Difference: PhysicsResultsSUS10006 (15 vs. 16)

Revision 162011-04-15 - RobertSchoefbeck

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META TOPICPARENT name="PhysicsResultsSUS"

Search for new physics in proton-proton collisions at 7 TeV in events with a single lepton, jets, and missing transverse momentum

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RA4_Ele_pf-4j30_ht_lin.gif Fig.2b: Distribution of HT in the electron channel. The preselection requirements as well as MET>25 GeV have been applied. The yield for W+jets has been adjusted to have equal event numbers for data and simulation.
RA4_Ele_pf-4j30_lepton_pt_lin.gif Fig.2c: Distribution of electron pT. The preselection requirements as well as MET>25 GeV have been applied. The yield for W+jets has been adjusted to have equal event numbers for data and simulation.
RA4_table_regions.gif Tab.1: Definition of loose and tight regions for the ABCD method.
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RA4_table_region_counts_a.gif Tab.2: Predicted and observed yields in the different regions of the ABCD method. The yields from simulation are included for comparison - the actual prediction is based on data.
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RA4_table_region_counts_a.png Tab.2: Predicted and observed yields in the different regions of the ABCD method. The yields from simulation are included for comparison - the actual prediction is based on data.
 
RA4_Mu_pf-4j30_mc_htVSkinMetSig.gif Fig.3a: Distribution of HT vs. MET/sqrt(HT) for standard model backgrounds (simulation) in the muon channel. The control regions ABC and the signal region D are shown for the tight selection.
RA4_Mu_pf-4j30_lm1_htVSkinMetSig.gif Fig.3b: Distribution of HT vs. MET/sqrt(HT) for the SUSY benchmark point LM1 (simulation) in the muon channel.
RA4_Ele_pf-4j30_data_htVSkinMetSig.gif Fig.3c: Distribution of HT vs. MET/sqrt(HT) for data in the electron channel.
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