Abstract

We predict that the $a_0^0(980)$-$f_0(980)$ mixing would lead to large CP violation. We calculate the localized direct CP asymmetry in the decays $B^\pm \to f_0(980) [a_0^0(980)] \pi^\pm \to \pi^+ \pi^- \pi^\pm $ via the $a_0^0(980)$-$f_0(980)$ mixing mechanism based on the hypothetical $q\bar q$ structures of $a^0_0(980)$ and $f_0(980)$ in the QCD factorization. It is shown that there is a peak for CP violation, which could be as large as 58%, when the invariance mass of $\pi\pi$ is near the masses of $a^0_0(980)$ and $f_0(980)$. Since the CP asymmetry is sensitive to the $a_0^0(980)$-$f_0(980)$ mixing, measuring the CP violating parameter in the aforementioned decays could provide a new way to verify the existence of the $a_0^0(980)$-$f_0(980)$ mixing and be helpful in clarifying the configuration nature of the light scalar mesons.

Highlights

  • We predict that a00ð980Þ − f0ð980Þ mixing would lead to large CP violation

  • We calculate the localized direct CP asymmetry in the decays BÆ → f0ð980Þ1⁄2a00ð980ފπÆ → πþπ−πÆ via the a00ð980Þ − f0ð980Þ mixing mechanism based on the hypothetical qqstructures of a00ð980Þ and f0ð980Þ in the QCD factorization approach

  • Since the CP asymmetry is sensitive to a00ð980Þ − f0ð980Þ mixing, measuring the CP-violating parameter in the aforementioned decays could provide a new way to verify the existence of a00ð980Þ − f0ð980Þ mixing and be helpful in clarifying the configuration of the light scalar mesons

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Summary

Published by the American Physical Society

These KKloops would lead to a mixing amplitude. The LHCb Collaboration has focused on multibody final states in the decays of the B mesons and used a novel strategy to probe CP asymmetries in the Dalitz plots [7]. These multibody decays provide much more information on strong phases than the two-body decays. A00ð980Þ − f0ð980Þ mixing, if it exists, would affect the CP violation of the sequential three-body decay B → f0ð980Þ1⁄2a00ð980ފP → ππP (where P represents a pseudoscalar meson) when the invariant mass of the final ππ is located around 980 MeV. 2m2Bðm þ m2PÞ þ ðm2B − m2PÞ2Š=ð2mBÞ with mP being the mass of P

The amplitudes can be expressed as
By defining
XHðAÞ ln mB Λh
ΦBðρÞ dξ ξ
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