Phenomenological studies on neutral $B$-meson decays into $J/\psi f_1$ and $\eta_c f_1$

TL;DR

This study uses perturbative QCD to analyze $B$-meson decays into $J/$ and $\u03b5_c$ with $f_1$ mesons, predicting measurable branching ratios and CP asymmetries to understand axial-vector meson mixing.

Contribution

It provides detailed predictions for branching fractions, CP asymmetries, and polarization fractions of specific $B$-meson decays, aiding in constraining the $f_1$ meson mixing angle and testing PQCD.

Findings

Branching fractions are large enough for detection at LHCb and Belle-II.

Decays involving $f_1(1420)$ have sizable branching ratios.

CP asymmetries suggest penguin pollution is significant.

Abstract

The axial-vector mesons $f_1(1285)$ and $f_1(1420)$ are particularly viewed as the mixtures of flavor states $f_n$ and $f_s$ with mixing angle $\varphi$. In order to determine this angle, we study the $B_{d,s}^0\to J/\psi f_1(1285,1420)$ and $B_{d,s}^0\to \eta_c f_1(1285,1420)$ decays in perturbative QCD (PQCD) approach, including the effects of vertex corrections, nonfactorizable diagrams and penguin operators. Not only the branching fractions, but also the direct $CP$ asymmetries and the polarization fractions are calculated. It is found that the branching fractions of these decays are large enough to be measured in the running LHCb and Belle-II experiments. Moreover, in comparison with the observed ${\cal B}(B_{d,s}^0 \to J/\psi f_1(1285))$, $B_s^0 \to (J/\psi, \eta_c) f_1(1420)$ decays have large branching fractions, which could be measured promisingly through $f_1(1420) \to K_S^0 K^\pm \pi^\mp$ in experiments. We also propose several ratios that could be used to further constrain the absolute value of the mixing angle $\varphi$, but its sign cannot be determined yet in these decays. The direct CP asymmetries of these decays indicate the penguin pollution in the $B_d^0 \to (J/\psi, \eta_c) f_1$ decays cannot be neglected. We acknowledge that there are large theoretical uncertainties arising from the distribution amplitudes of axial-vector mesons and charmonium states, and more precise nonperturbative parameters are called. The comparisons between our results and future experimental data would help us to understand the nature of $f_1$ states and to test the PQCD approach.