Search for supersymmetry with the vector boson fusion topology in proton-proton collisions at collisions at $\sqrt{s}=8$ CMS.TeV

Abstract

The first search for supersymmetry with the vector boson fusion (VBF) topology is presented. The VBF topology offers a promising avenue to study the electroweak sector of supersymmetry. The search targets final states with at least two leptons, large missing transverse momentum, and two jets with a large pseudorapidity gap. The data sample used in this analysis corresponds to an integrated luminosity of 19.7$fb^{-1}$ of pp collisions at $\sqrt{s}=8$ CMS.TeV collected with the CMS detector. The observed dijet invariant mass spectrum after the final selections is consistent with the expected standard model predictions. Upper limits are set for the production of charginos and neutralinos with two associated jets, where sleptons are ligher than charginos.

Approved tables and plots

Tables in Paper

Tables Caption
Number of observed events in data and estimated background rates for the OS search channels. The uncertainties are based on the number of observed events in the control regions as well as the statistics in simulation.
Number of observed events in data and estimated background rates for the LS channels. The uncertainties are based on the number of observed events in the control regions as well as the statistics in simulation.
Cumulative signal acceptance for m(j,j) > 250 CMS.GeV.
Simulated yield of signal events. The terms in only curly brackets, {m(${\tilde{\chi}^{\pm}_{1}}$), m(${\tilde{\tau_{1}}}$)}, represent the scenarios where $\Delta$m(${\tilde{\chi}^{\pm}_{1}}, {\tilde{\tau_{1}}}$) = 5 CMS.GeV, while the terms in parenthesis, ({m(${\tilde{\chi}^{\pm}_{1}}$), m(${\tilde{\tau_{1}}}$)}), are for scenarios where m(${\tilde{\tau_{1}}}$) = 1/2m(${\tilde{\chi}^{\pm}_{1}}$) + 1/2m(${\tilde{\chi}^{0}_{1}}$).

Plots in Paper

  Figures Caption
a m(j, j) distributions in the (a) OS ${\mu\mu}$, (b) LS ${\mu\mu}$, (c) OS ${e\mu}$, and (d) LS ${e\mu}$ signal regions. The signal scenario with m(${\tilde{\chi}^{0}_{2}})$ = m(${\tilde{\chi}^{\pm}_{1}}$) = 200 CMS.GeV, m(${\tilde{\tau_{1}}}$) = 195 CMS.GeV, and m(${\tilde{\chi}^{0}_{1}}$)= 0 CMS.GeV is shown. The shaded band in the ratio plot corresponds to the systematic uncertainty on the background prediction.
b
c
d
a m(j, j) distributions in the (a) OS ${\mu\tau_{h}}$, (b) LS ${\mu\tau_{h}}$, (c) OS ${\tau_{h}\tau_{h}}$, and (d) LS ${\tau_{h}\tau_{h}}$ signal regions. The signal scenario with m(${\tilde{\chi}^{0}_{2}})$ = m(${\tilde{\chi}^{\pm}_{1}}$) = 200 CMS.GeV, m(${\tilde{\tau_{1}}}$) = 195 CMS.GeV, and m(${\tilde{\chi}^{0}_{1}}$)= 0 CMS.GeV is shown. The shaded band in the ratio plot corresponds to the systematic uncertainty on the background prediction.
b
c
d
a (a) m(j,j) efficiencies for the Z and $t\bar{t}$ control regions of the $\mu\mu$jj final state. (b) m(j,j) signal region distribution for the combination of all search channels. The signal scenario with m(${\tilde{\chi}^{0}_{2}})$ = m(${\tilde{\chi}^{\pm}_{1}}$) = 200 CMS.GeV, m(${\tilde{\tau_{1}}}$) = 195 CMS.GeV, and m(${\tilde{\chi}^{0}_{1}}$)= 0 CMS.GeV is shown. The shaded band in the ratio plot corresponds to the systematic uncertainty on the background prediction.
b
a Combined 95% CL upper limits on the cross section as a function of m(${\tilde{\chi}^{0}_{2}})$ = m(${\tilde{\chi}^{\pm}_{1}}$). The figure (a) shows the upper limits for the scenario where m(${\tilde{\tau_{1}}}$) is defined as m(${\tilde{\chi}^{\pm}_{1}}$) - m(${\tilde{\tau_{1}}}$) = 5 CMS.GeV, for two different m(${\tilde{\chi}^{0}_{1}}$) definitions:m(${\tilde{\chi}^{\pm}_{1}}$) - m(${\tilde{\chi}^{0}_{1}}$) = 50 CMS.GeV (compressed spectra) and m(${\tilde{\chi}^{0}_{1}}$) = 0 CMS.GeV (large mass gap). The figure (b) shows the upper limits for the scenarios where is defined as m(${\tilde{\tau_{1}}}$) = 1/2m(${\tilde{\chi}^{\pm}_{1}}$) + 1/2m(${\tilde{\chi}^{0}_{1}}$), for the same two m(${\tilde{\chi}^{0}_{1}}$) definitions.
b

