First Observation of $D^{0(+)}\to \bar K\omega e^+\nu_e$ and Determination of the Branching Fraction of $\bar K_1(1270)\to \bar K \omega$

TL;DR

This paper reports the first observation of specific semileptonic D meson decays involving omega and kaon resonances, measuring their branching fractions and providing the most precise collider-based measurement of the $\bar{K}_1(1270)$ decay to $\bar{K}\omega$.

Contribution

It presents the first observation of $D^0$ and $D^+$ semileptonic decays to $K\omega e^+\nu_e$, measures their branching fractions, and determines the $\bar{K}_1(1270)$ decay branching ratio with unprecedented precision.

Findings

First observation of $D^0\to K^-\omega e^+\nu_e$ and $D^+\to K_S^0\omega e^+\nu_e$.

Measured branching fractions for these decays.

Most precise collider measurement of $\bar{K}_1(1270)\to \bar{K}\omega$ branching fraction.

Abstract

Using 20.3~fb$^{-1}$ of $e^+e^-$ annihilation data collected at a center-of-mass energy of 3.773~GeV with the BESIII detector, we report the first observation of the semileptonic decays $D^0\to K^-\omega e^+\nu_e$ and $D^+\to K_S^0\omega e^+\nu_e$ with significances of $8.0\sigma$ and $5.8\sigma$, respectively, including systematic uncertainties. Their decay branching fractions are measured to be ${\cal B}(D^0\to K^-\omega e^+\nu_e)=(9.3^{+2.1}_{-1.9}\pm 0.7)\times10^{-5}$ and ${\cal B}(D^+\to K_S^0\omega e^+\nu_e)=(6.6^{+2.0}_{-1.8}\pm 0.6)\times10^{-5}$. Combining with the latest measurements of $D^{0(+)}\to K^-\pi^+\pi^{-(0)} e^+\nu_e$ and assuming $\bar{K}_1(1270)$ to be the sole mediating resonance in all processes, the branching ratios are determined to be $\frac{\Gamma(K_1(1270)^-\to K^-\pi^+\pi^-)}{\Gamma(K_1(1270)^-\to K^-\omega)} = 3.4^{+0.8}_{-0.7} \pm 0.3$ and $\frac{\Gamma(\bar{K}_1(1270)^0\to K^-\pi^+\pi^0)}{\Gamma(\bar{K}_1(1270)^0\to \bar{K}^0\omega)} = 9.6^{+3.0}_{-2.7} \pm 0.8$. The combined branching fraction is determined to be $\mathcal B(\bar{K}_1(1270)\to \bar{K}\omega) = (7.5\pm 1.3 \pm 0.5)\%$, which is the most precise measurement from a collider experiment. The first uncertainties are statistical, and the second are systematic.