Strong constraints on the $b \to s\gamma$ photon polarisation from $B^0 \to K^{*0} e^+ e^-$ decays

TL;DR

This study performs an angular analysis of the rare decay $B^0 o K^{*0} e^+ e^-$ at very low $q^2$, providing the most stringent constraints to date on the photon polarisation in $b o s \gamma$ transitions, consistent with the Standard Model.

Contribution

The paper presents the first measurement of photon polarisation in $b o s \gamma$ decays using $B^0 o K^{*0} e^+ e^-$ decays at low $q^2$, setting the world's best constraints.

Findings

Measured $F_L$ as $(4.4 \pm 2.6 \pm 1.4)\%$

Measured $A_T^{Re}$ as $-0.06 \pm 0.08 \pm 0.02$

Results are consistent with Standard Model predictions.

Abstract

An angular analysis of the $B^0 \to K^{*0} e^+ e^-$ decay is performed using a data sample corresponding to an integrated luminosity of $9~{\rm fb}^{-1}$ of $pp$ collisions collected with the LHCb experiment. The analysis is conducted in the very low dielectron mass squared ($q^2$) interval between $0.0008$ and $0.257~{\rm GeV}^2$, where the rate is dominated by the $B^0\to K^{\ast 0}\gamma$ transition with a virtual photon. The fraction of longitudinal polarisation of the $K^{\ast 0}$ meson, $F_{\rm L}$, is measured to be $F_{\rm L} = (4.4 \pm 2.6 \pm 1.4)\%$, where the first uncertainty is statistical and the second systematic. The $A_{\rm T}^{\rm Re}$ observable, which is related to the lepton forward-backward asymmetry, is measured to be $A_{\rm T}^{\rm Re}=-0.06 \pm 0.08 \pm 0.02$. The $A_{\rm T}^{(2)}$ and $A_{\rm T}^{\rm Im}$ transverse asymmetries, which are sensitive to the virtual photon polarisation, are found to be $A_{\rm T}^{(2)} = 0.11 \pm 0.10 \ \pm 0.02$ and $A_{\rm T}^{\rm Im} = 0.02 \pm 0.10 \pm 0.01$. The results are consistent with Standard Model predictions and provide the world's best constraint on the $b\to s\gamma$ photon polarisation.