Abstract:We present a formalism for the calculation of multi-particle one-loop amplitudes, valid for an arbitrary number N of external legs, and for massive as well as massless particles. A new method for the tensor reduction is suggested which naturally isolates infrared divergences by construction. We prove that for N ≥ 5, higher dimensional integrals can be avoided. We derive many useful relations which allow for algebraic simplifications of one-loop amplitudes. We introduce a form factor representation of tensor in… Show more
Pair production of W bosons constitutes an important background to Higgs boson and new physics searches at the Large Hadron Collider LHC. We have calculated the loop-induced gluon-fusion process gg → W * W * → leptons, including intermediate light and heavy quarks and allowing for arbitrary invariant masses of the W bosons. While formally of next-to-next-to-leading order, the gg → W * W * → leptons process is enhanced by the large gluon flux at the LHC and by experimental Higgs search cuts, and increases the next-to-leading order W W background estimate for Higgs searches by about 30%. We have extended our previous calculation to include the contribution from the intermediate topbottom massive quark loop and the Higgs signal process. We provide updated results for cross sections and differential distributions and study the interference between the different gluon scattering contributions. We describe important analytical and numerical aspects of our calculation and present the public GG2WW event generator.
Pair production of W bosons constitutes an important background to Higgs boson and new physics searches at the Large Hadron Collider LHC. We have calculated the loop-induced gluon-fusion process gg → W * W * → leptons, including intermediate light and heavy quarks and allowing for arbitrary invariant masses of the W bosons. While formally of next-to-next-to-leading order, the gg → W * W * → leptons process is enhanced by the large gluon flux at the LHC and by experimental Higgs search cuts, and increases the next-to-leading order W W background estimate for Higgs searches by about 30%. We have extended our previous calculation to include the contribution from the intermediate topbottom massive quark loop and the Higgs signal process. We provide updated results for cross sections and differential distributions and study the interference between the different gluon scattering contributions. We describe important analytical and numerical aspects of our calculation and present the public GG2WW event generator.
“…To avoid the latter, we use integrals with Feynman parameters in the numerator as reduction endpoints. Explicit representations for all form factors for r ≤ N ≤ 5 can be found in [5]. The form factors are expressed in terms of the following basis integrals…”
Section: Reduction Formalismmentioning
confidence: 99%
“…IR divergencies are only present for N = 3 and d = 4 − 2ǫ. For the IR divergent integrals explicit analytical formulas can be found in [5]. The numerical evaluation of the remaining IR finite integrals is problematic due to kinematical singularities, which occur if the quadratic form x · S · x changes sign.…”
Section: Numerical Evaluation Of Basis Integralsmentioning
confidence: 99%
“…Due to its phenomenological relevance, a lot of activity has been going on in this direction during the last years [1,2,3,4,5,6,7,8,9,10,11,12].…”
Section: Introductionmentioning
confidence: 99%
“…In this talk, a method [5] for the evaluation of one-loop diagrams occurring in multi-particle computaions at NLO is presented. This approach allows for a good analytical control over the expressions, but also provides stable numerical representations in phase space regions which typically pose numerical problems.…”
A precise understanding of LHC phenomenology requires the inclusion of one-loop corrections for multi-particle final states. In this talk we describe a semi-numerical method to compute one-loop amplitudes with many external particles and present first applications.
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