-06-03 - 00:40 JavierDuarte  
PNGpng eff_T1tttt_Jet2b.png r1 manage 166.0 K 2015-06-03 - 00:40 JavierDuarte  
PDFpdf eff_T1tttt_MuEle.pdf r1 manage 25.8 K 2015-06-03 - 00:41 JavierDuarte  
PNGpng eff_T1tttt_MuEle.png r1 manage 159.8 K 2015-06-03 - 00:41 JavierDuarte  
PDFpdf eff_T1tttt_MuJet.pdf r1 manage 25.8 K 2015-06-03 - 00:41 JavierDuarte  
PNGpng eff_T1tttt_MuJet.png r1 manage 160.4 K 2015-06-03 - 00:41 JavierDuarte  
PDFpdf eff_T1tttt_MuMu.pdf r1 manage 26.2 K 2015-06-03 - 00:41 JavierDuarte  
PNGpng eff_T1tttt_MuMu.png r1 manage 151.0 K 2015-06-03 - 00:41 JavierDuarte  
PDFpdf eff_T1tttt_MuMultiJet.pdf r1 manage 26.0 K 2015-06-03 - 00:41 JavierDuarte  
PNGpng eff_T1tttt_MuMultiJet.png r1 manage 151.0 K 2015-06-03 - 00:41 JavierDuarte  
PDFpdf eff_T1tttt_MultiJet.pdf r1 manage 26.4 K 2015-06-03 - 00:41 JavierDuarte  
PNGpng eff_T1tttt_MultiJet.png r1 manage 164.7 K 2015-06-03 - 00:41 JavierDuarte  
PDFpdf eff_T2bw_EleEle.pdf r1 manage 21.4 K 2015-06-03 - 00:41 JavierDuarte  
PNGpng eff_T2bw_EleEle.png r1 manage 153.4 K 2015-06-03 - 00:41 JavierDuarte  
PDFpdf eff_T2bw_EleJet.pdf r1 manage 21.9 K 2015-06-03 - 00:41 JavierDuarte  
PNGpng eff_T2bw_EleJet.png r1 manage 153.3 K 2015-06-03 - 00:41 JavierDuarte  
PDFpdf eff_T2bw_EleMultiJet.pdf r1 manage 21.5 K 2015-06-03 - 00:41 JavierDuarte  
PNGpng eff_T2bw_EleMultiJet.png r1 manage 158.1 K 2015-06-03 - 00:41 JavierDuarte  
PDFpdf eff_T2bw_Jet2b.pdf r1 manage 22.9 K 2015-06-03 - 00:41 JavierDuarte  
PNGpng eff_T2bw_Jet2b.png r1 manage 155.6 K 2015-06-03 - 00:41 JavierDuarte  
PDFpdf eff_T2bw_MuEle.pdf r1 manage 21.3 K 2015-06-03 - 00:41 JavierDuarte  
PNGpng eff_T2bw_MuEle.png r1 manage 163.8 K 2015-06-03 - 00:41 JavierDuarte  
PDFpdf eff_T2bw_MuJet.pdf r1 manage 21.8 K 2015-06-03 - 00:41 JavierDuarte  
PNGpng eff_T2bw_MuJet.png r1 manage 161.7 K 2015-06-03 - 00:41 JavierDuarte  
PDFpdf eff_T2bw_MuMu.pdf r1 manage 21.4 K 2015-06-03 - 00:41 JavierDuarte  
PNGpng eff_T2bw_MuMu.png r1 manage 150.8 K 2015-06-03 - 00:41 JavierDuarte  
PDFpdf eff_T2bw_MuMultiJet.pdf r1 manage 21.5 K 2015-06-03 - 00:41 JavierDuarte  
PNGpng eff_T2bw_MuMultiJet.png r1 manage 155.2 K 2015-06-03 - 00:41 JavierDuarte  
PDFpdf eff_T2bw_MultiJet.pdf r1 manage 22.7 K 2015-06-03 - 00:41 JavierDuarte  
PNGpng eff_T2bw_MultiJet.png r1 manage 160.6 K 2015-06-03 - 00:41 JavierDuarte  
PDFpdf eff_T2tb_EleEle.pdf r1 manage 22.8 K 2015-06-03 - 00:41 JavierDuarte  
