Weak Phase γγ and Strong Phase δδ from CP Averaged B→ππB\to ππ and πKπK Decays

preprint2000arXivOpen access

Abstract

Assuming SU(3) symmetry for the strong phases in the four decay modes $B\rarrow π^-π^+, π^0 π^+, π^- K^+, π^- \bar{K}^0$ and ignoring the relative small electroweak penguin effects in those decays, the weak phase γγ and the strong phase δδ can be determined in a model independent way by the CP-averaged branching ratios of the four decay modes. It appears that the current experimental data for B→ππB\to ππ and πKπK decays prefer a negative value of cos⁡γcos⁡δ\cosγ\cosδ. By combining with the other constraints from VubV_{ub}, Bd,s0−Bˉd,s0B^{0}_{d,s}-\bar{B}^{0}_{d,s} mixings and indirect CP-violating parameter εKε_K within the standard model, two favorable solutions for the phases γγ and δδ are found to lie in the region: $35^{\circ}\altγ\alt 62^{\circ}$ and $106^{\circ}\alt δ\alt 180^{\circ}$ or $86^{\circ}\altγ\alt 151^{\circ}$ and $0^{\circ}\altδ\alt 75^{\circ} $ within 1σσ standard deviation. It is noted that if allowing the standard deviation of the data to be more than 1σσ, the two solutions could approach to one solution with a much larger region for the phases γγ and δδ. Direct CP asymme try aε′′(π−K+)a_{ε''}^{(π^- K^+)} in $B\rarrow π^-K^+$ decay can be as large as the present experimental upper bound. Direct CP asymmetry aε′′(π+π−)a_{ε''}^{(π^+π^-)} in $B\rarrow π^-π^+$ decay can reach up to about 40% at 1σσ level.

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