Early LHC data preparations for SUSY searches at CMS Didar Dobur University of Florida Representing the CMS Collaboration ICHEP 22-28 July 2010, Paris.

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Presentation transcript:

Early LHC data preparations for SUSY searches at CMS Didar Dobur University of Florida Representing the CMS Collaboration ICHEP July 2010, Paris

Introduction Didar Dobur 2/18 ICHEP 2010 Paris  7 TeV data of ~100 pb -1 should provide sensitivity to SUSY parameter space well beyond the current limits set by TEVATRON  The sensitivity reach strongly depends on how well we understand the SM backgrounds sensitivity to mSUGRA with fully hadronic signaure Sensitivity with Same-Sign di-lepton CMS TEVATRON

Introduction Didar Dobur 3/18 ICHEP 2010 Paris  Suppressing QCD using topological observables  Predicting QCD contributions to Missing E T (MET)  data-driven techniques to measure QCD background for lepton(s) + Jets +MET signatures  Strategies to suppress and measure SM backgrounds are studied in detail using MC in the past years  7 TeV data used (11-65 nb -1 ) for testing some of these methods in the available phase-space (not yet where we expect SUSY signal)  QCD is not expected to be dominant background for most of the search topologies, but poorly known (large!) cross sections, need to be measured from data: Material used in this presentation is documented in SUS , and see JME for detailed MET studies for SUSY searches, see Slide 18 for full references

Suppressing QCD with  T  A powerful variable for suppressing mis-measured QCD  Well measured back-to-back di-jet system α T ≈0.5, if one jet is mis-measured α T <0.5 √s= 10 TeV MC The data shows the expected sharp fall around α T ~ 0.5, improves for higher H T Didar Dobur 4/18 ICHEP 2010 Paris 2 Jets H T [80,120] 2 Jets H T >120 GeV SUSY Study fraction of events with α T >0.55

H T dependence of  T  Rejection power of  T is expected to get better with increasing H T  Examine this assumption in the available H T range: Expected decrease (approx. exponential) with H T is observed for both 2-jet and ≥3-jets Better performance with increasing H T holds also for: Extended also for leptonic search channels (not shown here) Didar Dobur 5/18 ICHEP 2010 Paris  In  +jet(s) events where photon is treated as a jet  Emulating extreme jet losses  Smearing jet energies 2-Jet multi-Jet

 T versus pseudorapidity √s= 10 TeV MC  Having verified α T behavior with H T, one can use data at lower H T to estimate SM background at high H T by exploiting its expected uniformity versus   The method was studied with 10 TeV MC  Fraction of events with α T >0.55 as a function of the leading jet  Flat behavior across , even when a jet is removed Didar Dobur 6/18 ICHEP 2010 Paris SUSY + SM

Suppressing QCD with  *  A complementary observable,  *, to diagnose background events where one jet mis-measured.  Test each jet to see if it is responsible for the MHT (vectorial sum of the jet p T )  expect small  * for QCD  more uniform for real MET (emulated by removing one jet) Data confirms the expected behavior in both di- and multi-jets Resolution improves with H T Didar Dobur 7/18 ICHEP 2010 Paris  jkjk MHT

Tracker (MPT) vs Calorimeter (MHT)  Independent measurement of missing momentum from Tracker & Calorimeter  Compare the direction of MPT and MHT, Δ ϕ (MPT,MHT) Very little correlation between the directions of MPT and MHT when no real MHT is present (QCD) peaks towards zero for real MHT (emulated by removing a random jet) Also useful to remove events with a fake MHT due to noise in the calorimeter Didar Dobur 8/18 ICHEP 2010 Paris

Predicting high MET tail  MET background to lepton+jets+MET signatures from real MET (e.g. in W/Z) and MET due to mis-measurements  Test the method for the latter  Use MET templates from multi-jet events to predict MET for  +jets events Good agreement between predicted and observed distributions: for MET > 15 GeV predicted = 12.5 observed = 11 Didar Dobur 9/18 ICHEP 2010 Paris p T (  ) > 15 GeV p T (Jet) > 40 GeV MET templates from multi-jet events

Predicting MET tail in  search Didar Dobur 10/18 ICHEP 2010 Paris   + MET is one of the early search channels  Physics backgrounds W   W , electron mis-id as   multi-jet (direct  + fake MET (dominant)  Prediction:  Measure MET distribution in a control sample with 2 fake photons, selected by inverting Isolation requirement  Use number of selected events at MET < 10 GeV to normalize the measured templates. Prediction consistent with number of observed events, For MET > 20 GeV: Predicted = 4.2 ± 1.5 Observed = 4 events

