Abstract:The bottom partners of the D * s0 (2317) and D s1 (2460) have not been measured yet but the existence of these bottom-strange J P = 0 + and J P = 1 + states is motivated by Heavy Quark Flavor Symmetry and Heavy Quark Spin Symmetry. Here we show the predictions for such heavy quark partners using a unitarized effective approach involving SU(3) Chiral Heavy Meson Symmetry and incorporating explicit di-quark Fock components (Qq) to the theory in a Heavy Quark Spin and Flavour Symmetry consistent way. We take adva… Show more
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