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Release Note -- Vbfnlo-2.6.0

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arxiv 1207.4975 v1 pith:GBPUFXBK submitted 2012-07-20 hep-ph hep-ex

classification hep-phhep-ex
keywords gammabosonproductiondibosonvectorbeenfusionanomalous
verification ladder T0 review T1 audit T2 compute T3 formal
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Vbfnlo is a flexible parton level Monte Carlo program for the simulation of vector boson fusion (VBF), double and triple vector boson (plus jet) production in hadronic collisions at next-to-leading order (NLO) in the strong coupling constant, as well as Higgs boson plus two jet production via gluon fusion at the one-loop level. This note briefly describes the main additional features and processes that have been added in the new release -- Vbfnlo Version 2.6.0. At NLO QCD diboson production (W\gamma, WZ, ZZ, Z\gamma and \gamma\gamma), same-sign W pair production via vector boson fusion and the process W\gamma\gamma j have been implemented (for which one-loop tensor integrals up to six-point functions are included). In addition, gluon induced diboson production can be studied separately at the leading order (one-loop) level. The diboson processes WW, WZ and W\gamma can be run with anomalous gauge boson couplings, and anomalous couplings between a Higgs and a pair of gauge bosons is included in WW, ZZ, Z\gamma and \gamma\gamma diboson production. The code has also been extended to include anomalous gauge boson couplings for single vector boson production via VBF, and a spin-2 model has been implemented for diboson pair production via vector boson fusion.

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Cited by 2 Pith papers

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  1. Probing the Symmetric Higgs Portal with Di-Higgs Boson Production

    hep-ph 2019-08 conditional novelty 6.0 of 10

    Di-Higgs production at a future 100 TeV hadron collider can probe Higgs portal couplings of a stable scalar of order one for masses above half the Higgs mass.

  2. Effective field theory and scalar extensions of the top quark sector

    hep-ph 2019-08 accept novelty 6.0 of 10

    For a heavy scalar coupled to top quarks, only an NLO-matched effective field theory reproduces the full model across the LHC energy range, while a leading-order fit overestimates the high-mass tail and LHC constraints.

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