Abstract

The transverse momentum QTQ_T distribution is computed for inclusive Higgs boson production at the energy of the CERN Large Hadron Collider. We focus on the dominant gluon-gluon subprocess in perturbative quantum chromodynamics and incorporate contributions from the quark-gluon and quark-antiquark channels. Using an impact-parameter bb-space formalism, we include all-orders resummation of large logarithms associated with emission of soft gluons. Our resummed results merge smoothly at large QTQ_T with the fixed-order expectations in perturbative quantum chromodynamics, as they should, with no need for a matching procedure. They show a high degree of stability with respect to variation of parameters associated with the non-perturbative input at low QTQ_T. We provide distributions dΟƒ/dydQTd\sigma/dy dQ_T for Higgs boson masses from MZM_Z to 200 GeV. The average transverse momentum at zero rapidity yy grows approximately linearly with mass of the Higgs boson over the range MZ<mh≃0.18mh+18M_Z < m_h \simeq 0.18 m_h + 18 ~GeV. We provide analogous results for ZZ boson production, for which we compute ≃25 \simeq 25 GeV. The harder transverse momentum distribution for the Higgs boson arises because there is more soft gluon radiation in Higgs boson production than in ZZ production.Comment: 42 pages, latex, 26 figures. All figures replaced. Some changes in wording. Published in Phys. Rev. D67, 034026 (2003

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