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Search for VH prodiuction in the ET b je

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Nội dung chi tiết: Search for VH prodiuction in the ET b je

Search for VH prodiuction in the ET b je

Search for VH prodiuction ill the j£r+ờ-jets signature ill the full CDF datasetK. PotamianosỊ D. Bortoletto, Q. Liu (Purdue) o. Gonzáỉez (CIEMAT)F. Ma

Search for VH prodiuction in the ET b je argaroli (Rome La Sapienza)K. Knoepfel, B. Kilminster, M. Kirby (FNAL)H. Wolfe (OSU)February 27. 2012AbstractWe present a search for a low-mass SM Hig

gs boson produced ill association with a vector boson (VH) where II decays to hb and the vector boson decays escape detection. We are sensitive to ZH Search for VH prodiuction in the ET b je

-* t'vbb. WH -* tt'bb (with the lepton not identified), and to a much lesser extent to Zfi -> ftfyb.lilts search is an update of the search using 7.8

Search for VH prodiuction in the ET b je

fb 1 of CDF' data presented at EPS-HEP2011 with the full CDF' dataset, i.e. 9.45 fb 1. improvements include a new determination of the jet energy corr

Search for VH prodiuction ill the j£r+ờ-jets signature ill the full CDF datasetK. PotamianosỊ D. Bortoletto, Q. Liu (Purdue) o. Gonzáỉez (CIEMAT)F. Ma

Search for VH prodiuction in the ET b je rgy resolution.Observing no significant excess in the data, we set 95% confidence level upper limits on the VH production cn*®-sectk>n times branching

fraction to for values of the Higgs maw (mil) between 90 and 150 GcV/c2. F°f mK = 125 GcV/c2. we set an observed (expected) limit of 6.7 (3.6) times Search for VH prodiuction in the ET b je

the SM prediction.We re-interpret this result in a search for wz + zz production, with 7. u>, and measure a cross-section compatible with SM predictio

Search for VH prodiuction in the ET b je

n.1IntroductionThis note describes the updates to the search for the SM Higgs boson in the /Cr+h-jets signature using 7.8 ill 1 described in [1]. Addi

Search for VH prodiuction ill the j£r+ờ-jets signature ill the full CDF datasetK. PotamianosỊ D. Bortoletto, Q. Liu (Purdue) o. Gonzáỉez (CIEMAT)F. Ma

Search for VH prodiuction in the ET b je the jet energy corrections applied to gluon jets, an jVjV designed to improve the jet energy resolution, as well as an expanded good run list.2Jet en

ergy resolutionThe previous version of the Br+bb analysis used a jet-energy algorithm where the calorimeter energies were adjusted according to the en Search for VH prodiuction in the ET b je

ergy inferred from tracks within the jet cone (Hl algorithm). Although such a method improved the jet energy resolution by accounting for* karolosOfna

Search for VH prodiuction in the ET b je

l.nov1energy leakage, various assumptions were made that led to lesfri than optimal determination of the jet energy. To improve the energy determinati

Search for VH prodiuction ill the j£r+ờ-jets signature ill the full CDF datasetK. PotamianosỊ D. Bortoletto, Q. Liu (Purdue) o. Gonzáỉez (CIEMAT)F. Ma

Search for VH prodiuction in the ET b je twork NNjer are listed in Table 2. Each of the variables is well-validated in a dedicated control region. The neural network is trained using the two

most energetic jets from 7.Í! -» t't ữ>, Witand ZH -» ppw> signal eventsfor Higgs ma^es in the full low-mass Higgs range of 100 < mu < 150 GeV/c2 at 5 Search for VH prodiuction in the ET b je

GeV increments. To avoid correcting jet energies to an average characteristic energy, cadi training event receives a weight such that the cumulative

Search for VH prodiuction in the ET b je

jet Ef distribution is flat.A more detailed descript ion of the A’A'jem is presented in CDF10591.VariableDescriptionRaw Er L5 mr III E, Energy EM frac

Search for VH prodiuction ill the j£r+ờ-jets signature ill the full CDF datasetK. PotamianosỊ D. Bortoletto, Q. Liu (Purdue) o. Gonzáỉez (CIEMAT)F. Ma

Search for VH prodiuction in the ET b je et energy CES detector energies of 5T0 candidates within jet cone fraction of jet energy collected in EM calor imeter Jet pseudorapidity Maximum trans

verse momentum of track within jet cone Linear sum of transverse momenta of tracks within jet coneTable 1: Description of the NNjhr input variables.Fo Search for VH prodiuction in the ET b je

r this analysis, the NNjkh algorithm is implemented by correcting the Hl-determined Krlo an jX'Njkr determination. An analysis cut of £-;•( A’A’jeh) >

Search for VH prodiuction in the ET b je

35 GeV is applied to reduce multijet Iwkgioimd, the dominant background Contribution in this analysis. As seen in Fig. 1. the NNtHH algorithm separat

Search for VH prodiuction ill the j£r+ờ-jets signature ill the full CDF datasetK. PotamianosỊ D. Bortoletto, Q. Liu (Purdue) o. Gonzáỉez (CIEMAT)F. Ma

Search for VH prodiuction in the ET b je T I/Ĩ>tó events in the preselection region. The

dashed vertical line at 35 GeV represents the additional analysis cut made after ntupling.The next iteration of thi» analysis trill implement the NNjb Search for VH prodiuction in the ET b je

r algorithm by correcting the.2

Search for VH prodiuction ill the j£r+ờ-jets signature ill the full CDF datasetK. PotamianosỊ D. Bortoletto, Q. Liu (Purdue) o. Gonzáỉez (CIEMAT)F. Ma

Search for VH prodiuction ill the j£r+ờ-jets signature ill the full CDF datasetK. PotamianosỊ D. Bortoletto, Q. Liu (Purdue) o. Gonzáỉez (CIEMAT)F. Ma

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