Measurement of |V_ub| near the endpoint of the electron momentum spectrum from semileptonic B-meson decays

TL;DR

This paper measures the |V_ub| element of the CKM matrix by analyzing the endpoint of the electron momentum spectrum in semileptonic B-meson decays, providing a precise determination based on Belle data.

Contribution

It presents the first measurement of |V_ub| near the electron momentum endpoint using Belle data, combining experimental results with theoretical predictions for improved accuracy.

Findings

Partial branching fraction measured as (8.47 ± 0.37 ± 1.53)×10^{-4}

|V_ub| determined as (5.08 ± 0.47 ± 0.42^{+0.26}_{-0.23})×10^{-3}

Theoretical partial rate R calculated with HQET parameters

Abstract

We report measurements of partial branching fractions of inclusive charmless semileptonic $B$-meson decays at the endpoint of the electron momentum spectrum. The measurements are made in six overlapping momentum intervals that have lower bounds ranging from 1.9 GeV/$c$ to 2.4 GeV/$c$ and a common upper bound of 2.6 GeV/$c$, as measured in the centre of mass frame. The results are based on a sample of 29 million $B\bar{B}$ pairs, accumulated by the Belle detector at the KEKB asymmetric $e^+e^-$ collider operating on the $\Upsilon(4S)$ resonance. In the momentum interval ranging from 1.9 GeV/$c$ to 2.6 GeV/$c$ we measure the partial branching fraction $\Delta \mathcal{B}(B\to X_u e \nu_e)=(8.47 \pm 0.37 \pm 1.53)\times 10^{-4}$, where the first error is statistical and the second is systematic. A prediction of the partial rate $R=(21.69 \pm 3.62^{+ 2.18}_{- 1.98}) |V_{ub}|^2 \mathrm{ps}^{-1}$ in this momentum interval based on theory is calculated with input HQET parameters that have been derived from Belle's measurement of the $B\to X_s\gamma$ photon energy spectrum, where the first error is due to the uncertainty on HQET parameters and the second error is from theory. Using both $\Delta \mathcal{B}(B\to X_u e \nu_e)$ and $R$ we find $|V_{ub}|=(5.08 \pm 0.47 \pm 0.42^{+ 0.26}_{- 0.23})\times 10^{-3}$, where the first error is from the partial branching fraction, and the second and third errors are from uncertainties in $R$.