On $Ω_{3c}NN$ and $Ω_{3c} Ω_{3c} N$ systems with HAL QCD potentials

Fuente: arXiv
Gespeichert in:
Bibliographische Detailangaben
Hauptverfasser: Filikhin, Igor, Kezerashvili, Roman Ya., Vlahovic, Branislav
Format: Preprint
Veröffentlicht: 2025
Schlagworte:
Online-Zugang:
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
_version_ 1866908515028697088
author Filikhin, Igor
Kezerashvili, Roman Ya.
Vlahovic, Branislav
author_facet Filikhin, Igor
Kezerashvili, Roman Ya.
Vlahovic, Branislav
contents This study employs the Faddeev formalism in configuration space to investigate the $Ω_{3c}NN$ cluster containing a triply charmed Omega baryon ($Ω_{3c}$). Using the recently reported HAL QCD $S$-wave $Ω_{3c}N$ potentials in the $^3S_1$ and $^5S_2$ channels, together with the MT-I--III nucleon--nucleon potential and neglecting the Coulomb force, we find no bound state for the $Ω_{3c}np$ system. We predict near-threshold resonances in the $J^π=5/2^{+}$ (maximal total spin) and $J^π=1/2^{+}$ (minimal total spin) states, with resonance energies of $1.1~\mathrm{MeV}$ below and $0.0~\mathrm{MeV}$ at the three-body breakup threshold, respectively, at Euclidean time $t/a = 16$. A similar analysis of the $Ω_{3c}Ω_{3c}N$ system likewise reveals no bound states, though a possible resonance is indicated. The short-distance behavior of the HAL QCD $Ω_{3c}N$ potential is also discussed.
format Preprint
id arxiv_https___arxiv_org_abs_2509_01902
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle On $Ω_{3c}NN$ and $Ω_{3c} Ω_{3c} N$ systems with HAL QCD potentials
Filikhin, Igor
Kezerashvili, Roman Ya.
Vlahovic, Branislav
Nuclear Theory
High Energy Physics - Lattice
This study employs the Faddeev formalism in configuration space to investigate the $Ω_{3c}NN$ cluster containing a triply charmed Omega baryon ($Ω_{3c}$). Using the recently reported HAL QCD $S$-wave $Ω_{3c}N$ potentials in the $^3S_1$ and $^5S_2$ channels, together with the MT-I--III nucleon--nucleon potential and neglecting the Coulomb force, we find no bound state for the $Ω_{3c}np$ system. We predict near-threshold resonances in the $J^π=5/2^{+}$ (maximal total spin) and $J^π=1/2^{+}$ (minimal total spin) states, with resonance energies of $1.1~\mathrm{MeV}$ below and $0.0~\mathrm{MeV}$ at the three-body breakup threshold, respectively, at Euclidean time $t/a = 16$. A similar analysis of the $Ω_{3c}Ω_{3c}N$ system likewise reveals no bound states, though a possible resonance is indicated. The short-distance behavior of the HAL QCD $Ω_{3c}N$ potential is also discussed.
title On $Ω_{3c}NN$ and $Ω_{3c} Ω_{3c} N$ systems with HAL QCD potentials
topic Nuclear Theory
High Energy Physics - Lattice
url https://arxiv.org/abs/2509.01902