First observation of quantum correlations in $e^+e^-\to XD\bar{D}$ and $C$-even constrained $D\bar{D}$ pairs

Abstract

The study of meson pairs produced with quantum correlations gives direct access to parameters that are challenging to measure in other systems. In this Letter, the existence of quantum correlations due to charge-conjugation symmetry $C$ are demonstrated in $D\bar{D}$ pairs produced through the processes $e^+e^-\to D\bar{D}$, $e^+e^- \to D^{*}\bar{D}$, and $e^+e^- \to D^{*} \bar{D}^*$, where the lack of charge superscripts refers to an admixture of neutral-charm-meson particle and antiparticle states, using $7.13 \text{ fb}^{-1}$ of $e^+e^-$ collision data collected by the BESIII experiment between center-of-mass energies of $4.13-4.23 \text{ GeV}$. Processes with either $C$-even or $C$-odd constraints are identified and separated. A procedure is presented that harnesses the entangled production process to enable measurements of $D^0$-meson hadronic parameters. This study provides the first confirmation of quantum correlations in $e^+e^-\to X D\bar{D}$ processes and the first observation of a $C$-even constrained $D\bar{D}$ system. The procedure is applied to measure $δ^{D}_{Kπ}$, the strong phase between the $D^0\to K^-π^+$ and $\bar{D}^0\to K^-π^+$ decay amplitudes, which results in the determination of $δ^{D}_{Kπ}=\left(192.8^{+11.0 + 1.9}_{-12.4 -2.4}\right)^\circ$. The potential for measurements of other hadronic decay parameters and charm mixing with these and future datasets is also discussed.

Figures (2)

• Figure 1: $M_{\text{miss,$\gamma D{\overline{ {D}}\xspace}$}}^2$ distribution of the ${D}\xspace{\overline{ {D}}\xspace}\xspace\to K_S^0\pi^0\text{ vs. }K_S^0\pi^0$ candidates identified with an $e^+e^-\to{{D}\xspace^*}\xspace{{\overline{ D\xspace}}\xspace{}^*}\xspace\xspace$ hypothesis in data, compared to a simulation without quantum correlations.
• Figure 2: The ratios of efficiency-corrected yields observed in data to those expected in the absence of correlations and mixing for each ${D}\xspace{\overline{ {D}}\xspace}\xspace$ final state originating from each production mechanism. The displayed errors include systematic uncertainties.