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- W80482912 abstract "We consider various contributions to the nonresonant decay ${mathit{B}}^{ifmmodepmelsetextpmfi{}}$ensuremath{rightarrow}${mathrm{ensuremath{pi}}}^{+}$${mathrm{ensuremath{pi}}}^{mathrm{ensuremath{-}}}$${mathrm{ensuremath{pi}}}^{ifmmodepmelsetextpmfi{}}$, both of the long-distance and short-distance types, with the former providing for most of the branching ratio, predicted to be scrB(${mathit{B}}^{ifmmodepmelsetextpmfi{}}$ensuremath{rightarrow}${mathrm{ensuremath{pi}}}^{+}$${mathrm{ensuremath{pi}}}^{mathrm{ensuremath{-}}}$${mathrm{ensuremath{pi}}}^{ifmmodepmelsetextpmfi{}}$)=(1.0--5.0)ifmmodetimeselsetexttimesfi{}${10}^{mathrm{ensuremath{-}}5}$. We also discuss an application to CP violation resulting from the interference of that nonresonant background [with m(${mathrm{ensuremath{pi}}}^{+}$${mathrm{ensuremath{pi}}}^{mathrm{ensuremath{-}}}$)ensuremath{approxeq}3.4 GeV] and ${mathit{B}}^{ifmmodepmelsetextpmfi{}}$ensuremath{rightarrow}${mathrm{ensuremath{chi}}}_{mathit{c}0}$${mathrm{ensuremath{pi}}}^{ifmmodepmelsetextpmfi{}}$ followed by ${mathrm{ensuremath{chi}}}_{mathit{c}0}$ensuremath{rightarrow}${mathrm{ensuremath{pi}}}^{+}$${mathrm{ensuremath{pi}}}^{mathrm{ensuremath{-}}}$. The resulting value of the partial rate asymmetry is (0.44--0.49)sinensuremath{gamma}, where ensuremath{gamma}=arg(${mathit{V}}_{mathit{u}mathit{b}}^{mathrm{*}}$)." @default.
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- W80482912 title "Nonresonant Cabibbo suppressed decay<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant=italic>B</mml:mi></mml:mrow><mml:mrow><mml:mo>±</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>→<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant=normal>π</mml:mi></mml:mrow><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math><mml:math …" @default.
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- W80482912 doi "https://doi.org/10.1103/physrevd.52.5354" @default.
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