Model-independent analysis of B → πℓ + ℓ − decays
Ahmed Ali, A. Ya. Parkhomenko, Aleksey V. Rusov
Abstract
Open-access reader
Ahmed Ali, A. Ya. Parkhomenko, Aleksey V. Rusov
Abstract
Open-access reader
The results obtained by calculating, on the basis of the Standard Model, the branching fractions for the decays B → πℓ + ℓ − (ℓ ± = e ±, µ±) and the invariant-mass spectrum of dileptons for the process B + → π + ℓ + ℓ − are presented. The resulting theoretical estimates depend on the choice of model for the B → π transition form factors f +(q 2), f 0(q 2), and f T (q 2). However, one can get rid of this arbitrariness by employing experimental data or the results of QCD lattice calculations to determine the parameter dependence of the form factors. Data from B-meson factories were used to determine the dependence of the form factor f +(q 2) on the transfer momentum squared. Yet another required form factor, f T (q 2), was extracted from available lattice data on B → π and B → K transitions with allowance for nearly identical effects of the breakdown of flavor SU(3) F symmetry in the respective form factors. The resulting value of the decay branching fraction, B(B + → π +µ+µ−) = (1.88 −0.21 +0.32 ) × 10−8, is in good agreement with the results of measurements of the LHCb Collaboration. The branching fraction for the isospin analog of the decay under consideration is B(B + → π +µ+µ−) = (0.94 −0.11 +0.16 ) × 10−8. Therefore, this decay can be measured at the Super-B factory under construction.
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The results obtained by calculating, on the basis of the Standard Model, the branching fractions for the decays B → πℓ + ℓ − (ℓ ± = e ±, µ±) and the invariant-mass spectrum of dileptons for the process B + → π + ℓ + ℓ − are presented. The resulting theoretical estimates depend on the choice of model for the B → π transition form factors f +(q 2), f 0(q 2), and f T (q 2). However, one can get rid of this arbitrariness by employing experimental data or the results of QCD lattice calculations to determine the parameter dependence of the form factors. Data from B-meson factories were used to determine the dependence of the form factor f +(q 2) on the transfer momentum squared. Yet another required form factor, f T (q 2), was extracted from available lattice data on B → π and B → K transitions with allowance for nearly identical effects of the breakdown of flavor SU(3) F symmetry in the respective form factors. The resulting value of the decay branching fraction, B(B + → π +µ+µ−) = (1.88 −0.21 +0.32 ) × 10−8, is in good agreement with the results of measurements of the LHCb Collaboration. The branching fraction for the isospin analog of the decay under consideration is B(B + → π +µ+µ−) = (0.94 −0.11 +0.16 ) × 10−8. Therefore, this decay can be measured at the Super-B factory under construction.
Key concepts: Physics, Isospin, Particle physics, Branching fraction, B meson, B-factory, Momentum transfer, Meson