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Weak phases from {ital B} decays to kaons and charged pions

Journal Article · · Physical Review, D
 [1];  [2];  [3]
  1. Enrico Fermi Institute and Department of Physics, University of Chicago, Chicago, Illinois 60637 (United States)
  2. Department of Physics, Technion---Israel Institute of Technology, Haifa 32000 (Israel)
  3. Div. TH, CERN, 1211 CH Geneva 23, Switzerl

Phases of elements of the Cabibbo-Kobayashi-Maskawa (CKM) matrix can be obtained using decays of {ital B} mesons to {pi}{sup +}{pi}{sup {minus}}, {pi}{sup {plus_minus}}{ital K}{sup {minus_plus}}, and {pi}{sup +}{ital K}{sup 0} or {pi}{sup {minus}}{ital {bar K}}{sup 0}. For {ital B}{sup 0} or {ital {bar B}}{sup 0}{r_arrow}{pi}{sup +}{pi}{sup {minus}}, one identifies the flavor of the neutral {ital B} meson at time of production and studies the time dependence of the decay rate. The other processes are self-tagging and only their rates need to be measured. By assuming flavor SU(3) symmetry and first-order SU(3) breaking, one can separately determine the phases {gamma}{equivalent_to}Arg{ital V}{sub {ital ub}}{sup {asterisk}} and {alpha}={pi}{minus}{beta}{minus}{gamma}, where {beta}{equivalent_to}Arg{ital V}{sub {ital td}}{sup {asterisk}}. Special cases include the vanishing of strong interaction phase differences between amplitudes, the possibility of recovering partial information when {pi}{sup +}{pi}{sup {minus}} and {pi}{sup {plus_minus}}{ital K}{sup {minus_plus}} decays cannot be distinguished from one another, and the use of a correlation between {gamma} and {alpha} in the region of allowed parameters. {copyright} {ital 1996 The American Physical Society.}

Research Organization:
University of Chicago
DOE Contract Number:
FG02-90ER40560
OSTI ID:
383386
Journal Information:
Physical Review, D, Journal Name: Physical Review, D Journal Issue: 5 Vol. 54; ISSN PRVDAQ; ISSN 0556-2821
Country of Publication:
United States
Language:
English

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