Abstract

It is by now well known that, at subleading power in scale ratios, factorization theorems for high-energy cross sections and decay amplitudes contain endpoint-divergent convolution integrals. The presence of endpoint divergences hints at a violation of simple scale separation. At the technical level, they indicate an unexpected failure of dimensional regularization and the overline{mathrm{MS}} subtraction scheme. In this paper we start a detailed discussion of factorization at subleading power within the framework of soft-collinear effective theory. As a concrete example, we factorize the decay amplitude for the radiative Higgs-boson decay h → γγ mediated by a b-quark loop, for which endpoint-divergent convolution integrals require both dimensional and rapidity regulators. We derive a factorization theorem for the decay amplitude in terms of bare Wilson coefficients and operator matrix elements. We show that endpoint divergences caused by rapidity divergences cancel to all orders of perturbation theory, while endpoint divergences that are regularized dimensionally can be removed by rearranging the terms in the factorization theorem. We use our result to resum the leading double-logarithmic corrections of order {alpha}_s^n{ln}^{2n+2}left(-{M}_h^2/{m}_b^2right) to the decay amplitude to all orders of perturbation theory.

Highlights

  • A method based on N -jettiness (TN ) slicing [1, 2] allows one to obtain the next-to-nextto-leading order (NNLO) QCD result from a much easier next-to-leading order (NLO) calculation, combined with information about the singular dependence of the cross section on the TN resolution variable [3]

  • We show that endpoint divergences caused by rapidity divergences cancel to all orders of perturbation theory, while endpoint divergences that are regularized dimensionally can be removed by rearranging the terms in the factorization theorem

  • The factorized decay amplitude in Soft-collinear effective theory (SCET) is subject to both types of endpoint divergences: those regularized with the dimensional regulator and those regularized by a rapidity regulator

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Summary

Bare factorization theorem

The h → γγ amplitude is always to be understood as the contribution mediated by virtual b-quarks. The difference between the b-quark pole mass mpb ole and the running mass mb(Mh) is almost a factor of 2, and scale ambiguities can have a large impact on the decay rate. Analyzing the QCD diagrams giving rise to the decay amplitude at one- and two-loop order using the method of regions [49,50,51], we find that the amplitude receives leading contributions from the following momentum regions of loop momenta: hard (h) : n1-collinear (c) : n2-collinear (c) : soft (s) :. This serves as a cross check that we have identified the leading momentum regions correctly

Matching onto SCET-1
Matching onto SCET-2
Hard matching coefficients
Operator matrix elements
Rapidity divergences and analytic regulators
Introducing rapidity regulators
Cancellation of rapidity divergences
Subtraction of endpoint divergences
Resummation of the leading double logarithms
Conclusions and outlook
A Operator matrix elements in SCET-1
B Exact analytic expression for the soft function
C NLO coefficients in the bare decay amplitude
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