PNGpng eff_T2tb_EleEle.png r1 manage 181.9 K 2015-06-03 - 00:41 JavierDuarte  
PDFpdf eff_T2tb_EleJet.pdf r1 manage 23.2 K 2015-06-03 - 00:41 JavierDuarte  
PNGpng eff_T2tb_EleJet.png r1 manage 175.6 K 2015-06-03 - 00:41 JavierDuarte  
PDFpdf eff_T2tb_EleMultiJet.pdf r1 manage 22.8 K 2015-06-03 - 00:41 JavierDuarte  
PNGpng eff_T2tb_EleMultiJet.png r1 manage 172.6 K 2015-06-03 - 00:41 JavierDuarte  
PDFpdf eff_T2tb_Jet2b.pdf r1 manage 23.0 K 2015-06-03 - 00:41 JavierDuarte  
PNGpng eff_T2tb_Jet2b.png r1 manage 172.4 K 2015-06-03 - 00:41 JavierDuarte  
PDFpdf eff_T2tb_MuEle.pdf r1 manage 22.9 K 2015-06-03 - 00:41 JavierDuarte  
PNGpng eff_T2tb_MuEle.png r1 manage 174.8 K 2015-06-03 - 00:41 JavierDuarte  
PDFpdf eff_T2tb_MuJet.pdf r1 manage 23.0 K 2015-06-03 - 00:41 JavierDuarte  
PNGpng eff_T2tb_MuJet.png r1 manage 172.0 K 2015-06-03 - 00:41 JavierDuarte  
PDFpdf eff_T2tb_MuMu.pdf r1 manage 22.6 K 2015-06-03 - 00:42 JavierDuarte  
PNGpng eff_T2tb_MuMu.png r1 manage 174.7 K 2015-06-03 - 00:42 JavierDuarte  
PDFpdf eff_T2tb_MuMultiJet.pdf r1 manage 22.7 K 2015-06-03 - 00:42 JavierDuarte  
PNGpng eff_T2tb_MuMultiJet.png r1 manage 171.9 K 2015-06-03 - 00:42 JavierDuarte  
PDFpdf eff_T2tb_MultiJet.pdf r1 manage 23.1 K 2015-06-03 - 00:42 JavierDuarte  
PNGpng eff_T2tb_MultiJet.png r1 manage 179.8 K 2015-06-03 - 00:42 JavierDuarte  
PDFpdf eff_T2tt_EleEle.pdf r1 manage 20.3 K 2015-06-03 - 00:42 JavierDuarte  
PNGpng eff_T2tt_EleEle.png r1 manage 144.2 K 2015-06-03 - 00:42 JavierDuarte  
PDFpdf eff_T2tt_EleJet.pdf r1 manage 20.5 K 2015-06-03 - 00:42 JavierDuarte  
PNGpng eff_T2tt_EleJet.png r1 manage 145.6 K 2015-06-03 - 00:42 JavierDuarte  
PDFpdf eff_T2tt_EleMultiJet.pdf r1 manage 20.5 K 2015-06-03 - 00:42 JavierDuarte  
PNGpng eff_T2tt_EleMultiJet.png r1 manage 145.1 K 2015-06-03 - 00:42 JavierDuarte  
PDFpdf eff_T2tt_Jet2b.pdf r1 manage 20.3 K 2015-06-03 - 00:42 JavierDuarte  
PNGpng eff_T2tt_Jet2b.png r1 manage 136.8 K 2015-06-03 - 00:42 JavierDuarte  
PDFpdf eff_T2tt_MuEle.pdf r1 manage 20.1 K 2015-06-03 - 00:42 JavierDuarte  
PNGpng eff_T2tt_MuEle.png r1 manage 147.1 K 2015-06-03 - 00:42 JavierDuarte  
PDFpdf eff_T2tt_MuJet.pdf r1 manage 20.5 K 2015-06-03 - 00:42 JavierDuarte  
PNGpng eff_T2tt_MuJet.png r1 manage 145.3 K 2015-06-03 - 00:42 JavierDuarte  
PDFpdf eff_T2tt_MuMu.pdf r1 manage 20.3 K 2015-06-03 - 00:42 JavierDuarte  
PNGpng eff_T2tt_MuMu.png r1 manage 136.1 K 2015-06-03 - 00:42 JavierDuarte  
