Perturbative QCD analysis of neutral B-meson decays into $$\sigma \sigma , \sigma f_0$$ σ σ , σ f 0 and $$f_0 f_0$$ f 0 f 0

• Published in: The European physical journal. C, Particles and fields Particles and fields, 2022-02, Vol.82 (2), p.1-14
• Main Authors: Hua-Dian Niu, Guo-Dong Li, Jia-Le Ren, Xin Liu
• Format: Article
• Language: English
• ISSN: 1434-6044; 1434-6052
• DOI: 10.1140/epjc/s10052-022-10111-8

Abstract The decays of $$B_{d,s}^0 \rightarrow \sigma \sigma , \sigma f_0, f_0 f_0$$ B d , s 0 → σ σ , σ f 0 , f 0 f 0 , with $$\sigma $$ σ and $$f_0$$ f 0 denoting the light scalar mesons $$f_0(500)$$ f 0 ( 500 ) and $$f_0(980)$$ f 0 ( 980 ) in the two-quark picture, are studied in the perturbative QCD approach based on $$k_T$$ k T factorization. With the referenced value of the mixing angle $$|\varphi | \sim 25^\circ $$ | φ | ∼ 25 ∘ for the $$\sigma -f_0$$ σ - f 0 mixing in the quark-flavor basis, it is of great interest to obtain that: (a) these neutral B-meson decays into $$\sigma \sigma , \sigma f_0$$ σ σ , σ f 0 , and $$f_0 f_0$$ f 0 f 0 have large branching ratios in the order of $$10^{-6}{-}10^{-4}$$ 10 - 6 - 10 - 4 , which mean the possibly constructive interferences existed in the decays with different flavor states, and then are expected to be tested at the Large Hadron Collider beauty and/or Belle-II experiments in the (near) future; (b) the large direct CP violations could be easily found in the $$B_d^0 \rightarrow \sigma \sigma , f_0 f_0$$ B d 0 → σ σ , f 0 f 0 and $$B_{d,s}^0 \rightarrow \sigma f_0$$ B d , s 0 → σ f 0 decays, which indicate the considerable interferences between the tree and the penguin decay amplitudes involved in these four modes, and would be confronted with the future measurements; (c) these neutral B-meson decays could be examined through the secondary decay chain $$\sigma /f_0 \rightarrow \pi ^+ \pi ^-$$ σ / f 0 → π + π - , namely, the four-body decays of $$B_{d,s}^0 \rightarrow (\pi ^+ \pi ^-)_{\sigma (f_0)} (\pi ^+ \pi ^-)_{\sigma (f_0)}$$ B d , s 0 → ( π + π - ) σ ( f 0 ) ( π + π - ) σ ( f 0 ) with still large branching ratios. On the other side, it seems that other 4 four-body decays of $$B_d^0 \rightarrow (\pi ^+ \pi ^-)_{\sigma } (K^+ K^-)_{f_0}$$ B d 0 → ( π + π - ) σ ( K + K - ) f 0 , $$B_s^0 \rightarrow (\pi ^+ \pi ^-)_{\sigma (f_0)} (K^+ K^-)_{f_0}$$ B s 0 → ( π + π - ) σ ( f 0 ) ( K + K - ) f 0 , and $$B_s^0 \rightarrow (K^+ K^-)_{f_0} (K^+ K^-)_{f_0}$$ B s 0 → ( K + K - ) f 0 ( K + K - ) f 0 could also be detected at the relevant experiments, if the $$f_0 \rightarrow K^+ K^-$$ f 0 → K + K - could be identified from the $$\phi \rightarrow K^+ K^-$$ ϕ → K + K - clearly. The (near) future experimental confirmations with good precision would help to further study the perturbative and/or nonperturbative QCD dynamics involved in these considered decay modes, as well as to explore the intrinsic characters of these