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Search for the standard model Higgs boson decaying to $W^+ W^-$ in the fully leptonic final state in pp collisions at $\sqrt{s}$ = 7 TeV

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Download Search for the standard model Higgs boson decaying to $W^+ W^-$ in the fully leptonic final state in pp collisions at $\sqrt{s}$ = 7 TeV
  EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH (CERN) CERN-PH-EP/2012-0182012/02/08 CMS-HIG-11-024 Search for the standard model Higgs boson decaying toW + W −  in the fully leptonic final state in pp collisions at √  s = 7 TeV The CMS Collaboration ∗ Abstract A search for the standard model Higgs boson decaying to W + W −  in pp collisions at √  s  =  7TeV is reported. The data are collected at the LHC with the CMS detector,and correspond to an integrated luminosity of 4.6fb − 1 . The W + W −  candidates areselected in events with two charged leptons and large missing transverse energy. Nosignificant excess of events above the standard model background expectations isobserved, and upper limits on the Higgs boson production relative to the standardmodel Higgs expectation are derived. The standard model Higgs boson is excludedin the mass range 129–270GeV at 95% confidence level. Submitted to Physics Letters B ∗ See Appendix A for the list of collaboration members   a  r   X   i  v  :   1   2   0   2 .   1   4   8   9  v   1   [   h  e  p  -  e  x   ]   7   F  e   b   2   0   1   2  1 1 Introduction One of the open questions in the standard model (SM) of particle physics [1–3] is the srcin of  the masses of fundamental particles. Within the SM, vector boson masses arise by the sponta-neous breaking of electroweak symmetry by the Higgs field [4–9]. The existence of the associ- ated field quantum, the Higgs boson, has yet to be established experimentally. The discoveryor the exclusion of the SM Higgs boson is one of the central goals of the CERN Large HadronCollider (LHC) physics program.Direct searches at the CERN e + e −  LEP collider set a limit on the Higgs boson mass  m H  > 114.4GeV at 95% confidence level (CL) [10]. Precision electroweak data constrain the mass of the SM Higgs boson to be less than 158GeV at 95% CL [11]. The SM Higgs boson is excludedat 95% CL by the Tevatron collider experiments in the mass range 162–166GeV [12], and bythe ATLAS experiment in the mass ranges 145–206, 214–224, 340–450GeV [13–15]. The H  → W + W −  → 2  2 ν  final state, where  is a charged lepton and  ν  a neutrino, was first proposed asa clean channel at the LHC in [16]. A previous search for the Higgs boson at the LHC in thisfinal state was published by the Compact Muon Solenoid (CMS) collaboration with 36pb − 1 of integrated luminosity [17]. This search is performed over the mass range 110–600GeV, and thedata sample corresponds to 4.6 ± 0.2fb − 1 of integrated luminosity collected in 2011 at a center-of-mass energy of 7TeV. A similar search was conducted by the ATLAS collaboration [13]. 2 CMS detector and simulation In lieu of a detailed description of the CMS detector [18], which is beyond the scope of theletter, a synopsis of the main components follows. The superconducting solenoid occupiesthe central region of the CMS detector, providing an axial magnetic field of 3.8T parallel tothe beam direction. Charged particle trajectories are measured by the silicon pixel and striptracker, which cover a pseudorapidity region of  | η |  < 2.5. Here, the pseudorapidity is definedas  η  =  − ln ( tan θ /2 ) , where  θ  is the polar angle of the trajectory of the particle with respectto the direction of the counterclockwise beam. The crystal electromagnetic calorimeter (ECAL)and the brass/scintillator hadron calorimeter (HCAL) surround the tracking volume and cover | η | < 3. The steel/quartz-fiber Cherenkov calorimeter (HF) extends the coverage to  | η |  < 5. The muon system consists of gas detectors embedded in the iron return yoke outside thesolenoid, with a coverage of   | η |  <  2.4. The first level of the CMS trigger system, composedof custom hardware processors, is designed to select the most interesting events in less than3 µ s, using information from the calorimeters and muon detectors. The High Level Triggerprocessor farm further reduces the event rate to a few hundred Hz before data storage.The expected SM Higgs cross section is 10 orders of magnitude smaller than the LHC in-elastic cross section, which is dominated by QCD processes. Selecting final states with twoleptons and missing energy eliminates the bulk of the QCD events, leaving non-resonant di- boson production (pp  →  W + W − , WZ, W γ , ZZ), Drell-Yan production (DY), top production(tt and tW), and W  +  jets and QCD multijet processes, where at least one jet is misidenti-fied as a lepton, as the background sources. Several Monte Carlo event generators are usedto simulate the signal and background processes. The  POWHEG  2.0 program [19] providesevent samples for the H  →  W + W −  signal and the Drell-Yan, tt, and tW processes. Theqq → W + W −  and W +  jets processes are generated using the  MADGRAPH  5.1.3 [20] event gen-erator, thegg → W + W −  processusing  GG 2 WW  [21], andtheremainingprocessesusing  PYTHIA 6.424 [22]. For leading-order generators, the default set of parton distribution functions (PDF)used to produce these samples is  CTEQ 6 L  [23], while  CT 10 [24] is used for next-to-leading or-  2  3  W + W − event selection der (NLO) generators. Cross section calculations [25] at next-to-next-to-leading order (NNLO)are used for the H  →  W + W −  process, while NLO calculations are used for background crosssections. For all processes, the detector response is simulated using a detailed description of the CMS detector, based on the  GEANT 4 package [26]. The simulated samples are reweightedto represent the distribution of number of pp interactions per bunch crossing (pile-up) as mea-sured in the data. 3  W + W − event selection The search strategy for H  →  W + W −  exploits diboson events where both W bosons decayleptonically, resulting in an experimental signature of two isolated, high transverse momen-tum (  p T ), oppositely charged leptons (electrons or muons) and large missing transverse energy(mainly due to the undetected neutrinos),  E missT  , defined as the modulus of the negative vec-tor sum of the transverse momenta of all reconstructed particles (charged or neutral) in theevent [27]. To improve the signal sensitivity, the events are separated into three mutually ex-clusive categories according to the jet multiplicity: 2  with  E missT  + 0 jets, 2  with  E missT  + 1 jet,and 2  with  E missT  + 2 jets. Events with more than 2 jets are not considered.Furthermore, the search strategy splits signal candidates into three final states denoted by:e + e − ,  µ + µ − , and e ± µ ∓ . The bulk of the signal arises through direct W decays to charged stableleptons of opposite charge, though the small contribution proceeding through an intermediate τ   lepton is implicitly included. The events are selected by triggers which require the presenceof one or two high-  p T  electrons or muons. The trigger efficiency for signal events is measuredto be above 95% in the  µ + µ −  final state, and above 98% in the e + e −  and e ± µ ∓  final states for aHiggs boson mass ∼ 130GeV. The trigger efficiencies increase with the Higgs boson mass.Two oppositely charged lepton candidates are required, with  p T  > 20GeV for the leading lep-ton (  p  ,maxT  ) and  p T  >  10GeV for the trailing lepton (  p  ,minT  ). To reduce the low-mass Z/ γ ∗  →  +  −  contribution, the requirement on the trailing lepton  p T  is raised to 15 GeV for the e + e − and  µ + µ −  final states. This tighter requirement also suppresses the W  +  jets background inthese final states. Only electrons (muons) with  | η |  < 2.5 (2.4) are considered in the analysis.Muon candidates [28] are identified using a selection similar to that described in [17], while electron candidates are selected using a multivariate approach, which exploits correlations be-tween the selection variables described in [29] to improve identification performance. Thelepton candidates are required to srcinate from the primary vertex of the event, which is cho-sen as the vertex with highest  ∑   p 2T , where the sum is performed on the tracks associated tothe vertex, including the tracks associated to the leptons. This criterion provides the correctassignment for the primary vertex in more than 99% of both signal and background events forthe pile-up distribution observed in the data. Isolation is used to distinguish lepton candidatesfrom W-boson decays from those stemming from QCD background processes, which are usu-ally immersed in hadronic activity. For each lepton candidate, a  ∆ R  ≡   ( ∆ η ) 2 + ( ∆ φ ) 2 coneof 0.3 (0.4) for muons (electrons) is constructed around the track direction at the event vertex.The scalar sum of the transverse energy of each particle reconstructed using a particle-flow al-gorithm [27] compatible with the primary vertex and contained within the cone is calculated,excluding the contribution from the lepton candidate itself. If this sum exceeds approximately10% of the candidate  p T  the