2016
DOI: 10.1016/j.physletb.2016.10.040
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Higgs production in bottom-quark fusion: Matching beyond leading order

Abstract: We compute the total cross-section for Higgs boson production in bottom-quark fusion using the so-called FONLL method for the matching of a scheme in which the b-quark is treated as a massless parton to that in which it is treated as a massive final-state particle, and extend our previous results to the case in which the next-to-next-to-leading-log five-flavor scheme result is combined with the next-to-leading-order O(α 3 s ) four-flavor scheme computation.

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Cited by 67 publications
(99 citation statements)
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“…of phenomenological applications [33][34][35][36][37][38][39] and in studies on the rationale behind the choice of either scheme [42][43][44][45].…”
Section: Jhep04(2018)046mentioning
confidence: 99%
“…of phenomenological applications [33][34][35][36][37][38][39] and in studies on the rationale behind the choice of either scheme [42][43][44][45].…”
Section: Jhep04(2018)046mentioning
confidence: 99%
“…This has been done at NLO+NNLL accuracy using the FONLL [2,3,7,8] method and a method based on EFT [9,10], and both methods have been found to agree. Results obtained in the FONLL approach are shown in Fig.…”
Section: Resummation Vs Mass Effectsmentioning
confidence: 97%
“…In this study we reconsider these differences. Firstly we examine the origin of the difference at the inclusive level in the case of Higgs production in bottom-quark fusion [2,3]. Secondly we set-up the two schemes in such a way that they can be compared likes with likes in differential distributions [1].…”
Section: F or 5f Scheme?mentioning
confidence: 99%
See 1 more Smart Citation
“…The FONLL scheme, first proposed for the transverse momentum spectrum of bottom quarks produced in hadronic collisions [35], has the advantage of being universally applicable and of allowing one to combine 4FS and 5FS calculations performed at any perturbative order. The formulation of the FONLL scheme has been extended to deep-inelastic scattering (DIS) [36] and adapted to the computation of the total cross section for Higgs and Z production in bottom-quark fusion [37][38][39]. Various recent attempts to consistently include both the resummation of initial-state collinear logarithms and mass effects also for differential and parton-shower matched observables have been recently put forward, see for example the five-flavour-massive scheme proposed in [16,40] or a similar approach based on multi-jet merging [41].…”
Section: Introductionmentioning
confidence: 99%