Strong decays $B_{s0}\to B_s\pi$ and $B_{s1}\to B_s^{\ast }\pi$ with light-cone QCD sum rules

Abstract

In this article, we calculate the strong coupling constants $g_{B_{s0}{B}_s\eta }$ and $g_{B_{s1}{B}_s^{\ast }\eta }$ with the light-cone QCD sum rules. Then we take into account the small $\eta -{\pi }^0$ transition matrix according to Dashen's theorem, and obtain the small decay widths for the isospin violation processes $B_{s0}\to B_s\eta \to B_s{\pi }^0$ and $B_{s1}\to B_s^{\ast }\eta \to B_s^{\ast }{\pi }^0$. We can search the strange-bottomed $(0^{+},1^{+})$ mesons $B_{s0}$ and $B_{s1}$ in the invariant $B_s{\pi }^0$ and $B_s^{\ast }{\pi }^0$ mass distributions respectively.

arXiv comment15 pages, 2 figures, revised version

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Cited by in corpus (5)

• Analysis of the masses and decay constants of the heavy-light mesons with QCD sum rules
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• The Strong Decays of Orbitally Excited $B_{sJ}^{\ast }$ Mesons by Improved Bethe-Salpeter Method
• Radiative decays of the $(0^{+},1^{+})$ strange-bottom mesons
• $B_{s1}(5778)$ as a $B^{\ast }\bar{K}$ molecule in the Bethe-Salpeter equation approach