Search for η c ( 2 S ) → K + K − η ′ decay

Using ( 2.712 ± 0.014 ) × 10 9 ψ ( 2 S ) events collected with the BESIII detector operating at the BEPCII, we search for the η c ( 2 S ) → K + K − η ′ decay. Its decay branching fraction is measured to be ( 11.11 ± 4.6 7 ( stat ) ± 1.8 2 ( syst ) ± 4.2 4 ( extr ) ) × 10 − 4 , where the first uncert...

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Veröffentlicht in:Physical review. D 2025-01, Vol.111 (1), Article 012004
Hauptverfasser: Ablikim, M., Achasov, M. N., Adlarson, P., Afedulidis, O., Ai, X. C., Aliberti, R., Amoroso, A., An, Q., Bai, Y., Bakina, O., Balossino, I., Ban, Y., Bao, H.-R., Batozskaya, V., Begzsuren, K., Berger, N., Berlowski, M., Bertani, M., Bettoni, D., Bianchi, F., Bianco, E., Bortone, A., Boyko, I., Briere, R. A., Brueggemann, A., Cai, H., Cai, X., Calcaterra, A., Cao, G. F., Cao, N., Cetin, S. A., Chang, J. F., Che, G. R., Chelkov, G., Chen, C., Chen, C. H., Chen, Chao, Chen, G., Chen, H. S., Chen, H. Y., Chen, M. L., Chen, S. J., Chen, S. L., Chen, S. M., Chen, T., Chen, X. R., Chen, X. T., Chen, Y. B., Chen, Y. Q., Chen, Z. J., Chen, Z. Y., Choi, S. K., Cibinetto, G., Cossio, F., Cui, J. J., Dai, H. L., Dai, J. P., Dbeyssi, A., de Boer, R. E., Dedovich, D., Deng, C. Q., Deng, Z. Y., Denig, A., Denysenko, I., Destefanis, M., De Mori, F., Ding, B., Ding, X. X., Ding, Y., Dong, J., Dong, L. Y., Dong, M. Y., Dong, X., Du, M. C., Du, S. X., Duan, Y. Y., Duan, Z. H., Egorov, P., Fan, Y. H., Fang, J., Fang, S. S., Fang, W. X., Fang, Y., Fang, Y. Q., Farinelli, R., Fava, L., Feldbauer, F., Felici, G., Feng, C. Q., Feng, J. H., Feng, Y. T., Fritsch, M., Fu, C. D., Fu, J. L., Fu, Y. W., Gao, H., Gao, X. B., Gao, Y. N.
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Sprache:eng
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Zusammenfassung:Using ( 2.712 ± 0.014 ) × 10 9 ψ ( 2 S ) events collected with the BESIII detector operating at the BEPCII, we search for the η c ( 2 S ) → K + K − η ′ decay. Its decay branching fraction is measured to be ( 11.11 ± 4.6 7 ( stat ) ± 1.8 2 ( syst ) ± 4.2 4 ( extr ) ) × 10 − 4 , where the first uncertainty is statistical, the second is systematic, and the third uncertainty is from the branching fraction of the ψ ( 2 S ) → γ η c ( 2 S ) decay. The statistical significance is 2.8 σ . The upper limit on the product branching fraction B [ ψ ( 2 S ) → γ η c ( 2 S ) ] × B [ η c ( 2 S ) → K + K − η ′ ] is set to be 0.94 × 10 − 6 at 90% confidence level. In addition, the branching fractions of χ c 1 → K + K − η ′ and χ c 2 → K + K − η ′ are updated to be ( 8.48 ± 0.10 ( stat ) ± 0.47 ( syst ) ) × 10 − 4 and ( 1.53 ± 0.04 ( stat ) ± 0.08 ( syst ) ) × 10 − 4 , respectively. The precision is improved by twofold.
ISSN:2470-0010
2470-0029
DOI:10.1103/PhysRevD.111.012004