Some properties of the states at the hidden-strangeness mixed ${\frac{1}{2}}^{+}+{\frac{1}{2}}^{-}$ heavy meson pair threshold in $e^{+}{e}^{-}$ annihilation

Abstract

The threshold behavior of $e^{+}{e}^{-}$ annihilation is considered in the channels $B_{s0}{\bar{B}}_s^{\ast }+c.c.$, $B_{s1}{\bar{B}}_s+c.c.$, and $B_{s1}{\bar{B}}_s^{\ast }+c.c.$, where $B_{s0}$ and $B_{s1}$ are the excited bottom-strange $J^P=0^{+}$ and $J^P=1^{+}$ mesons. It is argued that due to the heavy quark spin symmetry (HQSS) only one coherent combination of the first two channels is produced in the $S$ wave as well as the third channel. Thus, if there exist threshold molecular peaks in the considered channels, only two of such peaks can be formed in the annihilation. The properties of such threshold states are discussed, including the heavy-light spin structure and the related transitions to bottomonium plus light mesons, as well as mixing with the channels with and without hidden strangeness.

arXiv comment9 pages

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Cited by in corpus (3)

• The impact of $S$-wave thresholds $D_{s1}{\bar{D}}_s+c.c.$ and $D_{s0}{\bar{D}}_s^{\ast }+c.c.$ on vector charmonium spectrum
• $S$ wave hidden charm - hidden strangeness production in $e^{+}{e}^{-}$ annihilation
• Equality of $e^{+}{e}^{-}$ production amplitudes for scalar-vector and pseudoscalar-axial heavy meson-antimeson pairs