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      Report of the Higgs Working Group of the Tevatron Run 2 SUSY/Higgs Workshop

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          Abstract

          This report presents the theoretical analysis relevant for Higgs physics at the upgraded Tevatron collider and documents the Higgs Working Group simulations to estimate the discovery reach in Run 2 for the Standard Model and MSSM Higgs bosons. Based on a simple detector simulation, we have determined the integrated luminosity necessary to discover the SM Higgs in the mass range 100-190 GeV. The first phase of the Run 2 Higgs search, with a total integrated luminosity of 2 fb-1 per detector, will provide a 95% CL exclusion sensitivity comparable to that expected at the end of the LEP2 run. With 10 fb-1 per detector, this exclusion will extend up to Higgs masses of 180 GeV, and a tantalizing 3 sigma effect will be visible if the Higgs mass lies below 125 GeV. With 25 fb-1 of integrated luminosity per detector, evidence for SM Higgs production at the 3 sigma level is possible for Higgs masses up to 180 GeV. However, the discovery reach is much less impressive for achieving a 5 sigma Higgs boson signal. Even with 30 fb-1 per detector, only Higgs bosons with masses up to about 130 GeV can be detected with 5 sigma significance. These results can also be re-interpreted in the MSSM framework and yield the required luminosities to discover at least one Higgs boson of the MSSM Higgs sector. With 5-10 fb-1 of data per detector, it will be possible to exclude at 95% CL nearly the entire MSSM Higgs parameter space, whereas 20-30 fb-1 is required to obtain a 5 sigma Higgs discovery over a significant portion of the parameter space. Moreover, in one interesting region of the MSSM parameter space (at large tan(beta)), the associated production of a Higgs boson and a b b-bar pair is significantly enhanced and provides potential for discovering a non-SM-like Higgs boson in Run 2.

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          Higgs Bosons from Two-Gluon Annihilation in Proton-Proton Collisions

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            Updated Estimate of Running Quark Masses

            Stimulated by recent development of the calculation methods of the running quark masses \(m_q(\mu)\) and renewal of the input data, for the purpose of making a standard table of \(m_q(\mu)\) for convenience of particle physicists, the values of \(m_q(\mu)\) at various energy scales \(\mu\) (\(\mu = 1\) GeV, \(\mu = m_c\), \(\mu=m_b\), \(\mu=m_t\) and so on), especially at \(\mu = m_Z\), are systematically evaluated by using the mass renormalization equations and by taking into consideration a matching condition at the quark threshold.
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              Associated Production of Higgs and Weak Bosons, with H -> b\bar b, at Hadron Colliders

              We consider the search for the Higgs boson at a high-luminosity Fermilab Tevatron, an upgraded Tevatron of energy 3.5 TeV, and the CERN Large Hadron Collider, via \(WH/ZH\) production followed by H -> bb~ and leptonic decay of the weak vector bosons. We show that each of these colliders can potentially observe the standard Higgs boson in the intermediate-mass range, 80 GeV \gamma\gamma at the LHC. In addition, it can potentially be used to observe the lightest Higgs scalar of the minimal supersymmetric model in a region of parameter space not accessible to CERN LEP II or the LHC (using h -> \gamma\gamma,ZZ^*).
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                Author and article information

                Journal
                31 October 2000
                2000-12-06
                Article
                hep-ph/0010338
                b45c8a28-f605-4f35-afd6-7805680f717f
                History
                Custom metadata
                Fermilab-Conf-00/279-T and SCIPP-00/37
                185 pages, 124 figures, 55 tables
                hep-ph hep-ex

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