We report a measurement of the branching fraction of B→K∗(892)ℓ+ℓ− decays, where ℓ+ℓ−=μ+μ− or
e+e−, using electron-positron collisions recorded at an energy at or near
the Υ(4S) mass and corresponding to an integrated luminosity of 189
fb−1. The data was collected during 2019--2021 by the Belle II experiment
at the SuperKEKB e+e− asymmetric-energy collider. We reconstruct
K∗(892) candidates in the K+π−, KS0π+, and K+π0
final states. The signal yields with statistical uncertainties are 22±6,
18±6, and 38±9 for the decays B→K∗(892)μ+μ−, B→K∗(892)e+e−, and B→K∗(892)ℓ+ℓ−, respectively.
We measure the branching fractions of these decays for the entire range of the
dilepton mass, excluding the very low mass region to suppress the B→K∗(892)γ(→e+e−) background and regions compatible with decays
of charmonium resonances, to be \begin{equation} {\cal B}(B \to
K^{\ast}(892)\mu^+\mu^-) = (1.19 \pm 0.31 ^{+0.08}_{-0.07}) \times 10^{-6},
{\cal B}(B \to K^{\ast}(892)e^+e^-) = (1.42 \pm 0.48 \pm 0.09)\times 10^{-6},
{\cal B}(B \to K^{\ast}(892)\ell^+\ell^-) = (1.25 \pm 0.30 ^{+0.08}_{-0.07})
\times 10^{-6}, \end{equation} where the first and second uncertainties are
statistical and systematic, respectively. These results, limited by sample
size, are the first measurements of B→K∗(892)ℓ+ℓ− branching
fractions from the Belle II experiment