lepton is rejected, the exact requirement depending on the lepton η ,  p T  and flavour. Jets are reconstructed from calorimeter and tracker information using the particle-flow tech-nique [27, 30], combining the information from all CMS subdetectors to reconstruct each indi-  3 vidual particle. The anti-k T  clustering algorithm [31] with distance parameter R  =  0.5 is used,as implemented in the  FASTJET  package [32, 33]. To correct for the contribution to the jet en-ergy due to the pile-up, a median energy density (  ρ ) is determined event by event. Then thepile-up contribution to the jet energy is estimated as the product of   ρ  and the area of the jet andsubsequently subtracted [34] from the jet transverse energy  E T . Jet energy corrections are alsoapplied as a function of the jet  E T  and  η  [35]. Jets are required to have  E T  > 30GeV and | η | < 5to contribute to the event classification according to the jet multiplicityIn addition to high momentum isolated leptons and minimal jet activity, missing energy ispresent in signal events but not in background. In this analysis, a  projected E missT  variable, de-fined as the component of   E missT  transverse to the nearest lepton if that lepton is within  π  /2 inazimuthalangle, orthefull  E missT  otherwise, isemployed. Acutonthisobservableefficientlyre- jects Z/ γ ∗  →  τ  + τ  −  background events, where the  E missT  is preferentially aligned with leptons,as well as Z/ γ ∗  →   +  −  events with mismeasured  E missT  associated with poorly reconstructedleptons or jets. The  E missT  reconstruction makes use of event reconstruction via the particle-flow technique [27]. Since the  projected E missT  resolution is degraded by pile-up, a minimum of two different observables is used: the first includes all reconstructed particles in the event [27],while the second uses only the charged particles associated with the primary vertex. For thesame cut value with the first observable, the Z/ γ ∗  →   +  −  background doubles when goingfrom 5 to 15 pile-up events, while it remains approximately constant with the second observ-able. The use of both observables exploits the presence of a correlation between them in signalevents with genuine  E missT  , and its absence otherwise, as in Drell-Yan events.Drell-Yanbackgroundproducessame-flavourleptonpairs(e + e −  and µ + µ − ): thus,theselectionrequirements designed to suppress this background are slightly different for same-flavour andopposite-flavour (e ± µ ∓ ) events. Same-flavour events must have  projected E missT  above about40GeV, with the exact requirement depending on the number of reconstructed primary ver-tices ( N  vtx ) according to the relation  projected E missT  >  ( 37  +  N  vtx /2 ) GeV. For opposite-flavourevents, the requirement is lowered to 20GeV with no dependence on the number of vertices.These requirements remove more than 99% of the Drell-Yan background. In addition, require-ments of a minimum dilepton transverse momentum (  p  T  ) of 45GeV for both types and a min-imum dilepton mass ( m  ) of 20 (12)GeV for same- (opposite-) flavour events are applied. Twoadditional selection criteria are applied only to the same-flavour events. First, the dileptonmass must be outside a 30GeV window centered on the Z mass, and second, to suppress Drell-Yan events with the Z/ γ ∗  recoiling against a jet, the angle in the transverse plane between thedilepton system and the leading jet must be less than 165 degrees, when the leading jet has E T  > 15GeV.To suppress the top-quark background, a  top tagging  technique based on soft-muon and b- jets tagging methods [36, 37] is applied. The first method is designed to veto events containingmuons from b-quarks coming from the top-quark decay. The second method uses b-jet tagging,which looks for tracks with large impact parameter within jets. The algorithm is also appliedin the case of 0-jet bin, which can still contain jets with  E T  <  30GeV. The rejection factor fortop-quark background is about two in the 0-jet category and above 10 for events with at leastone jet passing the selection criteria.To reduce the background from WZ and ZZ production, any event that has a third leptonpassing the identification and isolation requirements is rejected. This requirement rejects lessthan 0.1% of the H  →  W + W −  →  2  2 ν  events, while it rejects 60% of WZ and 10% of the ZZprocesses. After the  E missT  requirement ZZ events are dominated by the ZZ  →  2  2 ν  process,where there is no 3rd lepton. The W γ  production, where the photon is misidentified as an
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