Papers
Topics
Authors
Recent
Search
2000 character limit reached

Contributions of the subprocesses ρ(770,1450,1700)KKˉρ(770,1450,1700)\to K \bar{K} and ω(782,1420,1650)KKˉω(782,1420,1650)\to K \bar{K} for the three-body decays Bη()KKˉB\to η^{(\prime)} K\bar{K}

Published 2 Feb 2026 in hep-ph and hep-ex | (2602.01534v1)

Abstract: As an extension of our prior work, we analyze the resonance contributions for the kaon pair originating from the intermediate ρ(770)ρ(770), ω(782)ω(782) and their excited states in the three-body decays Bη<sup>()</sup>KKˉB\to η<sup>{(\prime)}</sup> K\bar{K} within the perturbative QCD approach. The information of subprocesses ρ(770,1450,1700)KKˉρ(770,1450,1700)\to K\bar K and ω(782,1420,1650)KKˉω(782,1420,1650)\to K\bar K are included in the distribution amplitudes for KKˉK\bar K system by using the kaon vector time-like form factors. We calculate the CPCP averaged branching fractions and the direct CPCP asymmetries for the relevant quasi-two-body BB meson decays. The branching fractions of the virtual contributions for KKˉK\bar K from the Breit-Wigner formula tails of ρ(770)ρ(770) and ω(782)ω(782) for these decays are found comparable to the corresponding contributions from the resonances ρ(1450,1700)ρ(1450,1700) and ω(1420,1650)ω(1420,1650). Consequently, they constitute a significant component that should be accounted for in the considered three-body decays. All the predictions in this work are expected to be tested by the LHCb and Belle-II experiments in the future.

Summary

No one has generated a summary of this paper yet.

Paper to Video (Beta)

No one has generated a video about this paper yet.

Whiteboard

No one has generated a whiteboard explanation for this paper yet.

Open Problems

We haven't generated a list of open problems mentioned in this paper yet.

Continue Learning

We haven't generated follow-up questions for this paper yet.