The $η(2225)$ observed by the BES Collaboration
| dc.creator | Li, De-Min | |
| dc.creator | Ma, Bing | |
| dc.date | 2008-03-02 | |
| dc.date | 2008-04-03 | |
| dc.date.accessioned | 2026-07-07T11:40:34Z | |
| dc.date.available | 2026-07-07T11:40:34Z | |
| dc.description | In the framework of the $^3P_0$ meson decay model, the strong decays of the $3 ^1S_0$ and $4 ^1S_0$ $s\bar{s}$ states are investigated. It is found that in the presence of the initial state mass being 2.24 GeV, the total widths of the $3 ^1S_0$ and $4 ^1S_0$ $s\bar{s}$ states are about 438 MeV and 125 MeV, respectively. Also, when the initial state mass varies from 2220 to 2400 MeV, the total width of the $4 ^1S_0$ $s\bar{s}$ state varies from about 100 to 132 MeV, while the total width of the $3 ^1S_0$ $s\bar{s}$ state varies from about 400 to 594 MeV. A comparison of the predicted widths and the experimental result of $(0.19\pm 0.03^{+0.04}_{-0.06})$ GeV, the width of the $η(2225)$ with a mass of $(2.24^{+0.03+0.03}_{-0.02-0.02})$ GeV recently observed by the BES Collaboration in the radiative decay $J/ψ\toγϕϕ\toγK^+K^-K^0_SK^0_L$, suggests that it would be very difficult to identify the $η(2225)$ as the $3 ^1S_0$ $s\bar{s}$ state, and the $η(2225)$ seams a good candidate for the $4 ^1S_0$ $s\bar{s}$ state. | |
| dc.description | 14 pages, 3 figures, typos corrected, Accepted by Physical Review D | |
| dc.identifier | https://arxiv.org/abs/0803.0106 | |
| dc.identifier | http://arxiv.org/abs/0803.0106 | |
| dc.identifier | Phys.Rev.D77:094021,2008 | |
| dc.identifier | doi:10.1103/PhysRevD.77.094021 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/200293 | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.title | The $η(2225)$ observed by the BES Collaboration | |
| dc.type | text |