Abstract

We systematically revisit the baryonic four-body semileptonic decays of $B^- \to {\bf B}\bar{\bf B}'\ell^- \bar{\nu}_{\ell}$ by the perturbative QCD counting rules with ${\bf B}$ representing octet baryons and $\ell=e,\mu$. We study the transition form factors of $B^- \to {\bf B} \bar{\bf B}'$ in the limit of $(p_{\bf B}+p_{\bar{\bf B}'})^2 \to \infty $ with the three-body $\bar{B}\to {\bf B}\bar{\bf B}' M$ and $B^- \to p\bar{p} \mu^- \bar{\nu}_{\mu}$ data along with $SU(3)_f$ flavor symmetry. We calculate the decay branching ratios and angular asymmetries as well as the differential decay branching fractions of $B^- \to p \bar{p} \ell^- \bar{\nu}_{\ell}$. In particular, we find that our new result of ${\cal B}( B^- \to p \bar{p} \ell^- \bar{\nu}_{\ell})=(5.21\pm0.34)\times 10^{-6}$, which is about one order of magnitude lower than the previous theoretical prediction of $(10.4\pm2.9)\times 10^{-5}$, agrees well with both experimental measurements of $(5.8^{+2.6}_{-2.3})\times 10^{-6}$ and $(5.3\pm0.4)\times 10^{-6}$ by the Belle and LHCb Collaborations, respectively. We also evaluate the branching ratios and angular asymmetries in other channels of $B^- \to {\bf B}\bar{\bf B}\ell^- \bar{\nu}_{\ell}$, which can be tested by the ongoing experiments at LHCb and BelleII.

Highlights

  • In 2011, the baryonic four-body semileptonic decay of B− → ppl−νl (l 1⁄4 e or μ) was studied with its decay branching ratio predicted to be ð10.4 Æ 2.6 Æ 1.2Þ × 10−5 in Ref. [1]

  • We find that our new result of BðB− → ppl−νlÞ 1⁄4 ð5.21 Æ 0.34Þ × 10−6, which is about one order of magnitude lower than the previous theoretical prediction of ð10.4 Æ 2.9Þ × 10−5, agrees well with both experimental measurements of ð5.8þ−22..36Þ × 10−6 and ð5.3 Æ 0.4Þ × 10−6 by the Belle and LHCb Collaborations, respectively

  • III, we show our numerical results of the form factors fitted by threebody B → BB 0M processes and the latest B− → ppμ−νμ result, and present our predictions of the branching ratios and angular asymmetries in B− → BBl−νl

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Summary

INTRODUCTION

In 2011, the baryonic four-body semileptonic decay of B− → ppl−νl (l 1⁄4 e or μ) was studied with its decay branching ratio predicted to be ð10.4 Æ 2.6 Æ 1.2Þ × 10−5 in Ref. [1]. In 2011, the baryonic four-body semileptonic decay of B− → ppl−νl (l 1⁄4 e or μ) was studied with its decay branching ratio predicted to be ð10.4 Æ 2.6 Æ 1.2Þ × 10−5 in Ref. Both statistical and systematic uncertainties of the LHCb data have significant improvements compared with the previous ones by Belle [2] These decay modes are useful for determining the value of jVubj as the works in the other baryonic modes [4], as well as the underlying new CPT-violating effects. QCD methods, such as the factorizations and sum rules which have been widely used in the mesonic decays of B− → πþπ−l−νl (Bl4) [5–7] These modes should be considered in the fit for the extraction of Vub. Qualitatively speaking, to reduce the theoretical values for the decay branching ratios of B− → pplνl, a smaller value of jVubj is needed besides the form factors.

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