Electroweak and finite quark-mass effects on the Higgs boson transverse momentum distribution

We perform a detailed study of the various one-loop contributions leading to production of the standard model Higgs boson in association with a hard jet. This production mode contributes to the current Tevatron exclusion limit of the standard model Higgs with 160 GeV{<=}M{sub H}{<=}170 GeV, and will also be important for discovery and interpretation of new scalar bosons at the Large Hadron Collider (LHC). We include top- and bottom-quark initiated contributions, maintaining the exact dependence on the quark masses, and also study previously neglected W- and Z-boson mediated effects which shift the qg and qq production modes. We consider the deviations from commonly used approximations for the Higgs boson transverse momentum spectrum caused by the finite top-quark mass, bottom-quark contributions, and electroweak gauge boson terms. All three effects act to decrease the Higgs boson transverse momentum distribution for observable momenta, with shifts reaching -8% at the Tevatron and -30% at the LHC. The shifts have a significant dependence on the Higgs p{sub T}, and are especially important if large momenta are selected by experimental cuts.

[1]  Dao Thi Nhung,et al.  D0C: A code to calculate scalar one-loop four-point integrals with complex masses , 2009, Comput. Phys. Commun..

[2]  Frank Petriello,et al.  Mixed QCD-electroweak corrections to Higgs boson production in gluon fusion , 2008, 0811.3458.

[3]  J. Zupan,et al.  Smoking guns for on-shell new physics at the LHC. , 2008, Physical review letters.

[4]  Li Lin Yang,et al.  Renormalization-group improved prediction for Higgs production at hadron colliders , 2008, 0809.4283.

[5]  M. Grazzini,et al.  NNLO predictions for the Higgs boson signal in the H → WW → lνlν and H → ZZ → 4l decay channels , 2008, 0801.3232.

[6]  M. Grazzini,et al.  HNNLO: a Monte Carlo program to compute Higgs boson production at hadron colliders , 2008 .

[7]  F. T. Collaboration,et al.  Combined CDF and Dzero Upper Limits on Standard Model Higgs-Boson Production , 2007, 0808.0534.

[8]  W. Quayle,et al.  Feasibility of Searches for a Higgs Boson using H ---> W+ W- ---> l+l- p(T) and High P(T) Jets at the Tevatron , 2007, 0708.2507.

[9]  Guenther Dissertori,et al.  NNLO QCD predictions for the H → WW → ℓνℓν signal at the LHC , 2007, 0707.2373.

[10]  R. S. Thorne,et al.  Parton distributions for the LHC , 2007, 0901.0002.

[11]  Oliver Brein,et al.  Distributions for MSSM Higgs boson+jet production at hadron colliders , 2007, 0705.2744.

[12]  M. Grazzini,et al.  Next-to-next-to-leading-order subtraction formalism in hadron collisions and its application to Higgs-boson production at the large hadron collider. , 2007, Physical review letters.

[13]  M. Dittmar,et al.  Combining Monte Carlo generators with next-to-next-to-leading order calculations: Event reweighting for Higgs boson production at the LHC , 2006, hep-ph/0604077.

[14]  J. Smith,et al.  An approximation for NLO single Higgs boson inclusive transverse momentum distributions in hadron-hadron collisions , 2005, hep-ph/0501098.

[15]  O. Brein,et al.  Minimal supersymmetric standard model Higgs bosons associated with high-pTjets at hadron colliders , 2003 .

[16]  E. Berger,et al.  Differential cross section for Higgs boson production including all-orders soft gluon resummation , 2002, hep-ph/0210135.

[17]  C. Schmidt,et al.  Next-to-leading corrections to the Higgs boson transverse momentum spectrum in gluon fusion , 2002, hep-ph/0209248.

[18]  Kirill Melnikov,et al.  Higgs Boson Production at Hadron Colliders in NNLO QCD , 2002, hep-ph/0207004.

[19]  Delphi collaboration,et al.  Search for the Standard Model Higgs Boson at LEP , 2001, hep-ex/0107029.

[20]  J. Vermaseren New features of FORM , 2000, math-ph/0010025.

[21]  D. N. Kovalenko,et al.  Higgs boson discovery potential of LHC in the channel pp→γγ+jet , 1998 .

[22]  Yuan,et al.  High-pT Higgs boson production at hadron colliders to O( alpha sGF3). , 1995, Physical review. D, Particles and fields.