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   <subfield code="a">Light meson mass dependence of the positive-parity heavy-strange mesons</subfield>
   <subfield code="h">[Elektronische Daten]</subfield>
   <subfield code="c">[M. Cleven, F. Guo, C. Hanhart, U. Meißner]</subfield>
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   <subfield code="a">Abstract.: We calculate the masses of the resonances $\ensuremath D_{s0}^{\ast}(2317)$ and $\ensuremath D_{s1}(2460)$ as well as their bottom partners as bound states of a kaon and a $\ensuremath D^{(\ast)}$ - and $\ensuremath B^{(\ast)}$ -meson, respectively, in unitarized chiral perturbation theory at next-to-leading order. After fixing the parameters in the $\ensuremath D_{s0}^{\ast}(2317)$ channel, the calculated mass for the $\ensuremath D_{s1}(2460)$ is found in excellent agreement with experiment. The masses for the analogous states with a bottom quark are predicted to be $\ensuremath M_{B^{\ast}_{s0}}=(5696\pm 40)$ MeV and $\ensuremath M_{B_{s1}}=(5742\pm 40)$ MeV in reasonable agreement with previous analyses. In particular, we predict $\ensuremath M_{B_{s1}}{-}M_{B_{s0}^{\ast}}=46\pm 1$ MeV. We also explore the dependence of the states on the pion and kaon masses. We argue that the kaon mass dependence of a kaonic bound state should be almost linear with slope about unity. Such a dependence is specific to the assumed molecular nature of the states. We suggest to extract the kaon mass dependence of these states from lattice QCD calculations.</subfield>
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   <subfield code="t">The European Physical Journal A</subfield>
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