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Axial-vector and pseudoscalar tetraquarks $[ud][\bar{c}\bar{s}]$ (2206.05004v3)

Published 10 Jun 2022 in hep-ph, hep-ex, and hep-lat

Abstract: Spectroscopic parameters and widths of the fully open-flavor axial-vector and pseudoscalar tetraquarks $X_{\mathrm{AV}}$ and $X_{\mathrm{PS}}$ with content $[ud][\overline{c}\overline{s}]$ are calculated by means of the QCD sum rule methods. Masses and current couplings of $X_{\mathrm{AV}}$ and $X_{ \mathrm{PS}}$ are found using two-point sum rule computations performed by taking into account various vacuum condensates up to dimension $10$. The full width of the axial-vector state $X_{\mathrm{AV}}$ is evaluated by including into analysis $S$-wave decay modes $X_{\mathrm{AV}}\to D{\ast }(2010){-}K{+}$, $\overline{D}{\ast }(2007){0}K{0}$, $D{-}K{\ast }(892){+}$, and $\overline{D}{0}K{\ast }(892){0}$. In the case of $X_{ \mathrm{PS}}$, we consider $S$-wave decay $X_{\mathrm{PS}}\to \overline{D} {0}{\ast }(2300){0}K{0}$, and $P$-wave processes $X{\mathrm{PS}}\to D{-}K{\ast}(892){+}$ and $X_{\mathrm{PS}}\to \overline{D} {0}K{\ast}(892){0}$. To determine partial widths of these decay modes, we employ the QCD light-cone sum rule method and soft-meson approximation, which are necessary to estimate strong couplings at tetraquark-meson-meson vertices $X_{\mathrm{AV}}D{-}D{\ast }(2010){-}K{+} $, etc. Our predictions for the mass $m_{\mathrm{AV}}=(2800 \pm 75)~\mathrm{MeV}$ and width $\Gamma_{\mathrm{AV}}=(58 \pm 10)~\mathrm{MeV}$ of the tetraquark $X_{ \mathrm{AV}}$, as well as results $m_{\mathrm{PS}}=(3000 \pm 60)~\mathrm{MeV} $ and $\Gamma_{\mathrm{PS}}=(65 \pm 12)~\mathrm{MeV}$ for the same parameters of $X_{\mathrm{PS}}$ may be useful in future experimental studies of multiquark hadrons.

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