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005     20211110132738.0
024 7 _ |a arXiv:1311.0283
|2 arXiv
024 7 _ |a 10.3204/DESY-PROC-2013-03/Kidonakis
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037 _ _ |a PUBDB-2015-05832
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088 1 _ |a KSU-HEP-110113; arXiv:1311.0283
088 _ _ |a KSU-HEP-110113
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088 _ _ |a arXiv:1311.0283
|2 arXiv
100 1 _ |a Kidonakis, Nikolaos
|0 P:(DE-H253)PIP1017558
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|e Corresponding author
111 2 _ |a Helmholtz International School on Physics of Heavy Quarks and Hadrons
|g HQ2013
|c Dubna
|d 2013-07-15 - 2013-07-28
|w Russia
245 _ _ |a Top Quark Production
260 _ _ |c 2014
|b Deutsches Elektronen-Synchrotron, DESY
|a Hamburg
300 _ _ |a 139-168
336 7 _ |a Conference Paper
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336 7 _ |a INPROCEEDINGS
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520 _ _ |a I 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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650 _ 7 |a top: production
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650 _ 7 |a top: transverse momentum
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650 _ 7 |a approximation: eikonal
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650 _ 7 |a Higgs particle: charged particle
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650 _ 7 |a hadron hadron: interaction
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650 _ 7 |a higher-order: 2
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650 _ 7 |a renormalization group
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650 _ 7 |a anomalous dimension
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650 _ 7 |a total cross section
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650 _ 7 |a pair production
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650 _ 7 |a factorization
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650 _ 7 |a resummation
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650 _ 7 |a rapidity
|2 INSPIRE
693 _ _ |a HERA
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773 _ _ |a 10.3204/DESY-PROC-2013-03/Kidonakis
787 0 _ |a Ali, Ahmed et.al.
|d Deutsches Elektronen-Synchrotron, DESY, Hamburg, 2014
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|t Proceedings, Helmholtz International School on Physics of Heavy Quarks and Hadrons (HQ2013)
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