J an 2 01 2 Standard Model Higgs Boson Combination at the Tevatron

We present the recent results from combinations of searches for a standard model (SM) Higgs boson (H) by the CDF and D0 experiments at the Tevatron pp̄ collider at √ s = 1.96 TeV. The data correspond to an integrated total luminosity of 8.2 (CDF) and 8.6 (D0) fb −1. Compared to the previous Tevatron Higgs boson search combination more data have been added, additional channels have been added, and some previously used channels have been reanalyzed to gain sensitivity. No excess is observed above background expectation, and set 95% C.L. upper limits (median expected) on Higgs boson production at factors of 1.17 (1.16), 1.71 (1.16), and 0.48(0.57) times the SM predictions for Higgs bosons of mass mH=115, 140, and 165 GeV /c2, respectively. We exclude a standard-model Higgs boson in the mass range 156–177 GeV /c2 at the 95% C.L, with an expected exclusion region 148–180 GeV /c2. The absence of a Higgs boson signal also constrains some new physics such as 4th generation models and other exotic models.


els and other
exotic models.

Introduction

The Higgs boson is the last unobserved particle postulated in SM to help explain the origin of mass.The global fit from the electroweak precision data indicates that the Higgs boson mass is lighter than 158 GeV/c 2 at 95% confidence level [1].The direct searches from LEP [2], the Tevatron [3] and LHC [4] further limit the Higgs boson mass between 114.4 and 141 GeV/c 2 .Recently, using 5 fb −1 of integrated luminosity collected in 2011 for each experiment, the AT-LAS and CMS collaborations [5] have reported excesses in the Higgs search channels (γγ, ZZ * → 4l, and WW * → 2l) with reconstructed invariant mass near 125 GeV/c 2 .The combined statistical significance is about 2.0 σ including the look elsewhere effect, but nevertheless, this is interesting and requiring more data to confirm r reject the hypothesis.

With full dataset and improved analyses, The Tevatron will be still competitive and will provide an unique sensitivity to H → b b in the remaining mass range.In this note, we present the recent results from the combination of multiple direct searches for the SM Higgs boson at the Tevatron [3].The analyses that are combined seek signals of Higgs bosons produced in association with vector bosons (q q → W/ZH), through gluon-gluon fusion (gg → H), and through vector boson fusion (VBF) (q q → q ′ q′ H) corresponding to integrated luminosities up to 8.2 fb −1

CDF and 8.6 fb −1 at D0.


Hi
gs Boson Search Strategies

The dominant Higgs boson production processes at the Tevatron are gluon-gluon fusion, and associated production with a W or Z boson.For a mass below 135 GeV/c 2 , the Higgs boson decays predominantly into b b, which makes the associated production most assessible while the direct production of gg → H → b b is limited by multi-jet QCD a e-mail: wmyao@lbl.govbackground.For a mass above 135 GeV/c 2 , the Higgs boson will decay predominately into WW * and ZZ, making the gg → H production most useful.However, the best sensitivity requires combining all production and decay channels together, includ ng both CDF and D0 data.

The search strategies for the Higgs boson are quite similar for the corresponding CDF and D0 analyses.For low mass signatures we look for a b b mass resonance in associated with W/Z events where W/Z decays leptonically.We apply b-tagging and advanced multivariate analysis (MVA) technique to suppress large W/Z +jets and top background.For high mass signatures we look for the Higgs boson decaying into WW pair in the inclusive Higgs boson events that lead to many interesting final states.The most sensitive channel is both W decaying leptonically that gives a final state of opposite-sign dilepton, large missing Et, and some jets.Due to missing neutrinos, we have to rely on the event kinematic distributions that distinguish the signal from the background using MVA techniques.There are in total 165 mutually exclusive final states, 94 channels from D0 and 7 channels from CDF.

All analyses provide binned histograms of the final discriminant for data, signal, and each individual background.More details for the low and high-mass SM Higgs boson searches can be found n these talks [6].

We use the most recent high-order calculations of the SM Higgs boson production cross section and decay branching ratio to normalize the signal event yield in each individual channel.So we can combine t

m statistically.


