BcB_c meson production at the Tevatron Revisited

preprint1999arXivOpen access

Abstract

CDF recently measured the quantity σ(Bc+)σ(B+)BR(Bc+→J/ψℓ+ν)BR(B+→J/ψK+)\frac{σ(B_c^+)}{σ(B^+)} \frac{{\rm BR}(B_c^+ \to J/ψ\ell^+ ν)}{{\rm BR}(B^+ \to J/ψK^+)}, {}from which we determine the ratio σ(Bc+)σ(bˉ)\frac{σ(B_c^+)}{σ(\bar b)} to be $(2.08\err{1.06}{0.95})\times 10^{-3}$. In this note, we show that the ratio σ(Bc+)σ(bˉ)\frac{σ(B_c^+)}{σ(\bar b)} obtained by dividing the σ(Bc+)σ(B_c^+) by the leading order σ(bˉ)σ(\bar b) is consistent with this derived CDF measurement. We calculate the cross section σ(Bc+)σ(B_c^+) using the perturbative QCD fragmentation functions of Braaten, Cheung, and Yuan and the corresponding induced gluon fragmentation functions, with the charm-quark mass mcm_c as a parameter. We also estimate the parameter mcm_c from the CDF data and then predict the production rate at RunII.

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