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Understanding the D^+_(sJ)(2317) and D^+_(sJ)(2460) with Sum Rules in HQET
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Understanding the D^+_(sJ)(2317) and D^+_(sJ)(2460) with Sum Rules in HQET
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In the framework of heavy quark effective theory we use QCD sum rules to calculate the masses of the $\bar c s$ $(0^+, 1^+)$ and $(1^+, 2^+)$ excited states. The results are consistent with that the states $D_{sJ}(2317)$ and $D_{sJ}(2460)$ observed by BABAR and CLEO are the $0^+$ and $1^+$ states in the $j_l={1\over 2}^+$ doublet.
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Cited by 1 Pith paper
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Medium modifications of $1P$-wave charmonia $\chi_{cJ}(1P)$ in cold nuclear matter
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