-- ShoMaruyama - 2015-03-07

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PDFpdf DiJetMass_combined.pdf r4 r3 r2 r1 manage 20.6 K 2015-03-20 - 20:25 ShoMaruyama  
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PDFpdf DiJetMass_combined_preliminary.pdf r3 r2 r1 manage 20.6 K 2015-03-20 - 20:25 ShoMaruyama  
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PDFpdf DiJetMass_diMu_LS.pdf r6 r5 r4 r3 r2 manage 19.6 K 2015-03-20 - 20:25 ShoMaruyama  
PNGpng DiJetMass_diMu_LS.png r6 r5 r4 r3 r2 manage 29.2 K 2015-03-20 - 20:25 ShoMaruyama  
PDFpdf DiJetMass_diMu_LS_preliminary.pdf r3 r2 r1 manage 19.6 K 2015-03-20 - 20:25 ShoMaruyama  
PNGpng DiJetMass_diMu_LS_preliminary.png r3 r2 r1 manage 29.9 K 2015-03-20 - 20:25 ShoMaruyama  
PDFpdf DiJetMass_diMu_OS.pdf r6 r5 r4 r3 r2 manage 20.3 K 2015-03-20 - 20:25 ShoMaruyama  
PNGpng DiJetMass_diMu_OS.png r6 r5 r4 r3 r2 manage 31.2 K 2015-03-20 - 20:25 ShoMaruyama  
PDFpdf DiJetMass_diMu_OS_preliminary.pdf r3 r2 r1 manage 20.3 K 2015-03-20 - 20:25 ShoMaruyama  
PNGpng DiJetMass_diMu_OS_preliminary.png r3 r2 r1 manage 31.9 K 2015-03-20 - 20:25 ShoMaruyama  
PDFpdf DiJetMass_diTau_LS.pdf r4 r3 r2 r1 manage 21.1 K 2015-03-20 - 20:25 ShoMaruyama  
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PDFpdf DiJetMass_diTau_LS_preliminary.pdf r3 r2 r1 manage 21.1 K 2015-03-20 - 20:25 ShoMaruyama  
PNGpng DiJetMass_diTau_LS_preliminary.png r3 r2 r1 manage 33.1 K 2015-03-20 - 20:25 ShoMaruyama  
PDFpdf DiJetMass_diTau_OS.pdf r4 r3 r2 r1 manage 20.9 K 2015-03-20 - 20:25 ShoMaruyama  
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PDFpdf DiJetMass_diTau_OS_preliminary.pdf r3 r2 r1 manage 20.9 K 2015-03-20 - 20:25 ShoMaruyama  
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PDFpdf DiJetMass_eMu_LS.pdf r6 r5 r4 r3 r2 manage 18.9 K 2015-03-20 - 20:26 ShoMaruyama  
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PDFpdf DiJetMass_eMu_OS.pdf r6 r5 r4 r3 r2 manage 20.0 K 2015-03-20 - 20:26 ShoMaruyama  
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PDFpdf DiJetMass_eMu_OS_preliminary.pdf r3 r2 r1 manage 20.0 K 2015-03-20 - 20:26 ShoMaruyama  
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