boson production in bottom-quark fusion: a study of -mass effects beyond leading order
arXiv:1803.10248 · doi:10.1140/epjc/s10052-018-6414-8
Abstract
We compute the total cross-section for boson production in bottom-quark fusion, applying to this case the method we previously used for Higgs production in bottom fusion. Namely, we match, through the FONLL procedure, the next-to-next-to-leading-log five-flavor scheme result, in which the ~quark is treated as a massless parton, with the next-to-leading-order $\order{α_s^3}$ four-flavor scheme computation in which bottom is treated as a massive final-state particle. Our computation provides a test-case for the discussion of issues of scale dependence and treatment of heavy quarks, which we discuss in light of our results.
Fixed Typos in Eqs. A.7,9,11
References in corpus (5)
- The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations
- Small x Resummation with Quarks: Deep-Inelastic Scattering
- Higgs production in bottom-quark fusion: matching beyond leading order
- Matched predictions for the cross section at the 13 TeV LHC
- Anatomy of double heavy-quark initiated processes
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