PERTURBATIVE RESUMMED SERIES FOR TOP-QUARK PRODUCTION IN HADRON REACTIONS

Citation
El. Berger et H. Contopanagos, PERTURBATIVE RESUMMED SERIES FOR TOP-QUARK PRODUCTION IN HADRON REACTIONS, Physical review. D. Particles and fields, 54(5), 1996, pp. 3085-3113
Citations number
36
Categorie Soggetti
Physics, Particles & Fields
ISSN journal
05562821
Volume
54
Issue
5
Year of publication
1996
Pages
3085 - 3113
Database
ISI
SICI code
0556-2821(1996)54:5<3085:PRSFTP>2.0.ZU;2-F
Abstract
Our calculation of the total cross section for inclusive production of <t(t)over bar> pairs in hadron collisions is presented. The principal ingredient of the calculation is resummation of the universal leading -logarithm effects of gluon radiation to all orders in the quantum chr omodynamics coupling strength, restricted to the region of phase space that is demonstrably perturbative. We derive the perturbative regime of the resummed series, starting from the principal-value resummation approach, and we isolate the perturbative domain in both moment space and, upon inversion of the corresponding Mellin transform, in momentum space. We show that our perturbative result does not depend on the ma nner nonperturbative or infrared effects are handled in principal-valu e resummation. We treat both the quark-antiquark and gluon-gluon produ ction channels consistently in the <(MS)over bar> factorization scheme . We compare our method and results with other resummation methods tha t rely on the choice of infrared cutoffs. We derive the renormalizatio n or factorization scale dependence of our resummed cross section, and we discuss factorization scheme dependence and remaining theoretical uncertainties, including estimates of possible nonperturbative contrib utions. We include the full content of the exact next-to-leading order calculation in obtaining our final results. We present predictions of the physical cross section as a function of top quark mass in proton- antiproton reactions at center-of-mass energies of 1.8 and 2.0 TeV. We also provide the differential cross section as a function of the part on-parton subenergy.