Difference: ProspectsforSUSYandUED (1 vs. 7)

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ProspectsforSUSYandUED

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Introduction

This note presents an evaluation of the discovery potential of Supersymmetry and Universal Extra Dimensions for channels with jets, leptons and missing transverse energy. The LHC running scenario at a centre-of-mass energy of 10 TeV, delivering an integrated luminosity of $200 {pb}^{-1}$ for the 2009-2010 run is investigated.
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The ATL-PHYS-PUB-2009-084 note can be found here
 Figure 1

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ProspectsforSUSYandUED

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  Figure3: Effective mass distributions for the 2 jet (upper plot), 3 jet (middle plot) and 4 jet channel (lower plot) with 0 leptons.
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Figure 4: Missing transverse energy distributions for the 4 jet channel with 0 leptons.

Figure 5

 
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Figure4: Effective mass distributions for the 2 jet (upper plot), 3 jet (middle plot) and 4 jet channel (lower plot) with 1 lepton.
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Figure5: Effective mass distributions for the 2 jet (upper plot), 3 jet (middle plot) and 4 jet channel (lower plot) with 1 lepton.
 
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Figure5: Effective mass distributions for the 2 jet (upper plot), 3 jet (middle plot) and 4 jet channel (lower plot) with 2 leptons with opposite sign (OS) charge.
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Figure6: Effective mass distributions for the 2 jet (upper plot), 3 jet (middle plot) and 4 jet channel (lower plot) with 2 leptons with opposite sign (OS) charge.
 
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Figure 7
 

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Figure 6: $M_T$ distributions for the 4 jet channel with 1 lepton.
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Figure 7: $M_T$ distributions for the 4 jet channel with 1 lepton.
 
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Figure 8
 
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Figure 7: $5\sigma$ discovery reach as a function of $m_{0}$ and $m_{1/2}$ for $\tan \beta =10$ mSUGRA scan for channels with 0, 1 and 2 leptons. Only the channels with the largest discovery reach are shown for each lepton multiplicity.
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Figure 8: $5\sigma$ discovery reach as a function of $m_{0}$ and $m_{1/2}$ for $\tan \beta =10$ mSUGRA scan for channels with 0, 1 and 2 leptons. Only the channels with the largest discovery reach are shown for each lepton multiplicity.
 
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Figure 9
 
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Figure 8: 5\sigma$ discovery reach as a function of $m_{0}$ and $m_{1/2}$ for $\tan \beta =50$ mSUGRA scan for channels with 0 and 1 leptons.
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Figure 9: 5\sigma$ discovery reach as a function of $m_{0}$ and $m_{1/2}$ for $\tan \beta =50$ mSUGRA scan for channels with 0 and 1 leptons.
 
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Figure 10
 
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Figure 9: The points of the pMSSM grids with constraints as a function of the total cross section and the minimal SUSY mass (upper plot) and as a function of the minimal mass of the light squarks and the mass of the gluino (lower plot).
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Figure 10: The points of the pMSSM grids with constraints as a function of the total cross section and the minimal SUSY mass (upper plot) and as a function of the minimal mass of the light squarks and the mass of the gluino (lower plot).
 
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Figure 11
 
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Figure 10: Significance $\sigma$ as a function of $1/R$ for the Universal Extra Dimensions scenario, taking into account channels with 0, 1 and 2 leptons.
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Figure 11: Significance $\sigma$ as a function of $1/R$ for the Universal Extra Dimensions scenario, taking into account channels with 0, 1 and 2 leptons.
 

Table1

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ProspectsforSUSYandUED

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ProspectsforSUSYandUED

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Introduction

This note presents an evaluation of the discovery potential of Supersymmetry and Universal Extra Dimensions for channels with jets, leptons and missing transverse energy. The LHC running scenario at a centre-of-mass energy of 10 TeV, delivering an integrated luminosity of $200 {pb}^{-1}$ for the 2009-2010 run is investigated. Figure 1

Figure 1: Parameters of the pMSSM with constraints grid. Shown are (from top to bottom) the distribution of $\tan \beta$, the mass of the gluino versus the mass of the light squarks, the mass of the $\chi_{0}^{1}$ and the mass of the $\tilde{t}_{1}$. The lowest plot shows the distribution of the various types of nLSP for the same pMSSM models.

Figure 2

Figure2: Number of events expected for 200 $\rm{pb}^{-1}$ in 0-lepton channels and multi-leptons channels after preselection for the main background processes and the SUSY signal SU4.

Figure 3

Figure3: Effective mass distributions for the 2 jet (upper plot), 3 jet (middle plot) and 4 jet channel (lower plot) with 0 leptons.

Figure 4

Figure4: Effective mass distributions for the 2 jet (upper plot), 3 jet (middle plot) and 4 jet channel (lower plot) with 1 lepton.