PDFpdf eff_T2tt_MuMultiJet.pdf r1 manage 20.5 K 2015-06-03 - 00:42 JavierDuarte  
PNGpng eff_T2tt_MuMultiJet.png r1 manage 138.4 K 2015-06-03 - 00:42 JavierDuarte  
PDFpdf eff_T2tt_MultiJet.pdf r1 manage 20.6 K 2015-06-03 - 00:42 JavierDuarte  
PNGpng eff_T2tt_MultiJet.png r1 manage 143.8 K 2015-06-03 - 00:42 JavierDuarte  
PDFpdf nSigmaLog_EleEle.pdf r1 manage 26.6 K 2015-02-18 - 09:18 JavierDuarte  
PNGpng nSigmaLog_EleEle.png r1 manage 109.5 K 2015-02-18 - 09:18 JavierDuarte  
PDFpdf nSigmaLog_EleJet.pdf r1 manage 26.7 K 2015-02-18 - 09:18 JavierDuarte  
PNGpng nSigmaLog_EleJet.png r1 manage 121.3 K 2015-02-18 - 09:18 JavierDuarte  
PDFpdf nSigmaLog_EleMultiJet.pdf r1 manage 26.7 K 2015-02-18 - 09:18 JavierDuarte  
PNGpng nSigmaLog_EleMultiJet.png r1 manage 116.7 K 2015-02-18 - 09:18 JavierDuarte  
PDFpdf nSigmaLog_Jet2b.pdf r1 manage 26.4 K 2015-02-18 - 09:18 JavierDuarte  
PNGpng nSigmaLog_Jet2b.png r1 manage 105.1 K 2015-02-18 - 09:18 JavierDuarte  
PDFpdf nSigmaLog_MuEle.pdf r1 manage 26.5 K 2015-02-18 - 09:18 JavierDuarte  
PNGpng nSigmaLog_MuEle.png r1 manage 100.8 K 2015-02-18 - 09:18 JavierDuarte  
PDFpdf nSigmaLog_MuJet.pdf r1 manage 26.7 K 2015-02-18 - 09:18 JavierDuarte  
PNGpng nSigmaLog_MuJet.png r1 manage 118.5 K 2015-02-18 - 09:18 JavierDuarte  
PDFpdf nSigmaLog_MuMu.pdf r1 manage 26.6 K 2015-02-18 - 09:18 JavierDuarte  
PNGpng nSigmaLog_MuMu.png r1 manage 104.5 K 2015-02-18 - 09:18 JavierDuarte  
PDFpdf nSigmaLog_MuMultiJet.pdf r1 manage 26.7 K 2015-02-18 - 09:19 JavierDuarte  
PNGpng nSigmaLog_MuMultiJet.png r1 manage 114.5 K 2015-02-18 - 09:19 JavierDuarte  
PDFpdf nSigmaLog_MultiJet.pdf r1 manage 26.9 K 2015-02-18 - 09:18 JavierDuarte  
PNGpng nSigmaLog_MultiJet.png r1 manage 151.9 K 2015-02-18 - 09:18 JavierDuarte  
PDFpdf nSigmaLog_MultiJetFITS.pdf r1 manage 26.4 K 2015-02-18 - 09:18 JavierDuarte  
PNGpng nSigmaLog_MultiJetFITS.png r1 manage 110.9 K 2015-02-18 - 09:18 JavierDuarte  
PDFpdf naturalSpectrum.pdf r1 manage 80.3 K 2015-02-18 - 09:18 JavierDuarte  
PNGpng naturalSpectrum.png r1 manage 315.2 K 2015-02-18 - 09:18 JavierDuarte  
PNGpng razor_8TeV_sms_results.png r1 manage 84.0 K 2015-06-03 - 01:16 JavierDuarte  
Unknown file formatroot razor_8TeV_sms_results.root r1 manage 354.6 K 2015-06-03 - 00:17 JavierDuarte  
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Topic revision: r9 - 2015-08-25 - JavierDuarte
 
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