Axial-vectorf1(1285)−f1(1420)mixing andBs→J/ψ(f1(1285),f1(1420))decays
Author:
Funder
National Natural Science Foundation of China
Publisher
American Physical Society (APS)
Subject
Nuclear and High Energy Physics
Link
http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevD.89.097503/fulltext
Reference28 articles.
1. Observation ofB¯(s)0→J/ψf1(1285)Decays and Measurement of thef1(1285)Mixing Angle
2. Implications of the Glueball- $q \overline q$ filter on the $1^{++}$ nonet
3. Is f 1 (1420) the Partner of f 1 (1285) in the 3 P 1 qq̄ Nonet?
4. Observation of spin-1f1(1285) in the reaction γγ*→η0π+π−
5. SU(3) mixing for excited mesons
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1. The $$B^0 \rightarrow J/\psi f_0(1370,1500,1710)$$ decays: an opportunity for scalar glueball hunting;The European Physical Journal C;2024-04-04
2. Phenomenological studies on neutral B-meson decays into $$J/\psi f_1$$ and $$\eta _c f_1$$;The European Physical Journal C;2023-01-10
3. Constraints imposed by the partial wave amplitudes on the decays of J=1 , 2 mesons;Physical Review D;2022-03-21
4. Bd,s0→f1f1 decays with f1(1285)−f1(1420) mixing in the perturbative QCD approach;Physical Review D;2020-12-21
5. Mixing and mq dependence of axial vector mesons in the Coulomb gauge QCD model;Physical Review D;2019-12-17
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