作者：
Ji, Hong-Tao;Lu, Yu-Han;Liu, Yan-Ting;Huang, Yu-Lin;Tian, Jiang-Feng;...
期刊：
中国化学快报：英文版,2025年36(2):110568 ISSN：1001-8417
通讯作者：
Zhang, YH;He, WM
作者机构：
[Liu, Yan-Ting; Liu, Feng; Ji, Hong-Tao; Huang, Yu-Lin; Zhang, Yong-Hong] Univ South China, Affiliated Nanhua Hosp, Hengyang Med Sch, Dept Ophthalmol, Hengyang 421001, Peoples R China.;[Zeng, Yan-Yan; Lu, Yu-Han; He, Wei-Min; Tian, Jiang-Feng; Ji, Hong-Tao; He, WM] Univ South China, Sch Chem & Chem Engn, Hengyang 421001, Peoples R China.;[Yang, Hai-Yan] Cent South Univ, Hunan Canc Hosp, Affiliated Canc Hosp,Xiangya Sch Med, Dept Lung Canc & Gastroenterol, Changsha 410013, Peoples R China.
通讯机构：
[Zhang, YH ; He, WM ] U;Univ South China, Affiliated Nanhua Hosp, Hengyang Med Sch, Dept Ophthalmol, Hengyang 421001, Peoples R China.;Univ South China, Sch Chem & Chem Engn, Hengyang 421001, Peoples R China.
关键词：
Dual catalysis;Semiconductor;Chlorine;Redox catalyst;Hydrogen atom transfer
摘要：
The first example of Nd@C3N4-photoredox/chlorine dual catalyzed alkylation with unactivated alkanes as the alkyl sources has been developed, which allows for the synthesis of various 4-alkylated cyclic sulfonyl ketimines. In this process, chlorine functions as both a redox and hydrogen atom transfer catalyst. The synergism of the reversible Nd2+/Nd3+ and Cl¯/Cl˙ redox pairs significantly enhances overall photocatalytic efficiency. The in vitro anticancer activity of 4-alkylated products was evaluated by using the CCK8 assay against both human choroidal melanoma (MUM-2B) and lung cancer (A549) cell. Compound 3da showed approximately triple the potency of 5-fluorouracil.
The first example of Nd@C3N4-photoredox/chlorine dual catalyzed alkylation with unactivated alkanes as the alkyl sources has been developed, which allows for the synthesis of various 4-alkylated cyclic sulfonyl ketimines. In this process, chlorine functions as both a redox and hydrogen atom transfer catalyst. The synergism of the reversible Nd2+/Nd3+ and Cl¯/Cl˙ redox pairs significantly enhances overall photocatalytic efficiency. The in vitro anticancer activity of 4-alkylated products was evaluated by using the CCK8 assay against both human choroidal melanoma (MUM-2B) and lung cancer (A549) cell. Compound 3da showed approximately triple the potency of 5-fluorouracil.
作者机构：
[Yu, B. X.; Yu, G.; Hu, T.; Ning, Z.; Zhang, P.; Wen, S. P.; Shi, X.; Sun, G. X.; Ma, M. M.; Guskov, A.; Chen, T.; Nikolaev, I. B.; Hou, X. T.; Zhu, Z. A.; Xu, G. F.; Wang, K.; Zhou, L. P.; Heng, Y. K.; Ji, Q.; Zhang, J. W.; Chen, Z. Y.; Rong, G.; Guan, C. Y.; Qi, F. Z.; Wang, Y. F.; Wang, L. L.; Ouyang, Q.; Jiang, D.; Liao, Y. P.; Zhang, A. Q.; Ji, X. B.; Qian, S.; Dong, M. Y.; Fang, S. S.; Chang, J. F.; Liu, Z. A.; Yang, T.; Yan, X. Q.; Ma, L. L.; Sun, Z. Q.; Han, T. T.; Wu, J. F.; Rivetti, A.; Sun, S. S.; Ding, B.; Fu, C. D.; Zhang, Y.; Lou, X. C.; Lin, T.; Zhang, B. X.; Xing, T. Y.; Cao, G. F.; Ji, W.; Wu, L. H.; Zhao, Y. B.; Fu, Y. W.; Zheng, J. P.; Jiang, X. S.; Kiuchi, R.; Fang, Y. Q.; Gu, M. H.; Lu, Y. P.; Dong, L. Y.; Zhang, H. Q.; Zhao, G.; Wu, L. J.; Li, L. J.; Yuan, Y.; Lu, X. L.