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We can reproduce the experimental data ${\\rm Br}\\left(D_{sJ}^*(2860)\\to D^*K\\right)/{\\rm Br}\\left(D_{sJ}^*(2860)\\to D K\\right) =1.10 \\pm 0.15 \\pm 0.19$ with suitable hadronic coupling constants, the assignment of the $D_{sJ}^*(2860)$ as the $D_{s3}^*(2860)$ is favored, the chiral symmetry breaking corrections are large. 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