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J. A. Marsé-Valera

Publications and source records attributed to J. A. Marsé-Valera.

2 recordsLinked to original sources

Double strangeness pentaquarks and other exotic hadrons in the $Ξ_b \to Ξ J/Ψ ϕ$ decay

We study the possibility that four $Ξ$ resonances $(Ξ(1620)$, $Ξ(1690)$, $Ξ(1820)$, $Ξ(1950))$ could correspond to pentaquark states, in the form of meson-baryon bound systems. We also explore the possible existence of doubly strange pentaquarks with hidden charm $(P_{css})$ and find two candidates structured in a similar form, at energies of $4493~{\rm MeV}$ and $4630~{\rm MeV}$. The meson-baryon interaction is built from t-channel meson exchange processes which are evaluated using effective Lagrangians. Moreover we analyse the $Ξ_b\toΞ~J/ψ~ϕ$ decay process, which permits exploring the existence of the heavy double strange pentaquark, as well as other exotic hadrons, in the three different two-body invariant mass spectra of the emitted particles. In the $J/ψϕ$ mass spectrum, we analyse the nature of the $X(4140)$ and $X(4160)$ resonances. In the $J/ψΞ$ invariant mass spectrum, we study the signal produced by the doubly strange pentaquark, where we conclude that it has a good chance to be detected in this reaction if its mass is around $4580-4680~{\rm MeV}$. Finally, in the $ϕΞ$ spectrum we study the likelihood to detect the $Ξ(2500)$ state.

hep-ph↗

Double strangeness molecular-type pentaquarks from coupled channel dynamics

The existence of pentaquarks with strangeness content zero and one are major discoveries of the latest years in hadron physics. Most of these states can be understood as hadronic molecules and were predicted prior to their discovery within a model based on unitarized meson-baryon amplitudes obtained from vector meson exchange interactions. Contrary to earlier statements, we show this model to also predict the existence of pentaquarks with double strangeness, at about 4500 MeV and 4600 MeV, which are generated in a very specific and unique mechanism, via an attraction induced by a strong coupling between the two heaviest meson-baryon states.

hep-ph↗