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Leading logarithms of the b quark mass in inclusive B → Xsγ decay
Part of the order α s correction to the inclusive B → X s γ photon spectrum is enhanced by log( m b 2 m s 2 ) . We discuss its origin and sum the corrections proportional to [α s log( m b 2 μ 2 )] n to all orders. These are the calculable leading logarithms in the parton fragmentation functions of a...
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Published in: | Physics letters. B 1995-09, Vol.357 (4), p.653-658 |
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Main Authors: | , , |
Format: | Article |
Language: | English |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | Part of the order
α
s
correction to the inclusive
B →
X
s
γ photon spectrum is enhanced by
log(
m
b
2
m
s
2
)
. We discuss its origin and sum the corrections proportional to
[α
s
log(
m
b
2
μ
2
)]
n
to all orders. These are the calculable leading logarithms in the parton fragmentation functions of a quark or gluon into a photon. Although the gluon fragmentation into a photon starts only at order
α
s
2, its contribution is of the same order as the
s quark's in the leading log sum. For not too small values of the photon energy, the resummation.yields a moderate suppression. In the standard model, the coefficient of the operator whose matrix element gives rise to such terms is small. A measurement of the photon spectrum around 1 GeV would provide a theoretically clean determination of
C
8, the Wilson coefficient of the
b →
s
g operator. |
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ISSN: | 0370-2693 1873-2445 |
DOI: | 10.1016/0370-2693(95)00962-K |