Measurements of e + e − → K S 0 K ± π ∓ π 0 and K S 0 K ± π ∓ η at center-of-mass energies from 3.90 to 4.60 GeV

Utilizing 5.2 fb-1 e+e- annihilation data samples collected with the BESIII detector, we measure the cross sections of e+e- → K$0\atop{S}$K±$\pi$∓$\pi$0 and K$0\atop{S}$K±$\pi$∓η at center-of-mass energies from 3.90 to 4.60 GeV. In addition, we search for the charmonium-like resonance Y (4260) decay...

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Veröffentlicht in:Physical review. D 2019-01, Vol.99 (1), Article 012003
Hauptverfasser: Ablikim, M., Achasov, M. N., Ahmed, S., Albrecht, M., Alekseev, M., Amoroso, A., An, F. F., An, Q., Bai, Y., Bakina, O., Baldini Ferroli, R., Ban, Y., Begzsuren, K., Bennett, D. W., Bennett, J. V., Berger, N., Bertani, M., Bettoni, D., Bianchi, F., Boyko, I., Briere, R. A., Cai, H., Cai, X., Calcaterra, A., Cao, G. F., Cetin, S. A., Chai, J., Chang, J. F., Chang, W. L., Chelkov, G., Chen, G., Chen, H. S., Chen, J. C., Chen, M. L., Chen, P. L., Chen, S. J., Chen, Y. B., Cheng, W., Cibinetto, G., Cossio, F., Dai, H. L., Dai, J. P., Dbeyssi, A., Dedovich, D., Deng, Z. Y., Denig, A., Denysenko, I., Destefanis, M., De Mori, F., Ding, Y., Dong, C., Dong, J., Dong, L. Y., Dong, M. Y., Dou, Z. L., Du, S. X., Duan, P. F., Fan, J. Z., Fang, J., Fang, S. S., Fang, Y., Farinelli, R., Fava, L., Fegan, S., Feldbauer, F., Felici, G., Feng, C. Q., Fritsch, M., Fu, C. D., Fu, Y., Gao, Q., Gao, X. L., Gao, Y., Gao, Y. G., Gao, Z., Garillon, B., Garzia, I., Gilman, A., Goetzen, K., Gong, L., Gong, W. X., Gradl, W., Greco, M., Gu, L. M., Gu, M. H., Gu, Y. T., Guo, A. Q., Guo, L. B., Guo, R. P., Guo, Y. P., Guskov, A., Haddadi, Z., Han, S., Hao, X. Q., Harris, F. A., He, K. L., Heinsius, F. H., Held, T., Heng, Y. K., Hou, Z. L.
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Sprache:eng
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Zusammenfassung:Utilizing 5.2 fb-1 e+e- annihilation data samples collected with the BESIII detector, we measure the cross sections of e+e- → K$0\atop{S}$K±$\pi$∓$\pi$0 and K$0\atop{S}$K±$\pi$∓η at center-of-mass energies from 3.90 to 4.60 GeV. In addition, we search for the charmonium-like resonance Y (4260) decays into K$0\atop{S}$K±$\pi$∓$\pi$0 and K$0\atop{S}$K±$\pi$∓η, and Z$0,\atop{c}$± (3900) decays into K$0\atop{S}$K±∓$\pi$,0 and K$0\atop{S}$K±η. Corresponding upper limits are provided since no clear signal is observed.
ISSN:2470-0010
2470-0029
DOI:10.1103/PhysRevD.99.012003