Transverse Momentum Distribution in Drell-Yan Pair and W and Z Boson Production
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TLDR
In this paper, the transverse momentum distribution of W bosons, Z bosons and high-mass virtual photons produced in high-energy hadron-hadron collisions is predicted.About:
This article is published in Nuclear Physics.The article was published on 1985-01-01 and is currently open access. It has received 1178 citations till now. The article focuses on the topics: Boson & Drell–Yan process.read more
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References
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Non-leading corrections to the Drell-Yan cross section at small transverse momentum
Christine Davies,W. J. Stirling +1 more
TL;DR: In this paper, the production of Drell-Yan lepton pairs at small transverse momentum is analyzed to second order in QCD perturbation theory, and the predictions of soft gluon cross sections in which these logarithms are summed to all orders are confirmed.
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Initial state interactions and the drell-yan process*
TL;DR: In this paper, it was shown that initial-state interactions violate the usual QCD factorization predictions for massive lepton-pair production in leading twist, and also smear the lepton pair transverse momentum distribution.
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QCD jets from coherent states
TL;DR: In this paper, the authors extended this approach to the problem of massless quark and gluon jets, and derived explicit expressions for the total KT distributions, taking into account transverse-momentum conservation.
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Lepton Pair Production at Large Transverse Momentum in Second Order QCD
TL;DR: In this article, the production of Drell-Yan pairs at large transverse momentum up to O(α s 2 ) was shown for a non-singlet combination defined as the cross section for an incident particle minus the analogous cross-sections of an incident antiparticle.
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Hard semi-inclusive processes in QCD
TL;DR: In this article, a new double logarithmic quark form factor is derived for massive lepton pair production in hadron collisions, leptoproduction of a particle from the current fragmentation region, and production of two particles from opposite jets in e+e− annihilation into hadrons.