Abstract

We investigate the pure annihilation type radiative $B$ meson decays $B^0 \to \phi \gamma$ and $B_s \to \rho^0(\omega)\gamma$ in the soft-collinear effective theory. We consider three types of contributions to the decay amplitudes, including the direct annihilation topology, the contribution from the electro-magnetic penguin operator and the contribution of the neutral vector meson mixings. The numerical analysis shows that the decay amplitudes are dominated by the $\omega-\phi$ mixing effect in the $B^0 \to \phi\gamma$ and $B_s \to \omega\gamma$ modes. The corresponding decay branching ratios are enhanced about three orders of magnitudes relative to the pure annihilation type contribution in these two decay channels. The decay rate of $B_s \to \rho^0\gamma$ is much smaller than that of $B_s \to \omega\gamma$ because of the smaller $\rho^0-\phi$ mixing. The predicted branching ratios $B(B^{0}\rightarrow\phi\gamma)=(3.99^{+1.67}_{-1.46} )\times10^{-9},\,B(B_s\rightarrow\omega\gamma)=(2.01^{+0.81}_{-0.71} )\times10^{-7}$ are to be tested by the Belle-II and LHC-b experiments.

Highlights

  • The exclusive radiative B decay modes B → Vγ are very interesting and valuable probes of flavor physics, since they provide an excellent platform to constrain standard model parameters, to test new physics models, and to understand QCD factorization of the decay amplitudes [1]

  • We investigate the pure annihilation type radiative B meson decays B0 → φγ and Bs → ρ0ðωÞγ in the soft-collinear effective theory

  • Collecting all the contributions to the factorization amplitudes calculated in the previous section together, we arrive at the final expression of the decay amplitudes for the pure annihilation type B → Vγ decays: AðB0 → φγÞ 1⁄4 cos δ1⁄2AðB0 → φIγÞjanni þ AðB0 → φIγÞjEMPŠ − sinδAðB → ωIγÞ; AðBs → ωγÞ 1⁄4 cos δ1⁄2AðBs → ωIγÞjanni þ AðBs → ωIγÞjEMPŠ þ sin δAðBs → φIγÞ; AðBs → ρ0γÞ 1⁄4 AðBs → ρ0γÞjanni þ AðBs → ρ0γÞjEMP: ð31Þ

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Summary

INTRODUCTION

The exclusive radiative B decay modes B → Vγ are very interesting and valuable probes of flavor physics, since they provide an excellent platform to constrain standard model parameters, to test new physics models, and to understand QCD factorization of the decay amplitudes [1]. The predicted branching ratio within the framework of the perturbative QCD factorization approach is at this order [21]. For the Bs → ρ0ðωÞγ mode, the contribution from the electromagnetic penguin operator is of great importance, and the branching ratio is at the order of 10−10 − 10−9 [20]. If the branching ratios of pure annihilation type B decays can be significantly enhanced by the neutral meson mixing, the Super-B factory and LHCb might have a chance to find the signals of these processes. This paper is arranged as follows: we will present the factorization formulas of B0 → φγ and Bs → ρ0ðωÞγ decays, including the leading power contribution, and the contributions from the annihilation topology, the electromagnetic penguin operator, and the ω − φ mixing effect.

THEORETICAL OVERVIEW OF PURE ANNIHILATION TYPE RADIATIVE BðBsÞ DECAYS
Contribution from weak annihilation
C10 V 1 Þ ð16Þ with the vertex correction term
Contribution from electromagnetic penguin operator
Contribution from mixing of neutral vector mesons
Input parameters
Phenomenological predictions
CLOSING REMARKS

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