Abstract

We show how to compute directly the renormalization/evolution of the radiative jet function that appears in the factorization theorems for $B\to \gamma\ell\nu$ and $H\to \gamma\gamma$ through a $b$-quark loop. We point out that, in order to avoid double counting of soft contributions, one should use in the factorization theorems a subtracted radiative jet function, from which soft contributions have been removed. The soft-contribution subtractions are zero-bin subtractions in the terminology of soft-collinear effective theory. We show that they can be factored from the radiative jet function and that the resulting soft-subtraction function gives rise to a nonlocal renormalization of the subtracted radiative jet function. This is a novel instance in which zero-bin subtractions lead to a nonlocality in the renormalization of a subtracted quantity that is not present in the renormalization of the unsubtracted quantity. We demonstrate the use of our formalism by computing the order-$\alpha_s$ evolution kernel for the subtracted radiative jet function. Our result is in agreement with the result that had been inferred previously by making use of the factorization theorem for $B\to \gamma\ell\nu$, but that had been ascribed to the unsubtracted radiative jet function.

Highlights

  • In the amplitudes for exclusive processes, contributions in which a quark carries a soft momentum appear at subleading power in the ratio of the quark mass to the large momentum transfer in the process

  • Our result is in agreement with the result that had been inferred previously by making use of the factorization theorem for B → γlν, but that had been ascribed to the unsubtracted radiative jet function

  • In the language of soft-collinear effective theory (SCET) [13,14,15,16,17], the softquark contributions occur through a process in which a jet function containing collinear quarks and gluons emits a soft quark via a subleading-power interaction

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Summary

INTRODUCTION

In the amplitudes for exclusive processes, contributions in which a quark carries a soft momentum appear at subleading power in the ratio of the quark mass to the large momentum transfer in the process. We point out that the radiative jet function contains soft contributions that are already taken into account in the soft functions of the exclusive factorization theorems These soft contributions must be subtracted from the radiative jet function in order to avoid double counting. Our result for the order-αs renormalization-group kernel of the subtracted radiative jet function is in agreement with the result in Ref.

NOTATION AND CONVENTIONS
Operator definition of the radiative jet function
RENORMALIZATION OF THE RADIATIVE JET FUNCTION
LOWEST-ORDER EXPRESSIONS
UV divergences of JsAubðp2Þ at order αs
Jsubðp2Þ x
VANISHING OF THE SOFT SUBTRACTIONS IN DIMENSIONAL REGULARIZATION
VIII. SUMMARY AND DISCUSSION

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