Within the quasi-two-body decay model,we study the localized CP violation and branching fraction of the four-body decay B^(0)→[K^(-)π^(+)]s/v[π^(+)π^(-)]v/s→K^(-)π^(+)π^(+)π^(-)whenthe K^(-)π^(+)andπ^(-)π^(...Within the quasi-two-body decay model,we study the localized CP violation and branching fraction of the four-body decay B^(0)→[K^(-)π^(+)]s/v[π^(+)π^(-)]v/s→K^(-)π^(+)π^(+)π^(-)whenthe K^(-)π^(+)andπ^(-)π^(+)pair invariant masses are 0.35<mK^(-)π^(+)<2.04GeV and 0<mπ^(-)π^(+)<1.06 GeV,with the pairs being dominated by the K*0(700)0,K*(892)0,K*(1410)0,K*0(1430)and K*(1680)0,and fo(500),ρ0(770),ω(782)and f0(980)resonances,respectively.When dealing with the dynamical functions of these resonances,f0(500),ρ0(770),f0(980)and K*0(1430)are modeled with the Bugg model,Gounaris-Sakurai function,Flatte formalism and LASS lineshape,respectively,while the others are described by the relativistic Breit-W igner function.Adopting the end point divergence parametersρA∈[0,0.5]andφA∈[0,2π],our predicted results are ACρ(B0→K-π^(+)π^(+)π^(-))∈[-0.365.0.447]and B(B0→K-π^(+)π^(+)π^(-))∈[6.11,185.32]×10^(-8),based on the hypothetical qq structures for the scalar mesons in the QCD factorization ap-proach.Meanwhile,we calculate the CP violating asymmetries and branching fractions of the two-body decaysB0→SV(VS)and all the individual four-body decays B0→SV(VS)→K^(-)π^(+)π^(-)π^(+),respectively.Our theoretical results for the two-body decays B0→K<(892)0 f0(980),B0→K*0(1430)0ω(782),B0→K*(892)0f0(980),B0→K*0(1430)0ρ,and B0→K*0(1430)0ωare consistent with the available experimental data,with the remaining predic-tions await testing in future high precision experiments.展开更多
基金Supported by National Natural Science Foundation of China (11575023, 11775024, 11947001, 11605150, 11805153)Natural Science Foundation of Zhejiang pvovince (LQ21A050005)Achievements of the Basic Scientific Research Businessof Universities in Zhejiang Province and Natural Science Foundation of Ningbo (2019A610067)
文摘Within the quasi-two-body decay model,we study the localized CP violation and branching fraction of the four-body decay B^(0)→[K^(-)π^(+)]s/v[π^(+)π^(-)]v/s→K^(-)π^(+)π^(+)π^(-)whenthe K^(-)π^(+)andπ^(-)π^(+)pair invariant masses are 0.35<mK^(-)π^(+)<2.04GeV and 0<mπ^(-)π^(+)<1.06 GeV,with the pairs being dominated by the K*0(700)0,K*(892)0,K*(1410)0,K*0(1430)and K*(1680)0,and fo(500),ρ0(770),ω(782)and f0(980)resonances,respectively.When dealing with the dynamical functions of these resonances,f0(500),ρ0(770),f0(980)and K*0(1430)are modeled with the Bugg model,Gounaris-Sakurai function,Flatte formalism and LASS lineshape,respectively,while the others are described by the relativistic Breit-W igner function.Adopting the end point divergence parametersρA∈[0,0.5]andφA∈[0,2π],our predicted results are ACρ(B0→K-π^(+)π^(+)π^(-))∈[-0.365.0.447]and B(B0→K-π^(+)π^(+)π^(-))∈[6.11,185.32]×10^(-8),based on the hypothetical qq structures for the scalar mesons in the QCD factorization ap-proach.Meanwhile,we calculate the CP violating asymmetries and branching fractions of the two-body decaysB0→SV(VS)and all the individual four-body decays B0→SV(VS)→K^(-)π^(+)π^(-)π^(+),respectively.Our theoretical results for the two-body decays B0→K<(892)0 f0(980),B0→K*0(1430)0ω(782),B0→K*(892)0f0(980),B0→K*0(1430)0ρ,and B0→K*0(1430)0ωare consistent with the available experimental data,with the remaining predic-tions await testing in future high precision experiments.