We show that the τ− decay into f1(1285)π−ντ is dominated by a triangle loop mechanism with K⁎, K¯⁎ and K (or K¯) as internal lines, which manifests a strong enhancement reminiscent of a nearby singularity present in the narrow K⁎ limit and the near K¯⁎K⁎ threshold of the internal K⁎ propagators. The f1(1285) is then produced by its coupling to the K⁎K¯ and K¯⁎K which is obtained from a previous model where this resonance was dynamically generated as a molecular K⁎K¯ (or K¯⁎K) state using the techniques of the chiral unitary approach. We make predictions for the f1π mass distribution which significantly deviates from the phase-space shape, due to the distortion caused by the triangle mechanism and the K⁎K¯ threshold. We find a good agreement...
We study the appearance of structures in the decay of the B− into K−π−D+s0(2317) and K−π−D+s1(2460) ...
We investigate the decay of f1(1285)→πKK¯ with the assumption that the f1(1285) is dynamically gener...
We study theoretically the decay τ-→ντP-A, with P- a π- or K- and A an axial-vector resonance b1(123...
We study the role of the f1(1285) resonance in the decays of J/ψ→ϕK¯K⁎ and J/ψ→ϕf1(1285). The theore...
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 Λc+→π0ϕp decay by considering a triangle singularity mechanism. In this mechanism, the ...
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...
We investigate the decay of f1 (1285) → πK K bar 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...
Within the chiral unitary approach, the axial-vector resonance K1(1270) has been predicted to manife...
We study for the first time the pΣ− → K−d and its time reversal reaction close to threshold and show...
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 study the appearance of structures in the decay of the B− into K−π−D+s0(2317) and K−π−D+s1(2460) ...
By looking at the pseudoscalar-vector meson spectra in the B¯→J/ψρK̄ and B¯→J/ψK̄∗π weak decays, we ...
We study the appearance of structures in the decay of the B− into K−π−D+s0(2317) and K−π−D+s1(2460) ...
We investigate the decay of f1(1285)→πKK¯ with the assumption that the f1(1285) is dynamically gener...
We study theoretically the decay τ-→ντP-A, with P- a π- or K- and A an axial-vector resonance b1(123...
We study the role of the f1(1285) resonance in the decays of J/ψ→ϕK¯K⁎ and J/ψ→ϕf1(1285). The theore...
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 Λc+→π0ϕp decay by considering a triangle singularity mechanism. In this mechanism, the ...
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...
We investigate the decay of f1 (1285) → πK K bar 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...
Within the chiral unitary approach, the axial-vector resonance K1(1270) has been predicted to manife...
We study for the first time the pΣ− → K−d and its time reversal reaction close to threshold and show...
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 study the appearance of structures in the decay of the B− into K−π−D+s0(2317) and K−π−D+s1(2460) ...
By looking at the pseudoscalar-vector meson spectra in the B¯→J/ψρK̄ and B¯→J/ψK̄∗π weak decays, we ...
We study the appearance of structures in the decay of the B− into K−π−D+s0(2317) and K−π−D+s1(2460) ...
We investigate the decay of f1(1285)→πKK¯ with the assumption that the f1(1285) is dynamically gener...
We study theoretically the decay τ-→ντP-A, with P- a π- or K- and A an axial-vector resonance b1(123...