Strange partners of the doubly charmed tetraquark $T_{cc}^{+}$

The spectroscopic parameters and widths of the axial-vector $T_{cc:s}^{\mathrm{A}\mathrm{V}}$ and scalar $T_{cc:s}^{\mathrm{S}}$, ${\tilde{T}}_{cc:s}^{\mathrm{S}}$ strange partners of the doubly charmed exotic meson $T_{cc}^{+}$ with the content $cc\bar{u}\bar{s}$, are calculated in the framework of the QCD sum rule method. We model $T_{cc:s}^{\mathrm{A}\mathrm{V}}$ as the diquark-antidiquark state composed of axial-vector and scalar components, whereas scalar particles $T_{cc:s}^{\mathrm{S}}$ and ${\tilde{T}}_{cc:s}^{\mathrm{S}}$ are built of axial-vector and scalar diquarks, respectively. The masses and current couplings of these tetraquarks are calculated in the context of the two-point sum rule approach by taking into account the quark, gluon and mixed condensates up to dimension $10$. The full width of the state $T_{cc:s}^{\mathrm{A}\mathrm{V}}$ is found from analysis of the processes $T_{cc:s}^{\mathrm{A}\mathrm{V}}\to D^0{D}_s^{\ast +}$ and $T_{cc:s}^{\mathrm{A}\mathrm{V}}\to D^{\ast }(2007{)}^0{D}_s^{+}$. Decays to $D^0{D}_s^{+}$, $D^{\ast }(2007{)}^0{D}_s^{\ast +}$ and $D^0{D}_s^{+}$ mesons are utilized in the case of the scalar tetraquarks $T_{cc:s}^{\mathrm{S}}$ and ${\tilde{T}}_{cc:s}^{\mathrm{S}}$, respectively. The partial widths of the aforementioned decays are determined via the strong couplings $g_1$, $g_2$, $G_1$, $G_2$ and $\tilde{G}$, which describe the strong interactions of the particles at the relevant tetraquark-meson-meson vertices. These couplings are computed using the QCD three-point sum rule method, most appropriate for the strong decays under study. …