Weak corrections to four-parton processes
Weak corrections to four-parton processes
We report on a calculation of the ‘mixed’ strong and (purely) weak corrections through the order αS2αW to parton–parton processes in all possible channels at hadron colliders entering the single jet inclusive cross section. At both Tevatron and LHC, such effects are always negligible (below permille level) in the total integrated cross section whilst they become sizable in differential rates. Specifically, if such corrections are defined with respect to the full leading-order result of [equ'n], we find that, at the FNAL accelerator, they can reach the -5% benchmark in the jet transverse energy (at the kinematical limit of the machine, rendering their detection quite difficult). At the CERN collider, in the same observable, they exceed the -10% level already at 1 TeV and can reach -40% at 4 TeV, kinematic regions where such corrections will be comfortably observable for standard luminosity. In addition, such corrections are somewhat sensitive to the factorisation/renormalisation scale choice.
hadron colliders, electroweak physics, higher-order calculations
50-82
Moretti, S.
b57cf0f0-4bc3-4e02-96e3-071255366614
Nolten, M.R.
4f2ad5b9-777d-4337-ab8c-0de1605b4ea2
Ross, D.A.
eb79bbfe-fb97-4bb3-813c-98f278e5a55f
18 December 2006
Moretti, S.
b57cf0f0-4bc3-4e02-96e3-071255366614
Nolten, M.R.
4f2ad5b9-777d-4337-ab8c-0de1605b4ea2
Ross, D.A.
eb79bbfe-fb97-4bb3-813c-98f278e5a55f
Moretti, S., Nolten, M.R. and Ross, D.A.
(2006)
Weak corrections to four-parton processes.
Nuclear Physics B - Proceedings Supplements, 759 (1-2), .
(doi:10.1016/j.nuclphysb.2006.09.028).
Abstract
We report on a calculation of the ‘mixed’ strong and (purely) weak corrections through the order αS2αW to parton–parton processes in all possible channels at hadron colliders entering the single jet inclusive cross section. At both Tevatron and LHC, such effects are always negligible (below permille level) in the total integrated cross section whilst they become sizable in differential rates. Specifically, if such corrections are defined with respect to the full leading-order result of [equ'n], we find that, at the FNAL accelerator, they can reach the -5% benchmark in the jet transverse energy (at the kinematical limit of the machine, rendering their detection quite difficult). At the CERN collider, in the same observable, they exceed the -10% level already at 1 TeV and can reach -40% at 4 TeV, kinematic regions where such corrections will be comfortably observable for standard luminosity. In addition, such corrections are somewhat sensitive to the factorisation/renormalisation scale choice.
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Published date: 18 December 2006
Keywords:
hadron colliders, electroweak physics, higher-order calculations
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Local EPrints ID: 57486
URI: http://eprints.soton.ac.uk/id/eprint/57486
ISSN: 0920-5632
PURE UUID: c99bc80f-7cf3-43a6-b932-8f7e4eecb858
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Date deposited: 14 Aug 2008
Last modified: 16 Mar 2024 03:34
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Author:
M.R. Nolten
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