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000292119 005__ 20211110132738.0
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000292119 088__ $$2arXiv$$aKSU-HEP-110113
000292119 088__ $$2arXiv$$aarXiv:1311.0283
000292119 1001_ $$0P:(DE-H253)PIP1017558$$aKidonakis, Nikolaos$$b0$$eCorresponding author
000292119 1112_ $$aHelmholtz International School on Physics of Heavy Quarks and Hadrons$$cDubna$$d2013-07-15 - 2013-07-28$$gHQ2013$$wRussia
000292119 245__ $$aTop Quark Production
000292119 260__ $$aHamburg$$bDeutsches Elektronen-Synchrotron, DESY$$c2014
000292119 300__ $$a139-168
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000292119 520__ $$aI discuss top quark production in hadronic collisions. I present thesoft-gluon resummation formalism and its derivation from factorizationand renormalization-group evolution, and two-loop calculations ofsoft anomalous dimensions in the eikonal approximation. I discussthe contributions of next-to-next-to-leading order (NNLO) soft-gluoncorrections to the total cross sections and top-quark transverse momentumand rapidity distributions for top-antitop pair production, and forsingle-top production in the $t$ and $s$ channels and in associationwith a $W$ boson or a charged Higgs boson.T = Top Quark Production
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000292119 650_7 $$2INSPIRE$$atop: production
000292119 650_7 $$2INSPIRE$$atop: transverse momentum
000292119 650_7 $$2INSPIRE$$aapproximation: eikonal
000292119 650_7 $$2INSPIRE$$aHiggs particle: charged particle
000292119 650_7 $$2INSPIRE$$ahadron hadron: interaction
000292119 650_7 $$2INSPIRE$$ahigher-order: 2
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000292119 650_7 $$2INSPIRE$$aanomalous dimension
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000292119 650_7 $$2INSPIRE$$apair production
000292119 650_7 $$2INSPIRE$$afactorization
000292119 650_7 $$2INSPIRE$$aresummation
000292119 650_7 $$2INSPIRE$$arapidity
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000292119 773__ $$a10.3204/DESY-PROC-2013-03/Kidonakis
000292119 7870_ $$0PUBDB-2015-05817$$aAli, Ahmed et.al.$$dDeutsches Elektronen-Synchrotron, DESY, Hamburg, 2014$$iIsPartOf$$rDESY-PROC-2013-03$$tProceedings, Helmholtz International School on Physics of Heavy Quarks and Hadrons (HQ2013)
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