Abstract

We probe the rare semileptonic decays $B_{(s)} \to K_2^*(1430)(f_2'(1525)) \ell^+\ell^-$ proceeding via $b\to s \ell \ell$ transition in the presence of a light $Z^{\prime}$ boson. We employ the presence of an additional vector type interaction and constrain the new physics coupling parameter using the existing experimental measurements on $R_K$ and $R_{K^*}$ observables. To understand the sensitivity of the new physics coupling, we investigate the impact of this coupling on various physical observables such as differential branching ratio, the forward-backward asymmetry, the lepton polarization asymmetry, the angular observable $P_5^{\prime}$, and the lepton universality parameters such as the ratio of the branching ratio $R_{f_2'(K_2^*)}$ and some important Q parameters of $B_{(s)} \to K_2^*(1430)(f_2'(1525)) \ell^+\ell^-$ processes at large recoil. We find some noticeable differences of the observables in the presence of light $Z^{\prime}$ contribution.

Highlights

  • According to our best understanding, the standard model (SM), a successful theory, is not enough to explain some key puzzles such as matter-antimatter asymmetry in the Universe, dark matter, dark energy, hierarchy problem, neutrino mass, and so on

  • In order to scrutinize the structure of new physics, we explore with various interesting observables for the processes BðsÞ → Tlþl− given as follows [52]: (i) differential branching ratio

  • Using the new physics (NP) coupling, we report the impact on various observables such as differential branching ratio, the lepton polarization fraction FL, the forward-backward asymmetry AFB, and the angular observable P05

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Summary

INTRODUCTION

According to our best understanding, the standard model (SM), a successful theory, is not enough to explain some key puzzles such as matter-antimatter asymmetry in the Universe, dark matter, dark energy, hierarchy problem, neutrino mass, and so on. In the light of neutral quark-level transitions, several measurements, most importantly, the lepton flavor universality violation (LFUV) parameter RKÃ 1⁄4 BRðB → KÃμþμ−Þ= BRðB → KÃeþe−Þ observed from LHCb [1,2] and Belle [3], have 2.1 − 2.4σ deviation from SM prediction ∼1 [4,5]. In the presence of light mediators, the discrepancy can be explained for the observables like the RK and RKÃ [43,44,45] In this respect, we consider a light Z0 in which the NP Wilson coefficients are q2 dependent [33,38,44,45,46] and study the impact on BðBsÞ → TfKÃ2ð1430Þ ðf02ð1525ÞÞglþl− decays.

Generalized effective weak Hamiltonian
FORMULAS OF BRANCHING RATIO AND OTHER OBSERVABLES
NEW PHYSICS ANALYSIS
Relevant input parameters
CONCLUSION
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