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There has been speculation in the literature that the $D_{s1}^*(2710)$ is the $2^3S_1(c\\bar{s})$ state and the $D_{sJ}^*(2860)$ is the $1^3D_1(c\\bar{s})$ state. In this paper we explore this and other explanations in the context of the relativized quark model and the pseudoscalar emission decay model. 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