Transverse-momentum resummation and the spectrum of the Higgs boson at the LHC

We consider the transverse-momentum (qT) distribution of generic high-mass systems (lepton pairs, vector bosons, Higgs particles,...) produced in hadron collisions. At small qT, we concentrate on the all-order resummation of the logarithmically-enhanced contributions in QCD perturbation theory. We e...

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Autor principal: Bozzi, G.
Otros Autores: Catani, S., de Florian, D., Grazzini, M.
Formato: Capítulo de libro
Lenguaje:Inglés
Publicado: 2006
Acceso en línea:Registro en Scopus
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100 1 |a Bozzi, G. 
245 1 0 |a Transverse-momentum resummation and the spectrum of the Higgs boson at the LHC 
260 |c 2006 
270 1 0 |m Grazzini, M.; INFN, Sezione di Firenze, Università di Firenze, I-50019 Sesto Fiorentino, Florence, Italy; email: massimiliano.grazzini@cern.ch 
506 |2 openaire  |e Política editorial 
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520 3 |a We consider the transverse-momentum (qT) distribution of generic high-mass systems (lepton pairs, vector bosons, Higgs particles,...) produced in hadron collisions. At small qT, we concentrate on the all-order resummation of the logarithmically-enhanced contributions in QCD perturbation theory. We elaborate on the b-space resummation formalism and introduce some novel features: the large logarithmic contributions are systematically exponentiated in a process-independent form and, after integration over qT, they are constrained by perturbative unitarity to give a vanishing contribution to the total cross section. At intermediate and large qT, resummation is consistently combined with fixed-order perturbative results, to obtain predictions with uniform theoretical accuracy over the entire range of transverse momenta. The formalism is applied to Standard Model Higgs boson production at LHC energies. We combine the most advanced perturbative information available at present for this process: resummation up to next-to-next-to-leading logarithmic accuracy and fixed-order perturbation theory up to next-to-leading order. The results show a high stability with respect to perturbative QCD uncertainties. © 2005 Elsevier B.V. All rights reserved.  |l eng 
536 |a Detalles de la financiación: Fundación Antorchas 
536 |a Detalles de la financiación: Ministry of Higher Education and Scientific Research 
536 |a Detalles de la financiación: The work of G.B. was supported by a postdoctoral fellowship of the French ministry for education and research. The work of D.dF. was supported in part by Fundación Antorchas, CONICET and UBACyT. D.dF. wishes to thank the INFN for support and hospitality during his visit at the Sezione di Firenze. Appendix A 
593 |a Laboratoire de Physique Subatomique et de Cosmologie, Université Joseph Fourier, CNRS-IN2P3, F-38026 Grenoble, France 
593 |a INFN, Sezione di Firenze, Università di Firenze, I-50019 Sesto Fiorentino, Florence, Italy 
593 |a Departamento de Física, FCEYN, Universidad de Buenos Aires, 1428 Pabellón 1, Buenos Aires, Argentina 
700 1 |a Catani, S. 
700 1 |a de Florian, D. 
700 1 |a Grazzini, M. 
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