2014
DOI: 10.1051/epjconf/20148000047
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Rapidity resummation forB-meson wave functions

Abstract: Abstract. Transverse-momentum dependent (TMD) hadronic wave functions develop light-cone divergences under QCD corrections, which are commonly regularized by the rapidity ζ of gauge vector defining the non-light-like Wilson lines. The yielding rapidity logarithms from infrared enhancement need to be resummed for both hadronic wave functions and short-distance functions, to achieve scheme-independent calculations of physical quantities. We briefly review the recent progress on the rapidity resummation for B-mes… Show more

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Cited by 4 publications
(2 citation statements)
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“…It is evident that the standard momentum-space resummation technique cannot be applied to cope with this term which is independent of the factorization scale. Investigating resummation of such logarithm with the rapidity RG evolution equations [43][44][45][46] is apparently of conceptual interest and we will pursue this endeavour in a future work.…”
Section: The Lcsr Of λ B → λ Form Factors At O(α S )mentioning
confidence: 99%
“…It is evident that the standard momentum-space resummation technique cannot be applied to cope with this term which is independent of the factorization scale. Investigating resummation of such logarithm with the rapidity RG evolution equations [43][44][45][46] is apparently of conceptual interest and we will pursue this endeavour in a future work.…”
Section: The Lcsr Of λ B → λ Form Factors At O(α S )mentioning
confidence: 99%
“…Albeit the fact that factorization in a non-abelian gauge theory like QCD is by no means a trivial issue, collinear factorization for a number of interesting hard reactions, at leading power in 1/Q where Q is the typical hard scale for a given process, can be established with rigorous power counting schemes and standard assumptions. By contrast, transverse-momentum-dependent (TMD) factorization for hard exclusive processes based upon the theory of on-shell Sudakov form factor [1], with the original aim of avoiding the rapidity divergences in collinear factorization for the pion electromagnetic form factor at sub-leading power [2], turns out to be far more sophisticated conceptually due to the absence of a definite power counting scheme and to the emergence of lightcone singularities in the infrared subtraction, and this can be already partially recognized from the troubled history of TMD wave functions [3][4][5][6][7][8][9][10][11][12][13][14].…”
Section: Introductionmentioning
confidence: 99%