Combination of Tevatron Searches for the Standard Model Higgs Boson in theW+W−Decay Mode (original) (raw)

Search for New Physics in High p_{T} Like-Sign Dilepton Events at CDF II

Physical Review Letters, 2011

We present a search for new physics in events with two high p T leptons of the same electric charge, using data with an integrated luminosity of 6:1 fb À1. The observed data are consistent with standard model predictions. We set 95% C.L. lower limits on the mass of doubly charged scalars decaying to likesign dileptons, m H AEAE > 190-245 GeV=c 2 , assuming 100% BR to ee, or e.

Combined Tevatron upper limit ongg→H→W+W−and constraints on the Higgs boson mass in fourth-generation fermion models

Physical Review D, 2010

We combine results from searches by the CDF and D0 collaborations for a standard model Higgs boson (H) in the process gg ! H ! W þ W À in p " p collisions at the Fermilab Tevatron Collider at ffiffi ffi s p ¼ 1:96 TeV. With 4:8 fb À1 of integrated luminosity analyzed at CDF and 5:4 fb À1 at D0, the 95% confidence level upper limit on ðgg ! HÞ Â BðH ! W þ W À Þ is 1.75 pb at m H ¼ 120 GeV, 0.38 pb at m H ¼ 165 GeV, and 0.83 pb at m H ¼ 200 GeV. Assuming the presence of a fourth sequential generation of fermions with large masses, we exclude at the 95% confidence level a standard-modellike Higgs boson with a mass between 131 and 204 GeV.

Search for the Standard Model Higgs Boson in ZH→ℓ^{+}ℓ^{-}bb[over ¯] Production with the D0 Detector in 9.7 fb^{-1} of pp[over ¯] Collisions at sqrt[s]=1.96 TeV

Physical Review Letters, 2012

We present a search for the standard model (SM) Higgs boson produced in association with a Z boson in 9:7 fb À1 of p " p collisions collected with the D0 detector at the Fermilab Tevatron Collider at ffiffi ffi s p ¼ 1:96 TeV. Selected events contain one reconstructed Z ! e þ e À or Z ! þ À candidate and at least two jets, including at least one jet identified as likely to contain a b quark. To validate the search procedure, we also measure the cross section for ZZ production in the same final state. It is found to be consistent with its SM prediction. We set upper limits on the ZH production cross section times branching ratio for H ! b " b at the 95% C.L. for Higgs boson masses 90 M H 150 GeV. The observed (expected) limit for M H ¼ 125 GeV is 7.1 (5.1) times the SM cross section.

Search for Associated W and Higgs Boson Production in pp¯ Collisions at s=1.96 TeV

Physical Review Letters, 2009

We present results of a search for WH ! 'b " b production in p " p collisions based on the analysis of 1:05 fb À1 of data collected by the D0 experiment at the Fermilab Tevatron, using a neural network for separating the signal from backgrounds. No signal-like excess is observed, and we set 95% C.L. upper limits on the WH production cross section multiplied by the branching ratio for H ! b " b for Higgs boson masses between 100 and 150 GeV. For a mass of 115 GeV, we obtain an observed (expected) limit of 1.5 (1.4) pb, a factor of 11.4 (10.7) times larger than the standard model prediction.

Evidence for a Particle Produced in Association with Weak Bosons and Decaying to a Bottom-Antibottom Quark Pair in Higgs Boson Searches at the Tevatron

Physical Review Letters, 2012

We combine searches by the CDF and D0 Collaborations for the associated production of a Higgs boson with a W or Z boson and subsequent decay of the Higgs boson to a bottom-antibottom quark pair. The data, originating from Fermilab Tevatron pp collisions at √ s = 1.96 TeV, correspond to integrated luminosities of up to 9.7 fb −1. The searches are conducted for a Higgs boson with mass in the range 100-150 GeV/c 2. We observe an excess of events in the data compared with the background predictions, which is most significant in the mass range between 120 and 135 GeV/c 2. The largest local significance is 3.3 standard deviations, corresponding to a global significance of 3.1 standard deviations. We interpret this as evidence for the presence of a new particle consistent with the standard model Higgs boson, which is produced in association with a weak vector boson and decays to a bottom-antibottom quark pair.