From the $P^{N}_ψ$/$P^Λ_{ψs}$ to $\bar{T}^f_{cc}$: symmetry analysis to the interactions of the $(\bar{c}q)(\bar{c}q)$/$(ccq)(\bar{c}q)$/$(ccq)(ccq)$ di-hadron systems

Fuente: arXiv
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Auteurs principaux: Chen, Kan, Wang, Bo
Format: Preprint
Publié: 2024
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author Chen, Kan
Wang, Bo
author_facet Chen, Kan
Wang, Bo
contents We investigate the interactions of the $(\bar{c}q)(\bar{c}q)$/$(ccq)(\bar{c}q)$/$(ccq)(ccq)$ di-hadron systems based on a contact lagrangian possessing the SU(3) flavor and SU(2) spin symmetries. Under the assumptions of two scenarios for the $J^P$ quantum numbers of the $P_ψ^N(4440)$ and $P_ψ^N(4457)$ states, we obtain the parameters ($\tilde{g}_s$, $\tilde{g}_a$) introduced from this contact lagrangian. Then we include the SU(3) breaking effect by introducing a factor $g_x$, this quantity can be further constrained by the experimental mass of the $P_{ψs}^Λ(4338)$ state. We can reproduce the mass of the $T^f_{cc}(3875)$ state with the parameters extracted from the observed $P_ψ^N$ states, this consistency indicates a unified description of the di-hadron molecular states composed of two heavy-light hadrons. With the same parameters, we discuss the possible mass spectra of the $\bar{T}_{cc}^f$/$P_{ψc}^Λ$/$H_{Ω_{ccc}c}^Λ$ systems. Then we proceed to discuss the existences of the $\bar{T}_{cc\bar{s}}^θ$/$P_{ψcs}^N$/$H_{Ω_{ccc}cs}^N$ states by investigating the SU(3) breaking effects. Our results show that the states in the $\bar{T}_{cc\bar{s}}^θ$/$P_{ψcs}^N$ systems can hardly form bound states, while the states in the $H_{Ω_{ccc}cs}^N$ system can form bound states due to their larger reduced masses.
format Preprint
id arxiv_https___arxiv_org_abs_2407_01185
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle From the $P^{N}_ψ$/$P^Λ_{ψs}$ to $\bar{T}^f_{cc}$: symmetry analysis to the interactions of the $(\bar{c}q)(\bar{c}q)$/$(ccq)(\bar{c}q)$/$(ccq)(ccq)$ di-hadron systems
Chen, Kan
Wang, Bo
High Energy Physics - Phenomenology
High Energy Physics - Experiment
We investigate the interactions of the $(\bar{c}q)(\bar{c}q)$/$(ccq)(\bar{c}q)$/$(ccq)(ccq)$ di-hadron systems based on a contact lagrangian possessing the SU(3) flavor and SU(2) spin symmetries. Under the assumptions of two scenarios for the $J^P$ quantum numbers of the $P_ψ^N(4440)$ and $P_ψ^N(4457)$ states, we obtain the parameters ($\tilde{g}_s$, $\tilde{g}_a$) introduced from this contact lagrangian. Then we include the SU(3) breaking effect by introducing a factor $g_x$, this quantity can be further constrained by the experimental mass of the $P_{ψs}^Λ(4338)$ state. We can reproduce the mass of the $T^f_{cc}(3875)$ state with the parameters extracted from the observed $P_ψ^N$ states, this consistency indicates a unified description of the di-hadron molecular states composed of two heavy-light hadrons. With the same parameters, we discuss the possible mass spectra of the $\bar{T}_{cc}^f$/$P_{ψc}^Λ$/$H_{Ω_{ccc}c}^Λ$ systems. Then we proceed to discuss the existences of the $\bar{T}_{cc\bar{s}}^θ$/$P_{ψcs}^N$/$H_{Ω_{ccc}cs}^N$ states by investigating the SU(3) breaking effects. Our results show that the states in the $\bar{T}_{cc\bar{s}}^θ$/$P_{ψcs}^N$ systems can hardly form bound states, while the states in the $H_{Ω_{ccc}cs}^N$ system can form bound states due to their larger reduced masses.
title From the $P^{N}_ψ$/$P^Λ_{ψs}$ to $\bar{T}^f_{cc}$: symmetry analysis to the interactions of the $(\bar{c}q)(\bar{c}q)$/$(ccq)(\bar{c}q)$/$(ccq)(ccq)$ di-hadron systems
topic High Energy Physics - Phenomenology
High Energy Physics - Experiment
url https://arxiv.org/abs/2407.01185