We investigate the decay of f1(1285)→πKK¯ with the assumption that the f1(1285) is dynamically generated from the K⁎K¯−cc interaction. In addition to the tree level diagrams that proceed via f1(1285)→K⁎K¯−cc→πKK¯ , we take into account also the final state interactions of KK¯→KK¯ and πK→πK . The partial decay width and mass distributions of f1(1285)→πKK¯ are evaluated. We get a value for the partial decay width which, within errors, is in fair agreement with the experimental result. The contribution from the tree level diagrams is dominant, but the final state interactions have effects in the mass distributions. The predicted mass distributions are significantly different from phase space and tied to the K⁎K¯−cc nature of the f1(1285) state
Decays of ¯ B 0 s and ¯ B 0 mesons into J / ψ π + π − π + π − final states, produced in p p collisio...
Decays of ¯ B 0 s and ¯ B 0 mesons into J / ψ π + π − π + π − final states, produced in p p collisio...
We evaluate the decay width for the processes f 1(1285) → π0 a 0(980) and f 1(1285) → π0 f 1(980)tak...
We investigate the decay of f1(1285)→πKK¯ with the assumption that the f1(1285) is dynamically gener...
AbstractWe investigate the decay of f1(1285)→πKK¯ with the assumption that the f1(1285) is dynamical...
AbstractWe investigate the decay of f1(1285)→πKK¯ with the assumption that the f1(1285) is dynamical...
We investigate the decay of f1(1285)→πKK¯ with the assumption that the f1(1285) is dynamically gener...
AbstractWe study the role of the f1(1285) resonance in the decays of J/ψ→ϕK¯K⁎ and J/ψ→ϕf1(1285). Th...
We investigate the decay of f1 (1285) → πK K bar with the assumption that the f1 (1285) is dynamical...
We study the K¯ p→ YKK¯ π reactions with K¯ = K¯ , K and Y= Σ , Σ , Λ , in the region of KK¯ π invar...
AbstractWe study the role of the f1(1285) resonance in the decays of J/ψ→ϕK¯K⁎ and J/ψ→ϕf1(1285). Th...
We study the role of the f1(1285) resonance in the decays of J/ψ→ϕK¯K⁎ and J/ψ→ϕf1(1285). The theore...
We show that the τ− decay into f1(1285)π−ντ is dominated by a triangle loop mechanism with K⁎, K¯⁎ a...
We evaluate the decay width for the processes f1(1285). p 0 a0(980) and f1(1285). p 0 f0(980) taking...
Decays of ¯B0s and ¯B0 mesons into J/ψ π+π−π+π− final states, produced in pp collisions at the LHC, ...
Decays of ¯ B 0 s and ¯ B 0 mesons into J / ψ π + π − π + π − final states, produced in p p collisio...
Decays of ¯ B 0 s and ¯ B 0 mesons into J / ψ π + π − π + π − final states, produced in p p collisio...
We evaluate the decay width for the processes f 1(1285) → π0 a 0(980) and f 1(1285) → π0 f 1(980)tak...
We investigate the decay of f1(1285)→πKK¯ with the assumption that the f1(1285) is dynamically gener...
AbstractWe investigate the decay of f1(1285)→πKK¯ with the assumption that the f1(1285) is dynamical...
AbstractWe investigate the decay of f1(1285)→πKK¯ with the assumption that the f1(1285) is dynamical...
We investigate the decay of f1(1285)→πKK¯ with the assumption that the f1(1285) is dynamically gener...
AbstractWe study the role of the f1(1285) resonance in the decays of J/ψ→ϕK¯K⁎ and J/ψ→ϕf1(1285). Th...
We investigate the decay of f1 (1285) → πK K bar with the assumption that the f1 (1285) is dynamical...
We study the K¯ p→ YKK¯ π reactions with K¯ = K¯ , K and Y= Σ , Σ , Λ , in the region of KK¯ π invar...
AbstractWe study the role of the f1(1285) resonance in the decays of J/ψ→ϕK¯K⁎ and J/ψ→ϕf1(1285). Th...
We study the role of the f1(1285) resonance in the decays of J/ψ→ϕK¯K⁎ and J/ψ→ϕf1(1285). The theore...
We show that the τ− decay into f1(1285)π−ντ is dominated by a triangle loop mechanism with K⁎, K¯⁎ a...
We evaluate the decay width for the processes f1(1285). p 0 a0(980) and f1(1285). p 0 f0(980) taking...
Decays of ¯B0s and ¯B0 mesons into J/ψ π+π−π+π− final states, produced in pp collisions at the LHC, ...
Decays of ¯ B 0 s and ¯ B 0 mesons into J / ψ π + π − π + π − final states, produced in p p collisio...
Decays of ¯ B 0 s and ¯ B 0 mesons into J / ψ π + π − π + π − final states, produced in p p collisio...
We evaluate the decay width for the processes f 1(1285) → π0 a 0(980) and f 1(1285) → π0 f 1(980)tak...