Figure 5

Figure5: Effective mass distributions for the 2 jet (upper plot), 3 jet (middle plot) and 4 jet channel (lower plot) with 2 leptons with opposite sign (OS) charge.

Figure 6

Figure 6: $M_T$ distributions for the 4 jet channel with 1 lepton.

Figure 7

Figure 7: $5\sigma$ discovery reach as a function of $m_{0}$ and $m_{1/2}$ for $\tan \beta =10$ mSUGRA scan for channels with 0, 1 and 2 leptons. Only the channels with the largest discovery reach are shown for each lepton multiplicity.

Figure 8

Figure 8: 5\sigma$ discovery reach as a function of $m_{0}$ and $m_{1/2}$ for $\tan \beta =50$ mSUGRA scan for channels with 0 and 1 leptons.

Figure 9

Figure 9: The points of the pMSSM grids with constraints as a function of the total cross section and the minimal SUSY mass (upper plot) and as a function of the minimal mass of the light squarks and the mass of the gluino (lower plot).

Figure 10

Figure 10: Significance $\sigma$ as a function of $1/R$ for the Universal Extra Dimensions scenario, taking into account channels with 0, 1 and 2 leptons.

Table1

Process Generator Simulation $N_{\rm points}$ $N_{\rm events}$ per point
mSUGRA $\tan \beta =10$ HERWIG 6.5 ATLFAST2 76 30000
mSUGRA $\tan \beta =50$ HERWIG 6.5 & ATLFAST2 23 30000
pMSSM constraints PYTHIA 6.4 ATLFAST1 150 30000
UED PYTHIA 6.4 ATLFAST2 8 5000-100000

Table1: The Monte Carlo generator, detector simulation programme, the number of points in parameter space per model, and the number of events per point for all signal samples.

Table2

Process Generator $N_{events}$ $\sigma * BR * \it{eff}$ Simulation
\ttbar($\ell\nu qq$ + $\ell\nu\ell\nu$) MC@NLO+JIMMY 3327021 202.86 GEANT4
\ttbar($qqqqbb$) MC@NLO+JIMMY 3685781 170.74 ATLFAST2
Single top ($Wt$ + tchan) AcerMC 14281 55.53 GEANT4
QCD bb $(35<p_{T}<70)$ ALPGEN+JIMMY 70000 7522.42 ATLFAST2
QCD bb $(70<p_{T}<140)$ ALPGEN+JIMMY 289999 29119.15 ATLFAST2
QCD bb $(140<p_{T}<280)$ ALPGEN+JIMMY 45000 4384.20 ATLFAST2
QCD bb $(p_T>280)$ ALPGEN+JIMMY 57467 186.80 ATLFAST2
QCD udsc $(35<p_{T}<70)$ ALPGEN+JIMMY 2827992 375056.88 ATLFAST2
QCD udsc $(70<p_{T}<140)$ ALPGEN+JIMMY 1390216 1193879.82 ATLFAST2
QCD udsc $(140<p_{T}<280)$ ALPGEN+JIMMY 1821843 182230.10 ATLFAST2
QCD udsc $(p_T>280)$ ALPGEN+JIMMY 1938961 7210.30 ATLFAST2
$W \rightarrow e\nu$ + jets ALPGEN+JIMMY 3110747 13249.00 ATLFAST2
$W \rightarrow \mu\nu$ + jets ALPGEN+JIMMY 1635166 13237.30 ATLFAST2
$W \rightarrow \tau\nu$ + jets ALPGEN+JIMMY 2113632 13233.00 ATLFAST2
\Zboson \rarrow ee + jets ALPGEN+JIMMY 635835 1206.10 ATLFAST2
\Zboson \rarrow $\mu\mu$ + jets ALPGEN+JIMMY 605000 1204.20 ATLFAST2
\Zboson \rarrow $\nu\nu$ + jets ALPGEN+JIMMY 2399496 7056.30 ATLFAST2
\Zboson \rarrow $\tau\tau$ + jets ALPGEN+JIMMY 566498 1211.00 ATLFAST2
$WW$ gg2WW +JIMMY 52391 0.28 GEANT4
\Wminus\Zboson MC@NLO+JIMMY 16807 21.75 GEANT4
\Wplus\Wminus MC@NLO+JIMMY 41108 7.14 GEANT4
\Wplus\Zboson MC@NLO+JIMMY 7286 37.28 GEANT4
\Zboson\Zboson MC@NLO+JIMMY 13456 18.41 GEANT4

Table2 : Summary of Standard Model datasets used in this analysis. The QCD samples are subdivided according to the $p_T$ (GeV) of the leading jet and the type of quark produced. $N_{events}$ is the sum of MC weights, i.e. weight = \pm1$ for events produced with the MC@NLO generator. The cross section reduced by the branching ratio and the generator level filter efficiency is $\sigma * BR * eff.

Table3:

The number of background and SU4 events for the plots Figure 3-5 can be found here: number_of_events.txt

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