Feasibility of extracting Vtd from radiative B(Bs) decays

Nuovo Cimento della Societa Italiana di Fisica A

Volumn 109, Issue 6, 1996, Pages 873-883

  Atwood, D ^a   Blok, B ^b   Soni, A ^c  

^a SLAC NATIONAL ACCELERATOR LABORATORY   (United States)

^b TECHNION ISRAEL INSTITUTE OF TECHNOLOGY   (Israel)

^c BROOKHAVEN NATIONAL LABORATORY   (United States)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 5544320425     PISSN: 03693546     EISSN: None     Source Type: Journal    
DOI: 10.1007/bf02823629     Document Type: Article

References (45)

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29. BURAS A. J. et al., preprint MPI-PH-98-77; see also CIUCHINI M. et al., Phys. Lett. B, 334 (1994) 137. A partial list of earlier references on the subjects is GRINSTEIN B., SPRINGER R. and WISE M., Nucl. Phys. B, 339 (1990) 269; GRIGJANIS R. et al., Phys. Lett. B, 237 (1990) 252; MISIAK M., Phys. Lett. B, 269 (1969) 161.
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32. Recently other estimates on long-distance contributions to B → K* + γ due only to uū states have appeared in the literature. See CARLSON C. E. and MILANA J., preprint UMD-PP-94-129; GREUB C., SIMMA H. and WYLER D., DESY preprint 94-089.
33. Recently other estimates on long-distance contributions to B → K* + γ due only to uū states have appeared in the literature. See CARLSON C. E. and MILANA J., preprint UMD-PP-94-129; GREUB C., SIMMA H. and WYLER D., DESY preprint 94-089.
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35. BERNARD C., HSIEH P. and SONI A., Phys. Rev. Lett., 72 (1994) 1402. See also BOWLER K. C. et al., Phys. Rev. Lett., 72 (1994) 1398; HEP-LAT-9407013. The APE group is also working on this reaction but their results are, at the moment, preliminary. See ABADA A., contribution to the XXVII International Conference on HEP, Glasgow, July 1994.
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37. This is reminiscent of the situation in the non-leptonic two-body decays of D mesons. See BLOK B. and SHIFMAN M., Sov. J. Nucl. Phys., 45 (1987) 135, 301, 522.
38. BERNARD C. and SONI A., in Quantum Fields on the Computer, edited by M. CREUTZ (World Scientific). See in particular pp. 396-406.
39. 0 + γ (see eqs. (20) and (21)) they are both much too small compared to LD effects from c̄c states. Therefore in table I the difference between eqs. (20) and (21) is being disregarded.
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