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Three-loop soft function for heavy-to-light quark decays
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Three-loop soft function for heavy-to-light quark decays
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We compute the 1-jettiness soft function for the decay of a heavy quark into a light quark jet plus colorless particles at three-loop order in soft-collinear effective theory. The 1-jettiness measurement fixes the total small light-cone momentum component of the soft radiation with respect to the jet direction. This soft function is a universal ingredient to the factorization of heavy-to-light quark decays in the limit of small 1-jettiness. Our three-loop result is required for resummation at the N$^3$LL$^\prime$ level, e.g. near the endpoint in the photon energy spectrum of the $B \to X_s \gamma$ decay. It is also a necessary ingredient for future calculations of fully-differential heavy-to-light quark decay rates at N$^3$LO using the $N$-jettiness subtraction method, e.g. for semileptonic top decays. Using our result for the soft anomalous dimension we confirm predictions on the universal infrared structure of QCD scattering amplitudes with a massive external quark at three loops.
Forward citations
Cited by 2 Pith papers
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Progress on the soft anomalous dimension in QCD
A lightcone-expansion strategy using Wilson-line correlators and the Method of Regions yields the three-loop soft anomalous dimension for QCD amplitudes with one massive colored particle and arbitrary massless ones.
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Approximate N$^2$LO and N$^3$LO QCD Predictions for $tW$ Production
Higher-order QCD corrections to top-plus-W production raise the predicted rate by over 10% and give |Vtb|=0.99±0.03.
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