We apply the method of QCD sum rules to study the \(QQ\bar{ Q}\bar{ q}\) and \(QQ\bar{ Q}\bar{ s}\) tetraquark states, where $Q=c,b$ and $q=u,d$, with the quantum number \(J^P = 0^{ +}\). We consider the contributions of vacuum condensates up to dimension-9 in the operator product expansion, and use the energy scale formula \(\mu = \sqrt{ M_{ X}^2 - (i\mathbb{ M}_c + j\mathbb{ M}_b)^2} - k\mathbb{ M}_s\) to determine the optimal energy scales for the QCD spectral densities. Our results indicate that triply charm tetraquark states \(cc\bar{ c}\bar{ q}\) and \(cc\bar{ c}\bar{ s}\) have masses in the ranges of $5.38-5.84\,\text{ GeV}$ and $5.66-6.16\,\text{ GeV}$, respectively. In the bottom sector, triply bottom tetraquark states \(bb\bar{ b}\bar{ q}\) and \(bb\bar{ b}\bar{ s}\) have masses in the ranges of $14.89-15.55\,\text{ GeV}$ and $14.95-15.66\,\text{ GeV}$, respectively. This study could help distinguish these states in upcoming high-energy nuclear and particle experiments.
Categories: hep-ph