Υ(6S)Υ(6S) and triangle singularity in e+e−→B1(5721)Bˉ→Zb(10610) πe^+e^- \to B_1(5721) \bar B \to Z_b(10610) \, π

preprint2016arXivOpen access

Abstract

We discuss the possibility that production of final states with bottomonium and light mesons at the peak Υ(6S)Υ(6S) in the e+e−e^+e^- annihilation at approximately 11.00 GeV is in fact due to a triangular singularity at the threshold of the heavy meson pair production B1(5721)Bˉ+c.c.B_1(5721) \bar B + c.c. through the process e+e−→B1(5721)Bˉ→Zb(10610) πe^+e^- \to B_1(5721) \bar B \to Z_b(10610) \, π. The presence of the hidden-bottom resonance Zb(10610)Z_b(10610) then explains the observed enhanced production of the final channels with both ortho- and para- bottomonium states, Υ(nS)ππΥ(nS) ππ and hb(kP)ππh_b(kP) ππ. The discussed mechanism also predicts a distinct pattern for production of hidden-bottom states at the Υ(6S)Υ(6S) energy that can be tested by experiment.

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