We study the influence of the D*s0(2317)+ resonance in the decay Bc → J/ψKD. In this process, we consider that the Bc meson decays first into J/ψ and the quark pair cs̄, and then the quark pair hadronizes into DK or Dsη components. The final state interaction, generating the D*s0(2317)+ resonance, is described by the chiral heavy meson unitary approach. With the parameters chosen in order to match the pole position of the D*s0(2317)+, we obtain the DK invariant mass distribution of the decay Bc → J/ψDK, and also the rate for Bc → J/ψD*s0(2317). We predict the ratio of these two magnitudes. This decay mechanism has not been measured yet, and it would provide insight about the nature of this resonance
A broad peaking structure is observed in the dimuon spectrum of B[superscript +]→K[superscript +]μ[s...
We present Dalitz plot analyses for the decays of B mesons to D-D0K+ and D¯0D0K+. We report the obse...
We present a study of resonances in exclusive decays of B mesons to ¯¯¯ D ( * ) D ( * ) K . We repor...
AbstractWe describe the B0 and Bs0 decays into J/ψ f0(500) and J/ψ f0(980) by taking into account th...
We study the semileptonic B-s and B decays into the D-s0*(2317) and D-0*(2400) resonances, respectiv...
We present a study of resonances in exclusive decays of B mesons to D̄(*)D(*)K. We report the observ...
Using the simple model that the amplitude for η′ → η π π is dominated by the δ (970) resonance we fi...
A broad peaking structure is observed in the dimuon spectrum of B +→K+μ+μ- decays in the kinematic r...
We study the reactions J/ψ → $$ \bar \Lambda $$ K - p and J/ψ → $$ \bar \Lambda $$π+π-Λ with a uni...
A broad peaking structure is observed in the dimuon spectrum of B+→K+μ+μ− decays in the kinematic re...
A broad peaking structure is observed in the dimuon spectrum of B+\u2192K+\u3bc+\u3bc 12 decays in t...
We present a study of resonances in exclusive decays of B mesons to D̅ (*)D(*)K. We report the obser...
The decays D* → Dπ and D* → Dγ are well described by heavy meson chiral perturbation theory. With th...
We present Dalitz plot analyses for the decays of B mesons to D-D0K+ and D¯0D0K+. We report the obse...
We study the decay widths of the narrow resonances $D_{sj}^*(2317)$ and $D_{sj}(2460)$ in the chiral...
A broad peaking structure is observed in the dimuon spectrum of B[superscript +]→K[superscript +]μ[s...
We present Dalitz plot analyses for the decays of B mesons to D-D0K+ and D¯0D0K+. We report the obse...
We present a study of resonances in exclusive decays of B mesons to ¯¯¯ D ( * ) D ( * ) K . We repor...
AbstractWe describe the B0 and Bs0 decays into J/ψ f0(500) and J/ψ f0(980) by taking into account th...
We study the semileptonic B-s and B decays into the D-s0*(2317) and D-0*(2400) resonances, respectiv...
We present a study of resonances in exclusive decays of B mesons to D̄(*)D(*)K. We report the observ...
Using the simple model that the amplitude for η′ → η π π is dominated by the δ (970) resonance we fi...
A broad peaking structure is observed in the dimuon spectrum of B +→K+μ+μ- decays in the kinematic r...
We study the reactions J/ψ → $$ \bar \Lambda $$ K - p and J/ψ → $$ \bar \Lambda $$π+π-Λ with a uni...
A broad peaking structure is observed in the dimuon spectrum of B+→K+μ+μ− decays in the kinematic re...
A broad peaking structure is observed in the dimuon spectrum of B+\u2192K+\u3bc+\u3bc 12 decays in t...
We present a study of resonances in exclusive decays of B mesons to D̅ (*)D(*)K. We report the obser...
The decays D* → Dπ and D* → Dγ are well described by heavy meson chiral perturbation theory. With th...
We present Dalitz plot analyses for the decays of B mesons to D-D0K+ and D¯0D0K+. We report the obse...
We study the decay widths of the narrow resonances $D_{sj}^*(2317)$ and $D_{sj}(2460)$ in the chiral...
A broad peaking structure is observed in the dimuon spectrum of B[superscript +]→K[superscript +]μ[s...
We present Dalitz plot analyses for the decays of B mesons to D-D0K+ and D¯0D0K+. We report the obse...
We present a study of resonances in exclusive decays of B mesons to ¯¯¯ D ( * ) D ( * ) K . We repor...