Combination of Tevatron searches for the standard model Higgs boson in the W+W- decay mode
By T. Aaltonen, V. Abazov, B. Abbott, M. Abolins, B. Acharya, M. Adams, T. Adams, J. Adelman, E. Aguiló, G. Alexeev and 490 more. 2010
155 citations recorded by the source corpus.
We combine searches by the CDF and D0 collaborations for a Higgs boson decaying to W+W-. The data correspond to an integrated total luminosity of 4.8 (CDF) and 5.4 (D0) fb-1 of p-pbar collisions at sqrt{s}=1.96 TeV at the Fermilab Tevatron collider. No excess is observed above background expectation, and resulting limits on Higgs boson production exclude a standard-model Higgs boson in the mass range 162-166 GeV at the 95% C.L.
Subfields: Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/0d28b0d0785a46e904466751e5124425706a8a63
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In Nuclear and High Energy Physics
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- F. Tackmann
- Iain W. Stewart
- C. Berger
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Citations in the corpus
- Factorization at the LHC: From PDFs to Initial State Jets (Ph.D. thesis) (2009, methodology): “me from Standard Model processes producing the same signature of hard objects possibly with additional jets. An example are top quarks decaying into W plus b-jet, which is a major background for H!WW [5]. When reconstructing masses and decay chains of new-physics particles additional jets can cause ”
- Higgs production with a central jet veto at NNLL+NNLO (2010, background): “It is the dominant channel in the current Tevatron exclusion limit [1].”
- Factorization at the LHC: From parton distribution functions to initial state jets (2010, methodology): “It should be emphasized that Tevatron Higgs searches, which exclude the range mH = 162−166 GeV at 95% confidence level [5–7], already analyse their data using a jet algorithm and Monte Carlo to implement a jet veto on jets with pT ≥ 15 GeV and |ηj | ≤ 2.”
- Dark Matter Candidates from Particle Physics and Methods of Detection (2010, background): “In addition, the Tevatron pp̄ collider, currently running, excludes the region 162 GeV < mh < 166 GeV (18).”