DD wave bottomonia production from Zb(′)Z_b^{(\prime)} decay

preprint2020arXivOpen access

Abstract

In the present work, we investigate the dipion transitions between Υ(5S)Υ(5S) and ΥJ(1D)Υ_J(1D) with J=1,2,3J=1, 2, 3. Our analysis indicates that the dominant sources of the anomalously large widths of Υ(5S)→ΥJ(1D)π+π−Υ(5S)\to Υ_J(1D) π^+ π^- should be Zb(′)Z_b^{(\prime)}, i.e., the dipion transitions occur via the cascade decays Υ(5S)→Zb(′)±π∓→ΥJ(1D)π+π−Υ(5S)\to Z_b^{(\prime)\pm} π^\mp \to Υ_J(1D) π^+ π^-. With the assumption that all the short ranged dynamics could be absorbed in a single cutoff with a model parameter αα, the present estimations indicate that in a reasonable parameter range the measured branching ratios of Υ(5S)→ΥJ(1D)π+π−Υ(5S) \to Υ_J(1D) π^+ π^- can be reproduced in magnitude, which further proves that the decays via Zb(′)Z_b^{(\prime)} dominate the dipion transitions of Υ(5S)Υ(5S) to ΥJ(1D)Υ_J(1D). Moreover, we also predict the ratios of the branching fractions of Zb(′)→ΥJ(1D)πZ_b^{(\prime)} \to Υ_J(1D) π, which in our calculations are largely independent of the parameter αα and could be tested by further experiments in Belle II.

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