QCD background for e+Jets+MET  QCD contributes to e + Jets+ MET signature  heavy-flavor decays and jets mis-identified as electron  electrons due to photon conversion  Select control samples dominated by each of above sources by inverting selection cuts perform fit using Relative Isolation distributions  Isolation template for W  e ν contribution from MC Didar Dobur 11/18 ICHEP 2010 Paris (RelIso<0.3) Predicted : 224 ± 13 Observed : 263 (RelIso<0.3) Predicted : 215 ± 13 Observed : 215 MET < 20 GeV

QCD background for  +Jets+MET  QCD contributes to  + Jets+ MET signature :  mainly due to heavy-flavor decays to muons  A fit procedure for Relative Isolation to predict bckgrd from non-prompt muons Didar Dobur 12/18 ICHEP 2010 Paris Good agreement between Predicted and Observed event yield in the signal region MET < 20 GeV H T >20 GeV MET > 20 GeV Prompt : ± 17.9, Observed= 248 Bckgrd : 66.2 ± 11.3, Observed =72

ttBar background for SS di-   ttBar is the dominant background for Same-Sign (SS) di-μ signature: one from W and the other from b-decays  Isolation is the main handle  Tag&Probe method to measure isolation distribution of muons coming from heavy flavor decays Strong dependency on the event topology, e.g. jet multiplicity Didar Dobur 13/18 ICHEP 2010 Paris

Muon Isolation Template Didar Dobur 14/18 ICHEP 2010 Paris  Significant differences in jet multiplicity and p T (μ) in ttBar and generic QCD  Re-weighting procedure to take this difference into account The agreement between QCD MC ( data-driven ) and ttBar MC ( matching to the generator level ) demonstrates the principle of the method Data agrees qualitatively with ttBar MC, for a quantitative prediction more data is necessary

QCD background for SS di-  Didar Dobur 15/18 ICHEP 2010 Paris  QCD is expected to be the subdominant background for SS di-μ signature  Exploit the fact that some selection cuts are uncorrelated  selection efficiency for each cut can be measured in control samples IsoCut(   ) : Isolation of  , ε Iso  IsoCut(   ) : Isolation of  , ε Iso  METCut : third jet and MET, ε MET  test the factorization of cuts IsoCut(   ) and IsoCut(   ), no jet & MET requirement yet data indicates isolation of the  1 and  2 can be factorized ε AllCuts = ε Iso . ε Iso . ε MET ε Iso  = (ε Iso  ) 2 ?

SM background for SS di-lepton Monitor measured Tight-to-Loose-Ratios using different jet-triggered samples. Didar Dobur 16/18 ICHEP 2010 Paris  Data driven method for estimating SM background for SS ee,  and e  channels  Use a control sample (loose lepton-id & isolation) to measure efficiency of passing all analysis cuts, ( “TL ratio” ), as a function of lepton kinematics. Predictions obtained using HLT_Jet15U Electrons Muons Measured TL ratio is stable within 50% Predicted & observed number of SS di-lepton events consistent

Summary & Outlook Didar Dobur 17/18 ICHEP 2010 Paris Understanding of the SM background is the first step towards BSM searches Dedicated methods to suppress the backgrounds and data-driven techniques to measure them from data are in place The data collected by CMS at 7 TeV allowed us to test some of these methods; data confirms the performance of the methods obtained with MC LHC performs very well; as of today four times more ( ~300 nb -1 ) data than what is presented here is available Stay tuned for updates, we are at the beginning of an exciting journey

References Didar Dobur 18/18 ICHEP 2010 Paris 1. “Performance of Methods for Data-Driven Background Estimation in SUSY Searches”, CMS Physics Analysis Summary: SUS “CMS MET Performance in Jet Events from pp Collisions at sqrt s= 7 TeV”, JME “The CMS physics reach for searches at 7 TeV “, CMS-NOTE “SUSY searches with dijet events”, CMS Physics Analysis Summary: SUS “Search strategy for exclusive multi-jet events from supersymmetry at CMS”, CMS Physics Analysis Summary: SUS “Data-Driven Background Estimates for SUSY Di-Photon Searches”, CMS Physics Analysis Summary: SUS L.Randall and D. Tucker-Smith, “Dijet searches for Supersymmetry at the LHC ”, Phys.RevLett (2008)