Comb
nation Procedures

To gain confidence that the final result does not depend on the details of statistical method, we perform two types of combinations, using Bayesian and modified Frequentist approaches, which yield results that agree within 10%.We quote only the limits obtained with the Bayesian method, which is decided upon a priori.Both methods rely on distributions of final discriminants, not just on event counts.Systematic uncertainties are treated as nuisance parameters with truncated Gaussian.Both methods use likelihood calculations based on Poisson probabilities.There are two types of systematic uncertainties that affect the rate and shape of estimated signal and background in a correlated way.The rate systematic only affects overall normalization while the shape systematic is changing differential distribution due to the jet energy scale(JES) and Monte Carlo(M ) modeling.


EPJ Web of Conferences

CDF and D0 share common systematic uncertainties on luminosity, the theoretical cross sections, and some scale and PDF veriations, which are treated as correlated.Other sources of systematic are experiment dependent, treated uncorrelated between experiments, but correlated within the experiment, such as lepton identification, b-tagging efficiency, JES, detector e fects and instrumental backgrounds.

In order to check the consistency between data and expectations, we rebin the final discriminant from each channel in terms of signal to background ratio (s/b), data with similar s/b may be

dded without loss in sensitivity.


Combined Tevat
on Searches for the SM Higgs Boson

Before extracting the combined results, we check the search sensitivity using log-likelihood ratio(LLR) for different hypotheses to quantify the expected sensitivity across the mass range tested.Figure 4 shows the combined distributions of the log-likelihood ratio as a function of Higgs boson mass.The black dot curve is for the background-only hypothesis, the red dot curve is for the signal-plus-background hypothesis, and the solid curve is for the observed data.The sizes of one and two sigma bands indicate the width of the LLR background-only distribution.The separation between the background-only and signal-plus-background hypotheses provides a measure of the search sensitivity, which is about two sigma at low mass and close to 3 sigma at m H = 165 GeV/c 2 .

Figure 5 shows the ratio of the 95% C.L. expected and observed limit to the SM Higgs boson cross section times branching ratio at the Tevatron after combining CDF and D0 searches together [3].The observed and median expected ratios are listed in Table 1 for m H ≤ 150 GeV/c 2 , and in Table 2 for m H ≥ 155 GeV/c 2 , as obtained by the Bayesian and the CL s methods.We obtain the observed limit of 1.17 with expected 1.16 for m H = 115 GeV/c 2 and 0.48 with expecte 0.57 for m H = 165 GeV/c 2 .

We investigate the sensitivity and observed limits using CDF's and D0's searches for H → b b taken in combination.These channels contribute the most for values of m H below 135 geV/c 2 and will remain competitive with the LHC experiments.The result of this combina

on is shown in Figure 6.


Constraints on Fourth-Generati
n and other Exotic Models

With the absence of a H → WW signal, we can use it to set constraints on 4th generation and other exotic models [7] [8].For example, in a 4th generation model, the Higgs boson production cross section of gg → H could be enhanced by a factor of 9 due to additional 2 heavy quarks contributions in the loop.Reinterpreting H → WW limit in the 4th generation model, as shown in Figure 7 as a function of the Higgs boson mass, we are able to exclude the Higgs boson mass between 124 and 286 GeV/c 2 at 95% CL, Further combining H → γγ, WW limit in a fermiphobic model, as shown in Figure 8 as a function of the Higgs boson mass, we are able to exclude the Higgs boson mass abov

119 GeV/c 2 at 95% CL.


Conclus
on and Future Prospects

We have presented the recent combinations of searches for a standard model (SM) Higgs boson (H) by the CDF EPJ Web of Conferences and D0 experiments at the Tevatron p p collider at √ s = 1.96TeV.With up to 8.2 fb −1 of data analyzed at CDF and up to 8.6 fb −1 at D0, the 95% C.L. upper limits (median expected) on Higgs boson production are factors of 1.17 (1.16), 1.71 (1.16), a d 0.48(0.57)times the SM predictions for Higgs bosons of mass m H =115, 140, and 165 GeV/c 2 , respectively.We exclude a standard-model Higgs boson in the mass range 156-177 GeV/c 2 at the 95% C.L, with an expected exclusion region 148-180 GeV.c 2 .The absence of Higgs boson signal also constrains some new physics such as 4 th generation models and other exotic models as well.

The Tevatron has ended on 9/30/2011 for the last time after 28 years With 10 fb-1 analyzable dataset and anticipated improvement