Abstract

We investigate the $B_{d,s}^0 \to f_1 f_1$ decays in the framework of perturbative QCD(PQCD) approach with a referenced value $\phi_{f_1} \sim 24^\circ$. Here, $f_1$ denotes the axial-vector mesons $f_1(1285)$ and $f_1(1420)$ with mixing angle $\phi_{f_1}$ in the quark-flavor basis. The observables such as branching ratios, direct CP violations, and polarization fractions of the $B_s^0 \to f_1 f_1$ decays are predicted for the first time. We find that: (i) the almost pure penguin modes $B_s^0 \to f_1 f_1$ have large branching ratios in the order of $10^{-6} \sim 10^{-5}$ due to the Cabibbo-Kobayashi-Maskawa enhancement and generally constructive interferences between the amplitudes of $B_s^0 \to f_n f_s$ and $B_s^0 \to f_s f_s$ with $f_n$ and $f_s$ being the quark-flavor states of $f_1$ mesons; (ii) The observables receive important contributions from the weak annihilation diagrams in the PQCD approach. In particular, without the annihilation contributions, the $B_s^0 \to f_1(1420) f_1(1420)$ branching ratio will decrease about 81% and its longitudinal polarization fraction will reduce around 43%. And (iii) the dependence of the $B_{d,s}^0 \to f_1 f_1$ decay rates on $\phi_{f_1}$ exhibits some interesting line shapes, whose confirmations would be helpful to constrain the determination of $\phi_{f_1}$ inversely. All the PQCD predictions await for the (near) future examinations at Large Hadron Collider beauty and/or Belle-II experiments to further understand the properties of the axial-vector mesons and the perturbative dynamics released from the considered decay modes.

Highlights

  • As listed in the Particle Data Group (PDG) [1], the f1ð1285Þ and its partner, namely, the f1ð1420Þ,1 are categorized into the light axial-vector meson family with a spin-parity quantum number JP 1⁄4 1þ

  • All the perturbative QCD (PQCD) predictions await for the future examinations at Large Hadron Collider beauty and/or Belle-II experiments to further understand the properties of the axial-vector mesons and the perturbative dynamics released from the considered decay modes

  • We obtained the small decay rates that are hard to be measured in the CKM suppressed B0d → f1f1 decays while the large branching ratios that are easy to be accessible in the CKM favored B0s → f1f1 ones due to the interferences with different extents among the flavor decay amplitudes

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Summary

INTRODUCTION

As listed in the Particle Data Group (PDG) [1], the f1ð1285Þ and its partner, namely, the f1ð1420Þ,1 are categorized into the light axial-vector meson family with a spin-parity quantum number JP 1⁄4 1þ. The PQCD approach does not need to introduce any other parameters, except for the essential nonperturbative inputs, namely, wave functions or distribution amplitudes for the initial and final mesons Note that these inputs are universal and are usually computed in the nonperturbative techniques such as QCD sum rules and lattice QCD, or extracted from the available experimental data. The PQCD predictions for the B → PP, PV, and VV decays have shown good consistency globally with the existing data within errors It means that the PQCD approach has the unique advantage and general reliability at the aspects of calculating the hadronic matrix elements in the heavy B meson decays. The interested readers could refer to the review article [26] for more details about this PQCD approach

FORMALISM AND PERTURBATIVE CALCULATIONS
Perturbative calculations in the PQCD approach
C10 Mhnfe þ
NUMERICAL RESULTS AND DISCUSSIONS
CP-averaged branching ratios
CP-averaged polarization fractions
Direct CP-violating asymmetries
CONCLUSIONS AND SUMMARY
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