Pauli principle forbids $Ω_{QQQ}Ω_{QQQ}Ω_{QQQ}$ bound states

Fuente: arXiv
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Main Authors: Garcilazo, H., Valcarce, A.
Format: Preprint
Published: 2025
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author Garcilazo, H.
Valcarce, A.
author_facet Garcilazo, H.
Valcarce, A.
contents Lattice QCD studies have shown the attractive character of the $^1S_0$ $Ω_{QQQ}Ω_{QQQ}$, $Q=s,c,b$, interaction, predicting deeply bound states as the mass of the heavy quark increases. This has led to the question of the possible existence of bound states of more than two $Ω_{QQQ}$ baryons, in particular $Ω_{QQQ}Ω_{QQQ}Ω_{QQQ}$ bound states. We discuss how these states might not exist in nature in any flavor sector. The reason would be due to the simultaneous action of two consequences of the Pauli principle in the different partial waves: one at the baryon level, affecting the $^1S_0$ partial wave, and the other due to the quark substructure, affecting the $^5S_2$ partial wave.
format Preprint
id arxiv_https___arxiv_org_abs_2501_10276
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Pauli principle forbids $Ω_{QQQ}Ω_{QQQ}Ω_{QQQ}$ bound states
Garcilazo, H.
Valcarce, A.
High Energy Physics - Phenomenology
Nuclear Theory
Lattice QCD studies have shown the attractive character of the $^1S_0$ $Ω_{QQQ}Ω_{QQQ}$, $Q=s,c,b$, interaction, predicting deeply bound states as the mass of the heavy quark increases. This has led to the question of the possible existence of bound states of more than two $Ω_{QQQ}$ baryons, in particular $Ω_{QQQ}Ω_{QQQ}Ω_{QQQ}$ bound states. We discuss how these states might not exist in nature in any flavor sector. The reason would be due to the simultaneous action of two consequences of the Pauli principle in the different partial waves: one at the baryon level, affecting the $^1S_0$ partial wave, and the other due to the quark substructure, affecting the $^5S_2$ partial wave.
title Pauli principle forbids $Ω_{QQQ}Ω_{QQQ}Ω_{QQQ}$ bound states
topic High Energy Physics - Phenomenology
Nuclear Theory
url https://arxiv.org/abs/2501.10276