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Semileptonic and exclusive rare B decays
The exclusive rare decay B→K ∗γ takes place in a region of maximum recoil, q 2=0, posing a problem for nonrelativistic quark models which are usually thought to be most reliable at zero recoil. The Bauer-Stech-Wirbel (BSW) model, formulated in the infinite-momentum-frame (IMF) formalism, is designed...
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Published in: | Physics letters. B 1994-04, Vol.325 (1), p.219-226 |
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Main Authors: | , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | The exclusive rare decay
B→K
∗γ
takes place in a region of maximum recoil,
q
2=0, posing a problem for nonrelativistic quark models which are usually thought to be most reliable at zero recoil. The Bauer-Stech-Wirbel (BSW) model, formulated in the infinite-momentum-frame (IMF) formalism, is designed to work at
q
2=0. We show in this model that the ratio relating the decay
B→K
∗γ
and the
q
2-spectrum of the semileptonic decay
B→ϱe
ν
, becomes independent of the wave function in the SU(3) flavor symmetry limit. We show that this feature is also true in relativistic quark models formulated in the IMF or light-cone formalism, if the
b quark is infinitely heavy. In fact, these relativistic models, which have a different spin structure from the BSW case, reduce to the BSW model in the heavy
b-quark limit. A direct measurement of the
q
2-spectrum of the semileptonic decay cam therefore provide accurate information for the exclusive rare decay. |
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ISSN: | 0370-2693 1873-2445 |
DOI: | 10.1016/0370-2693(94)90095-7 |