6533b853fe1ef96bd12ac06e
RESEARCH PRODUCT
K¯-induced formation of thef0(980)anda0(980)resonances on proton targets
Ju-jun XieWei-hong LiangEulogio OsetEulogio Osetsubject
PhysicsUnitarityProton010308 nuclear & particles physicsHigh Energy Physics::Phenomenology0103 physical sciencesResonanceProduction (computer science)Atomic physics010306 general physics01 natural sciencesNuclear theoryBar (unit)description
We perform a calculation of the cross section for nine reactions induced by $\overline{K}$ scattering on protons. The reactions studied are ${K}^{\ensuremath{-}}p\ensuremath{\rightarrow}\mathrm{\ensuremath{\Lambda}}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}$, ${K}^{\ensuremath{-}}p\ensuremath{\rightarrow}{\mathrm{\ensuremath{\Sigma}}}^{0}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}$, ${K}^{\ensuremath{-}}p\ensuremath{\rightarrow}\mathrm{\ensuremath{\Lambda}}{\ensuremath{\pi}}^{0}\ensuremath{\eta}$, ${K}^{\ensuremath{-}}p\ensuremath{\rightarrow}{\mathrm{\ensuremath{\Sigma}}}^{0}{\ensuremath{\pi}}^{0}\ensuremath{\eta}$, ${K}^{\ensuremath{-}}p\ensuremath{\rightarrow}{\mathrm{\ensuremath{\Sigma}}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}\ensuremath{\eta}$, ${\overline{K}}^{0}p\ensuremath{\rightarrow}\mathrm{\ensuremath{\Lambda}}{\ensuremath{\pi}}^{+}\ensuremath{\eta}$, ${\overline{K}}^{0}p\ensuremath{\rightarrow}{\mathrm{\ensuremath{\Sigma}}}^{0}{\ensuremath{\pi}}^{+}\ensuremath{\eta}$, ${\overline{K}}^{0}p\ensuremath{\rightarrow}{\mathrm{\ensuremath{\Sigma}}}^{+}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}$, and ${\overline{K}}^{0}p\ensuremath{\rightarrow}{\mathrm{\ensuremath{\Sigma}}}^{+}{\ensuremath{\pi}}^{0}\ensuremath{\eta}$. We find that in the reactions producing ${\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}$, a clear peak for the ${f}_{0}(980)$ resonance is found, while no trace of ${f}_{0}(500)$ appears. Similarly, in the cases of $\ensuremath{\pi}\ensuremath{\eta}$ production, a strong peak is found for the ${a}_{0}(980)$ resonance, with the characteristic strong cusp shape. Cross sections and invariant mass distributions are evaluated which should serve, by comparing them with future data, to test the dynamics of the chiral unitary approach used for the evaluations and the nature of these resonances.
year | journal | country | edition | language |
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2016-03-24 | Physical Review C |