6533b82efe1ef96bd1292fe7
RESEARCH PRODUCT
Anomalous enhancement of the isospin-violating Λ(1405) production by a triangle singularity in Λc→π+π0π0Σ0
L. R. DaiL. R. DaiR. PavaoEulogi OsetS. Sakaisubject
Physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHadronLambda01 natural sciencesLoop (topology)SingularityIsospin0103 physical sciencesMass spectrumProduction (computer science)Invariant mass010306 general physicsMathematical physicsdescription
The decay of ${\mathrm{\ensuremath{\Lambda}}}_{c}^{+}$ into ${\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{0}\mathrm{\ensuremath{\Lambda}}(1405)$ with the $\mathrm{\ensuremath{\Lambda}}(1405)$ decay into ${\ensuremath{\pi}}^{0}{\mathrm{\ensuremath{\Sigma}}}^{0}$ through a triangle diagram is studied. This process is initiated by ${\mathrm{\ensuremath{\Lambda}}}_{c}^{+}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\overline{K}}^{*}N$, and then the ${\overline{K}}^{*}$ decays into $\overline{K}\ensuremath{\pi}$ and $\overline{K}N$ produce the $\mathrm{\ensuremath{\Lambda}}(1405)$ through a triangle loop containing ${\overline{K}}^{*}N\overline{K}$ which develops a singularity around 1890 MeV. This process is prohibited by the isospin symmetry, but the decay into this channel is enhanced by the contribution of the triangle diagram, which is sensitive to the mass of the internal particles. We find a narrow peak in the ${\ensuremath{\pi}}^{0}{\mathrm{\ensuremath{\Sigma}}}^{0}$ invariant mass distribution, which originates from the $\mathrm{\ensuremath{\Lambda}}(1405)$ amplitude, but is tied to the mass differences between the charged and neutral $\overline{K}$ or $N$ states. The observation of the unavoidable peak of the triangle singularity in the isospin-violating $\mathrm{\ensuremath{\Lambda}}(1405)$ production would provide further support for the hadronic molecular picture of the $\mathrm{\ensuremath{\Lambda}}(1405)$ and further information on the $\overline{K}N$ interaction.
year | journal | country | edition | language |
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2018-06-05 | Physical Review D |