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Combining with the measured masses and decay properties of $\\Xi_{b}(6327)^{0}$ and $\\Xi_{b}(6327)^{0}$, the two excited states can be explained as $1D$ $\\lambda$-mode $\\Xi_b$ states $\\Xi_{b}|J^{P}=\\frac{3}{2}^{+},2\\rangle_{\\lambda\\lambda}$ and $\\Xi_{b}|J^{P}=\\frac{5}{2}^{+},2\\rangle_{\\lambda\\lambda}$, respectively. 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Combining with the measured masses and decay properties of $\\Xi_{b}(6327)^{0}$ and $\\Xi_{b}(6327)^{0}$, the two excited states can be explained as $1D$ $\\lambda$-mode $\\Xi_b$ states $\\Xi_{b}|J^{P}=\\frac{3}{2}^{+},2\\rangle_{\\lambda\\lambda}$ and $\\Xi_{b}|J^{P}=\\frac{5}{2}^{+},2\\rangle_{\\lambda\\lambda}$, respectively. 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