λ and ρ Regge trajectories for hidden bottom and charm tetraquarks ( Q q ) ( Q ¯ q ¯ ′ )

We propose the Regge trajectory relations for the heavy tetraquarks ( Q q ) ( Q ¯ q ¯ ′ ) ( Q = b , c ; q , q ′ = u , d , s ) with hidden bottom and charm. By employing the new relations, both the λ -trajectories and the ρ -trajectories for the tetraquarks ( Q q ) ( Q ¯ q ¯ ′ ) can be discussed. The...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
Veröffentlicht in:Physical review. D 2024-10, Vol.110 (7), Article 074039
Hauptverfasser: Xie, Jia-Qi, Song, He, Feng, Xia, Chen, Jiao-Kai
Format: Artikel
Sprache:eng
Online-Zugang:Volltext
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
Beschreibung
Zusammenfassung:We propose the Regge trajectory relations for the heavy tetraquarks ( Q q ) ( Q ¯ q ¯ ′ ) ( Q = b , c ; q , q ′ = u , d , s ) with hidden bottom and charm. By employing the new relations, both the λ -trajectories and the ρ -trajectories for the tetraquarks ( Q q ) ( Q ¯ q ¯ ′ ) can be discussed. The masses of the λ -mode excited states and the ρ -mode excited states are estimated, and they agree with other theoretical predictions. We show that the behaviors of the ρ -trajectories are different from those of the λ -trajectories. The ρ -trajectories behave as M ∼ x ρ 1 / 2 ( x ρ = n r , l ) while the λ -trajectories behave as M ∼ x λ 2 / 3 ( x λ = N r , L ) . Moreover, the Regge trajectory behaviors for other types of tetraquarks are investigated based on the spinless Salpeter equation. We show that both the λ -trajectories and the ρ -trajectories are concave downward in the ( M 2 , x ) plane. The Regge trajectories for the tetraquarks containing the light diquark and/or the light antidiquark also are concave in the ( M 2 , x ) plane when the masses of the light constituents are included and the confining potential is linear.
ISSN:2470-0010
2470-0029
DOI:10.1103/PhysRevD.110.074039