Next-to-leading order QCD predictions for W+3-jet distributions at hadron colliders

We present next-to-leading order QCD predictions for a variety of distributions in W+3-jet production at both the Tevatron and the Large Hadron Collider. We include all subprocesses and incorporate the decay of the W boson into leptons. Our results are in excellent agreement with existing Tevatron d...

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Bibliographic Details
Main Authors: Berger, Carola (Contributor), Bern, Z. (Author), Dixon, L. J. (Author), Cordero, F. Febres (Author), Forde, D. (Author), Gleisberg, T. (Author), Ita, H. (Author), Kosower, D. A. (Author), Maître, D. (Author)
Other Authors: Massachusetts Institute of Technology. Center for Theoretical Physics (Contributor)
Format: Article
Language:English
Published: American Physical Society, 2010-03-18T12:28:17Z.
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Description
Summary:We present next-to-leading order QCD predictions for a variety of distributions in W+3-jet production at both the Tevatron and the Large Hadron Collider. We include all subprocesses and incorporate the decay of the W boson into leptons. Our results are in excellent agreement with existing Tevatron data and provide the first quantitatively precise next-to-leading order predictions for the LHC. We include all terms in an expansion in the number of colors, confirming that the specific leading-color approximation used in our previous study is accurate to within 3%. The dependence of the cross section on renormalization and factorization scales is reduced significantly with respect to a leading-order calculation. We study different dynamical scale choices, and find that the total transverse energy is significantly better than choices used in previous phenomenological studies. We compute the one-loop matrix elements using on-shell methods, as numerically implemented in the BlackHat code. The remaining parts of the calculation, including generation of the real-emission contributions and integration over phase space, are handled by the SHERPA package.
U.S. Department of Energy (Contract Nos. DE-FG03-91ER40662, DE-AC02- 76SF00515, and DE-FC02-94ER40818)