The possible members of the $5^1{S}_0$ meson nonet

Abstract

The strong decays of the $5^1{S}_0$ $q\bar{q}$ states are evaluated in the ${}^3{P}_0$ model with two types of space wave functions. Comparing the model expectations with the experimental data for the $\pi (2360)$, $\eta (2320)$, $X(2370)$, and $X(2500)$, we suggest that the $\pi (2360)$, $\eta (2320)$, and $X(2500)$ can be assigned as the members of the $5^1{S}_0$ meson nonet, while the $5^1{S}_0$ assignment for the $X(2370)$ is not favored by its width. The $5^1{S}_0$ kaon is predicted to have a mass of about 2418 MeV and a width of about 163 MeV or 225 MeV.

arXiv comment10 pages, 5 figures, version accepted by Eur. Phys. J. C

References in corpus (40)

• The glueball spectrum from an anisotropic lattice study
• Higher Charmonia
• Glueball Spectrum and Matrix Elements on Anisotropic Lattices
• On the Mechanism of Open-Flavor Strong Decays
• Higher Quarkonia
• Systematics of q anti-q states in the (n,M^2) and (J,M^2) planes
• Mass spectra and Regge trajectories of light mesons in the relativistic quark model
• Low lying axial-vector mesons as dynamically generated resonances
• Dynamics and Decay of Heavy-Light Hadrons
• Strong Decays of Strange Quarkonia
• The $\xi (2220)$ Revistited
• $D_{sJ}(2860)$ and $D_{sJ}(2715)$
• The newly observed open-charm states in quark model
• Y(2175): Distinguish Hybrid State from Higher Quarkonium
• Excited bottom and bottom-strange mesons in the quark model
• Clues for the existence of two $K_1(1270)$ resonances
• On the glueball spectrum in O(a)-improved lattice QCD
• Partial wave analysis of pbar-p annihilation channels in flight with I=1, C=+1
• Categorizing resonances X(1835), X(2120) and X(2370) in the pseudoscalar meson family
• Coupled-Channel Effects for the Bottomonium with Realistic Wave Functions
• Systematics of quark-antiquark states and scalar exotic mesons
• Low-lying even parity meson resonances and spin-flavor symmetry
• Understanding the charmed states recently observed by the LHCb and BaBar Collaborations in the quark model
• Implication of BaBar's new data on the $D_{s1}(2710)$ and $D_{sJ}(2860)$
• $X(1835)$ and $\eta (1760)$ observed by the BES Collaboration
• Canonical interpretation of the ${\eta }_2(1870)$
• Understanding masses of $c\bar{s}$ states in Regge phenomenology
• $X(1835)$ and the New Resonances $X(2120)$ and $X(2370)$ Observed by the BES Collaboration
• The $\eta (2225)$ observed by the BES Collaboration
• Towards the assignment for the $4^1{S}_0$ meson nonet
• Strong decays of the higher isovector scalar mesons
• Strong decays of the $X(2500)$ newly observed by the BESIII Collaboration
• On the nature of the $π_2(1880)
• A partial wave analysis of pbar-p -> eta-eta-pizero
• Constructing new pseudoscalar meson nonets with the observed $X(2100)$, $X(2500)$, and $\eta (2225)$
• Systematics of quark-antiquark states: where are the lightest glueballs?
• Systematics of q anti-q states, scalar mesons and glueball
• Analysis of the X(1835) and related baryonium states with Bethe-Salpeter equation
• Systematization of tensor mesons and the determination of the $2^{++}$ glueball
• Effects of Flavor-dependent $q\bar{q}$ Annihilation on the Mixing Angle of the Isoscalar Octet-Singlet and Schwinger's Nonet Mass Formula

Cited by in corpus (11)

• Mass spectrum and strong decays of strangeonium in a constituent quark model
• $S$- and $P$-wave fully-strange tetraquark states from QCD sum rules
• Concavity of the meson Regge trajectories
• Canonical interpretation of the $X(4140)$ state within the ${}^3{P}_0$ model
• Possible Assignment of Excited Light ${}^3{S}_1$ Vector Mesons
• QCD sum rule studies on the $ss\bar{s}\bar{s}$ tetraquark states of $J^{PC}=0^{-+}$
• Assignments of the $Y(2040)$, $\rho (1900)$, and $\rho (2150)$ in the quark model
• A new decay mode of higher charmonium
• The assignments of the $B_s$ mesons within the screened potential model and ${}^3{P}_0$ model
• The possible assignments of the scalar $K_0^{\ast }(1950)$ and $K_0^{\ast }(2130)$ within the ${}^3{P}_0$ model
• Strangeonium spectrum with the screening effects and interpretation of $h_1(1911)$ and $X(2300)$ observed by BESIII