Nonperturbative O( mc−2) effects in B→ Xsγ from heavy quark effective theory
The nonperturbative contribution, suppressed by powers of the charm quark mass m c , in the inclusive decay B→ X s γ is analyzed in the context of heavy quark effective field theory (HQEFT). According to previous analyses, the leading effects of O(1/ m c 2) arise from an external gluon attached to a...
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Published in | Physics letters. B Vol. 439; no. 1; pp. 165 - 170 |
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Main Author | |
Format | Journal Article |
Language | English |
Published |
Elsevier B.V
29.10.1998
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Subjects | |
Online Access | Get full text |
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Summary: | The nonperturbative contribution, suppressed by powers of the charm quark mass
m
c
, in the inclusive decay
B→
X
s
γ is analyzed in the context of heavy quark effective field theory (HQEFT). According to previous analyses, the leading effects of
O(1/
m
c
2) arise from an external gluon attached to a charm quark loop and can be expressed in terms of the chromomagnetic interaction of the
b quark inside the
B meson. This is also true at leading order in the HQEFT approach. However the structure of higher-dimensional operators is different because the effects of external gluons alone do not give a complete set of operators. A systematic method to derive all the high-dimensional operators can be obtained in the HQEFT scheme using the operator product expansion. |
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ISSN: | 0370-2693 1873-2445 |
DOI: | 10.1016/S0370-2693(98)01011-9 |