Revisiting the Annihilation Corrections in Non-leptonic Bˉs0\bar{B}_s^0 Decays within QCD Factorization

preprint2012arXivOpen access

Abstract

Motivated by the recent measurements of non-leptonic Bˉs0\bar{B}_s^0 decays by CDF and LHCb collaborations, especially the large B(Bˉs0→π+π−){\cal B}(\bar{B}_s^0\toπ^+π^-), we revisit the hard spectator and annihilation corrections in Bˉs0\bar{B}_s^0 decays within QCD factorization approach with two schemes for the possible parameters for the known end-point divergence appeared in the estimation of the hard spectator and annihilation diagrams. The first one is to conservatively estimate the possible contributions by parameterization (scheme I); another one uses an infrared finite gluon propagator (scheme II) to regulate the end-point singularity. In scheme I, with the constraints from the measured Bˉs0→PP(VV)\bar{B}_s^0\to PP (VV) decays, two (four) restricted solutions of the parameters spaces are found. In scheme II, we find that most of the theoretical predictions agree well with the experimental data with single parameter mg∼0.5GeVm_{g}\sim 0.5{\rm GeV}. However, within both schemes, B(Bˉs0→ϕϕ){\cal B}(\bar{B}_s^0\toϕϕ) are always much larger than B(Bˉs0→K∗0Kˉ∗0){\cal B}(\bar{B}_s^0\to K^{\ast 0}\bar{K}^{\ast 0}) in contrast to the experimental results B(Bˉs0→ϕϕ)≃B(Bˉs0→K∗0Kˉ∗0){\cal B}(\bar{B}_s^0\toϕϕ)\simeq{\cal B}(\bar{B}_s^0\to K^{\ast 0}\bar{K}^{\ast 0}). It is noted that the pattern B(Bˉs0→ϕϕ)>B(Bˉs0→K∗0Kˉ∗0){\cal B}(\bar{B}_s^0\toϕϕ)>{\cal B}(\bar{B}_s^0\to K^{\ast 0}\bar{K}^{\ast 0}) also persists in other theoretical framework, thus the present experimental result B(Bˉs0→ϕϕ)≃B(Bˉs0→K∗0Kˉ∗0){\cal B}(\bar{B}_s^0\toϕϕ) \simeq {\cal B}(\bar{B}_s^0\to K^{\ast 0}\bar{K}^{\ast 0}) rises a challenge to theoretical approaches for B non-leptonic decays. Further refined measurements and theoretical studies are called for to resolve such a possible anomaly.

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