2009
DOI: 10.1016/j.cpc.2009.03.006
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Vbfnlo: A parton level Monte Carlo for processes with electroweak bosons

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Cited by 369 publications
(294 citation statements)
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“…We can study the approach to the decoupling limit by writing α − β ¼ δ − π=2 and consider the parameter dependence of R BDRS . Assuming we are close to the decoupling limit and expanding to first order in δ we find that with the gluon-initiated process omitted μb b ðqq → hZÞ ≈ 1 − δð0.2 cot β þ 0.7 tan βÞ; (16) whereas with the gluon-initiated process included μb b ðqq; gg → hZÞ ≈ 1 − δð0.6 cot β þ 0.7 tan βÞ; (17) and the dependence on deviations from the decoupling limit is much stronger at low tan β. This is not surprising as the gluon-initiated associated production introduces strong dependence of the cross section on the Higgs-top quark coupling, which in this limit is given by c t ≈ 1 þ δ cot β.…”
Section: B Boosted Associated Productionmentioning
confidence: 93%
“…We can study the approach to the decoupling limit by writing α − β ¼ δ − π=2 and consider the parameter dependence of R BDRS . Assuming we are close to the decoupling limit and expanding to first order in δ we find that with the gluon-initiated process omitted μb b ðqq → hZÞ ≈ 1 − δð0.2 cot β þ 0.7 tan βÞ; (16) whereas with the gluon-initiated process included μb b ðqq; gg → hZÞ ≈ 1 − δð0.6 cot β þ 0.7 tan βÞ; (17) and the dependence on deviations from the decoupling limit is much stronger at low tan β. This is not surprising as the gluon-initiated associated production introduces strong dependence of the cross section on the Higgs-top quark coupling, which in this limit is given by c t ≈ 1 þ δ cot β.…”
Section: B Boosted Associated Productionmentioning
confidence: 93%
“…We have implemented this calculation in the VBFNLO code [92] in which we have provided the tensor structure depicted in figure 3 which has been calculated with MadGraph [101]. Up to now the VBFNLO implementation only involves on-shell Higgs pairs.…”
Section: The Vector Boson Fusion Processmentioning
confidence: 99%
“…In the next section, we discuss the QCD radiative corrections to double Higgs production in the gluon fusion, vector boson fusion and Higgs-strahlung processes (the ttHH process will be only considered at tree-level) and how they are implemented in the programs HPAIR [91], VBFNLO [92] and a code developed by us to evaluate the inclusive cross sections in Higgs-strahlung processes. In section 3, we evaluate the various theoretical uncertainties affecting these cross sections and collect at M H = 125 GeV the double Higgs production cross sections at the various LHC energies.…”
Section: Jhep04(2013)151mentioning
confidence: 99%
“…Then we use the VBFNLO code [35][36][37] to perform the phase space integration, where we set the parton distribution functions (PDFs) as CTEQ6L1 [38].…”
Section: The MC Simulationmentioning
confidence: 99%