Abstract

The symmetries arise due to heavy quark and large energy limit help us to reduce the number of independent form factors in the heavy-to-light $B$-meson decays. It is expected that these symmetry relations are not exact and are broken by the perturbative effects, namely, the vertex corrections and the hard-spectator scatterings. The former are included in the form factors via vertex renormalization whereas the later are calculated through light-cone distribution amplitudes. We first calculate these symmetry breaking corrections to the form factors involved in semileptonic $B$-meson to an axial-vector $(K_{1})$-meson decay. Later, by using these form factors we see their effect on the physical observables such as the zero-position of the forward-backward $(\mathcal{A}_{FB})$ asymmetry and the longitudinal lepton polarization ($P_L$) asymmetry in $B\rightarrow K_1(1270) \mu^+\mu^-$ decay. We find that as a result of these corrections to the form factors, the zero-position of the forward-backward asymmetry is shifted by $10\%$ from its SM value while the effects on $P_L$ are rather insignificant.

Highlights

  • Form factors for a B meson decaying to a light meson f, where f can be a pseudoscalar (P), a vector (V), an axialvector (A), or a tensor (T) meson, arise due to the matrix element of local flavor-changing currents (FCC) q Γq, with Γ representing some spin structure

  • The former are included in the form factors via vertex renormalization, whereas the latter are calculated through light-cone distribution amplitudes

  • To see how the symmetry breaking corrections influence the values of the observables, we study the implications of the modified form factors on the zero position of the forward-backward asymmetry and the longitudinal lepton polarization asymmetry ðPLÞ for the decay channel B → K1μþμ−

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Summary

INTRODUCTION

Form factors for a B meson decaying to a light meson f, where f can be a pseudoscalar (P), a vector (V), an axialvector (A), or a tensor (T) meson, arise due to the matrix element of local flavor-changing currents (FCC) q Γq, with Γ representing some spin structure. B → ρðKÃÞlþl− decays, it is shown that in the LEET the seven form factors reduce to two in the large recoil limit [10] These symmetry relations are not exact, and they are broken by the radiative corrections. The corrections to the soft part are manifested in the Wilson coefficients at an order αs by matching the LEET calculation with the full one-loop QCD calculation, while for the hardspectator part, the nonperturbative method is required, for which we use light-cone distribution amplitudes (LCDA). These hard-spectator corrections break the symmetry relations. Appendix C gives the detailed calculation of the hard-spectator correction to one of the form factors V2ðq2Þ

FORM FACTORS AT LARGE RECOIL
E Δ ðEF Þðεà vÞ ðmB
SYMMETRY BREAKING CORRECTIONS
Vertex renormalization
Hard-spectator corrections
Form factor analysis
Applications
Forward-backward asymmetry
Ãts V tb
Longitudinal lepton polarization
CONCLUSION
Findings
B-meson parton distribution amplitude
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