Difference: PhysicsResultsEXO12048 (34 vs. 35)

Revision 352014-09-22 - PhatSrimanobhas

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META TOPICPARENT name="HcalRocMonoJet2012"

Search for new physics in monojet events in pp collisions at sqrt(s) = 8 TeV

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LimitComparison_Unparticle_Spin0_19fb.jpg The expected and observed lower limits on the unparticle model parameters ΛU as a function of dU at 95% CL, compared to previous result. The shaded region indicates the side of the curve that is excluded.
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Public supplemental material

Figure Caption
The transverse momentum of Jet-1 after all selections for data and SM backgrounds. The processes contributing to the SM background are from simulation, normalised to the estimation from data using the MET threshold of 500 GeV. The shaded bands in the lower panel represent the statistical uncertainty. Overflow events are included in the last bin.
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The jet multiplicity disctibution after all selections for data and SM backgrounds. The processes contributing to the SM background are from simulation, normalised to the estimation from data using the MET threshold of 500 GeV. The shaded bands in the lower panel represent the statistical uncertainty. Overflow events are included in the last bin.
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Distribution of DeltaPhi betwen Jet-1 and Jet-2 after all selections for data and SM backgrounds. The processes contributing to the SM background are from simulation, normalised to the estimation from data using the MET threshold of 500 GeV. The shaded bands in the lower panel represent the statistical uncertainty. Overflow events are included in the last bin.
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The invariant mass distribution of the Z(mu,mu) control sample within the Z mass window 60-120 GeV after all monojet selections are applied, except muon veto.
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The transverse momentum distribution of the Z(mu,mu) control sample within the Z mass window 60-120 GeV. All monojet selections are applied, except the muon veto.
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The transverse mass distribution of the W(mu,nu) control sample. No mass window selection is applied here. All monojet selections are applied, except the muon veto. Overflow events are included in the last bin.
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The transverse momentum distribution of the W(mu,nu) control sample within the mass window 50-100 GeV. All monojet selections are applied, except the muon veto.
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Event displays from EXO-12-048

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(click on the event display to get PNG)
 
Event Details ρφ View ρZ View 3D View
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Run 204553

Event 26729384

Monojet candidate event

Monojet_Rho-Phi.png Monojet_Rho-Z.png Monojet_3DTower_AllDet.png
Run 204553

Event 36479045

W(mu+nu) + jets candidate event. The W(mu+nu) + jets events are used to predict the remaining W+jets background in monojet analysis.

W_Rho-Phi.png W_Rho-Z.png W_3DTower_AllDet.png
Run 204564

Event 448966153

Z(mu+mu) + jets candidate event. The Z(mu+mu) + jets events are used to predict the invisible Z background in monojet analysis.

Z_Rho-Phi.png Z_Rho-Z.png Z_3DTower_AllDet.png
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Run 204553

Event 26729384

Monojet candidate event

Monojet_Rho-Phi.png Monojet_Rho-Z.png Monojet_3DTower_AllDet.png
Download PDF Download PNG Download PDF Download PNG Download PDF Download PNG
Run 204553

Event 36479045

W(mu+nu) + jets candidate event. The W(mu+nu) + jets events are used to predict the remaining W+jets background in monojet analysis.

W_Rho-Phi.png W_Rho-Z.png W_3DTower_AllDet.png
Download PDF Download PNG Download PDF Download PNG Download PDF Download PNG
Run 204564

Event 448966153

Z(mu+mu) + jets candidate event. The Z(mu+mu) + jets events are used to predict the invisible Z background in monojet analysis.

Z_Rho-Phi.png Z_Rho-Z.png Z_3DTower_AllDet.png
Download PDF Download PNG Download PDF Download PNG Download PDF Download PNG
 
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