29,926 research outputs found

    Implications of Charmless B Decays with Large Direct CP Violation

    Full text link
    Based on the most recent data in charmless B decays including the very recently reported large direct CP violations, it is shown that the weak phase gamma can well be extracted without two-fold ambiguity even only from two decay modes pi^+pi^- and pi^+K^-, and its value is remarkably consistent with the global standard model fit at a compatible accuracy. A fit to all the pi pi, pi K data favor both large electroweak penguin and color-suppressed tree amplitude with large strong phases. It is demonstrated that the inclusion of small SU(3)symmetry breaking effects of strong phases and the inelastic rescattering effects can well improve the consistency of the data, while both effects may not be sufficient to arrive at a small electroweak penguin amplitude in the standard model. It is of interest to notice that large or small electroweak penguin amplitude becomes a testable prediction as they lead to significantly different predictions for the direct CP violations for pi^0 pi^0, pi^0 K^0 modes. Clearly, precise measurements on charmless B decays will provide a window for probing new physics.Comment: 4 pages, 1 figure, 1 table, results updated with the latest data. conclusions unchanged. Refence added. published versio

    Charmless decays B->pipi, piK and KK in broken SU(3)symmetry

    Full text link
    Charmless B decay modes B→ππ,πKB \to \pi \pi, \pi K and KKKK aresystematically investigated with and without flavor SU(3) symmetry. Independent analyses on ππ\pi \pi and πK\pi K modes both favor a large ratio between color-suppressed tree (CC) and tree (T)T) diagram, which suggests that they are more likely to originate from long distance effects. The sizes of QCD penguin diagrams extracted individually from ππ\pi\pi, πK\pi K and KKKK modes are found to follow a pattern of SU(3) breaking in agreement with the naive factorization estimates. Global fits to these modes are done under various scenarios of SU(3)relations. The results show good determinations of weak phase γ\gamma in consistency with the Standard Model (SM), but a large electro-weak penguin (P_{\tmop{EW}}) relative to T+CT + C with a large relative strong phase are favored, which requires an big enhancement of color suppressed electro-weak penguin (P_{\tmop{EW}}^C) compatible in size but destructively interfering with P_{\tmop{EW}} within the SM, or implies new physics. Possibility of sizable contributions from nonfactorizable diagrams such as WW-exchange (EE), annihilation(AA) and penguin-annihilation diagrams(PAP_A) are investigated. The implications to the branching ratios and CP violations in KKK Kmodes are discussed.Comment: 27 pages, 9 figures, reference added, to appear in Phy.Rev.

    Implications of new data in charmless B decays

    Get PDF
    Based on the latest experimental data of B→ππB \to \pi\pi and πK\pi K modes, a model-independent analytical analysis is presented. The CP-averaged branching ratio difference ΔR=Rc−Rn\Delta R = R_c - R_n in B→πKB\to \pi K decays with Rc=2Br(π0K−)/Br(π−Kˉ0)R_c = 2Br(\pi^0K^-)/Br(\pi^-\bar{K}^0) and Rn=Br(π+K−)/2Br(π0Kˉ0)R_n =Br(\pi^+K^-)/2Br(\pi^0\bar{K}^0) is reduced though it remains larger than the prediction from the standard model(SM) as both measured RnR_n and RcR_c are enhanced, which indicates that a room for new physics becomes smaller. The present data of ππ\pi\pi decay reduce the ratio ∣C/T∣|C/T| from the previous value of ∣C/T∣≃0.8|C/T|\simeq 0.8 to ∣C/T∣≃0.65|C/T| \simeq 0.65, which is still larger than the theoretical estimations based on QCD factorization and pQCD. Within SM and flavor SU(3) symmetry, the current πK\pi K data also diminish the ratio ∣C′/T′∣|C'/T'| from the previous value ∣C′/T′∣≃2|C'/T'| \simeq 2 to ∣C′/T′∣≃1.16|C'/T'| \simeq 1.16 with a large strong phase δC′≃−2.65\delta_{C'} \simeq -2.65, while its value remains much larger than the one extracted from the ππ\pi \pi modes. The direct CP violation ACP(π0Kˉ0)A_{CP}(\pi^0\bar{K}^0) is predicted to be ACP(π0Kˉ0)=−0.15±0.03A_{CP}(\pi^0\bar{K}^0) = -0.15\pm0.03, which is consistent with the present data. Two kinds of new effects in both strong and weak phases of the electroweak penguin diagram are considered. It is found that both cases can reduce the ratio to ∣C′/T′∣=0.40∼0.80|C'/T'| = 0.40\sim 0.80 and lead to roughly the same predictions for CP violation in π0K0\pi^0 K^0.Comment: 13 pages, 4 figure
    • …
    corecore