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Enhanced Charmless Yield in B Decays and Inclusive B-Decay Puzzles
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Enhanced Charmless Yield in B Decays and Inclusive B-Decay
Puzzles
Isard Dunietz
Fermi National Accelerator Laboratory, P.O. Box 500, Batavia, IL 60510
Our analysis suggests that the charmless yield in B decays is enhanced over tradi-
tional estimates. The cc pair produced in b → ccs transitions may be seen signifi-
cantly as light hadrons due to non-perturbative effects. Existing data samples at
Υ(4S) and Z0 factories allow key measurements which are outlined.
1 Motivation
One prime motivation for optimizing our understanding of inclusive B decays
is CP violation. CP asymmetries at the 50% level are predicted for the time-
evolved Bd → J/ψKS decays
1, within the CKM model. The few hundred
reconstructed J/ψKS events
2 would thus allow meaningful CP studies, once
they are tagged. Tagging denotes distinction of an initially pure Bd and Bd.
An optimal tagging algorithm combines self-tagging 3,4,2 with all available in-
formation from the other b-hadron decay 5. Thus inclusive b-hadron decays
must be understood. Such an understanding would enhance CP studies with
B samples both inclusive 6 or exclusive. It would reduce backgrounds for any
B-decay under study. Intriguing hadronization effects may be discovered 7.
2 Traditional Puzzles
The b is known to decay normally to a c, and that charm flavor is referred to
as “right” charm. In contrast, the b → c process produces “wrong” charm.
The penguin amplitudes give rise to b → s transitions, which are seen as a
kaon, additional light hadrons, and possibly additional KK pairs. Due to the
small |Vub/Vcb| ~ 0.1, the b → u transitions are negligible at the present level
of accuracy. Theory calculates the rates for b → c?ν 8, b → ccs 9,10,11, and the
ratio of rates 9
rud ≡
Γ(b → cud′)
Γ(b → ceν)
= 4.0± 0.4 . (1)
The CKM parameters cancel in the ratio. The phase-space factor cancels in
leading order and rud would be 3 because of color counting. QCD corrections
(comple
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