; Wu, Z.; Fang, Y.; Luo, X. L.; Chelkov, G.; Ji, X. L.; Zhang, X. M.; Li, X. Y.; Li, L. K.; Li, H. B.; Liu, F.; Liang, H.; Huang, Y. P.; Zhang, J. Y.; Zhao, L.; Yin, J. H.; Yang, Y. F.; Batozskaya, V.; Song, W. M.; Chen, X. T.; Zhang, J. Z.; He, K. L.; Chen, G.; Ablikim, M.; Liu, C. X.; Li, X.; Zhu, K.; Zhao, J. Z.; Mao, Z. P.; Xiao, S. Y.; Fava, L.; Lu, J. G.; Liu, P. L.; Jing, M. Q.; Sun, H. K.; Chen, Y. B.; Du, M. C.; Wang, Z.; Ablikim, M; Zhao, J. Y.; Dong, J.; Shi, J. Y.; Zhemchugov, A.; Yuan, C. Z.; Tang, G. Y.; Yuan, S. C.; Zhang, H. Y.; Chen, M. L.; Zhang, Z. H.; Hou, G. Y.; Shen, H. F.; Shao, L. G.; Hou, Z. L.; Sun, Y. Z.; Liu, B. J.; Xiang, B. H.; Zhu, K. J.; Liu, H. M.; Xu, C. F.; Ma, H. L.; Dedovich, D.; Ye, M.; Xie, Y. G.; Chen, H. S.; Cao, N.; Ma, X. T.; Deng, Z. Y.; Ma, Q. M.; Wang, Z. Y.; Cai, X.; Zhang, Y. H.; Ma, R. Q.; Zheng, W. J.; Zou, J. H.; Liu, J. Y.; Wang, X. N.; Kui, X.; Li, W. G.; Wang, Y. Q.; Mo, X. H.; Fang, J.; Li, Q. M.; Shen, X. Y.; Ma, X. Y.; Hu, H. M.; Li, K.; Gong, W. X.; Xu, W.; Hu, Y.; Wang, B.; Zhang, B. L.; Ma, J. L.; Yang, Y. X.; Miao, H.; Zhang, S. H.; Li, F.; Lu, Z. H.; Yang, H. X.; Qin, Z. H.; Li, G.; Ping, R. G.; Sarantsev, A.; Qiu, J. F.; Zhang, Z. D.; Zhang, H. C.; Dai, H. L.; Li, W. D.; Fang, W. X.; Zeng, Y. J.] Inst High Energy Phys, Beijing 100049, Peoples R China.;[Achasov, M. N.; Nikolaev, I. B.; Muchnoi, N. Yu.] Budker Inst Nucl Phys SB RAS BINP, Novosibirsk 630090, Russia.;[Adlarson, P.; Wolke, M.; Schoenning, K.; Johansson, T.; Kupsc, A.; Thoren, V.] Uppsala Univ, Box 516, SE-75120 Uppsala, Sweden.;[Afedulidis, O.; Fritsch, M.; Heinsius, F. H.; Kuessner, M.; Hanisch, F.; Pelizaeus, M.; Kopf, B.; Wollenberg, L.; Holtmann, T.; de Boer, R. E.; Feldbauer, F.; Wiedner, U.; Holzken, F.] Bochum Ruhr Univ, D-44780 Bochum, Germany.;[Ai, X. C.; Zhang, Y. T.; Qiao, X. K.; Ke, B. C.; Zhao, S. J.; Yan, W. C.; Ge, L.; Yu, Y. C.; Li, D. M.; Du, S. X.; Zhang, H.; Zhang, J.; Liu, Y.] Zhengzhou Univ, Zhengzhou 450001, Peoples R China.
通讯机构：
[Ablikim, M ] I;Inst High Energy Phys, Beijing 100049, Peoples R China.
摘要：
The beta decay of the lightest charmed baryon.+ c provides unique insights into the fundamental mechanism of strong and electro-weak interactions, serving as a testbed for investigating non-perturbative quantum chromodynamics and constraining the Cabibbo-Kobayashi-Maskawa (CKM) matrix parameters. This article presents the first observation of the Cabibbosuppressed decay Lambda(+) (c) -> ne(+)v(e), utilizing 4.5 fb(-1) of electron-positron annihilation data collected with the BESIII detector. A novel Graph Neural Network based technique effectively separates signals from dominant backgrounds, notably Lambda(+) (c) -> Lambda e(+)v(e), achieving a statistical significance exceeding 10s. The absolute branching fraction ismeasured to be (3.57 +/- 0.34(stat.)+/- 0.14(syst).) x 10(-3). For the first time, the CKM matrix element |V-cd| is extracted via a charmed baryon decay as 0:208 +/- 0:011(exp): +/- 0:007(LQCD) +/- 0:001 tau(+)(Lambda) (c). This work highlights a new approach to further understand fundamental interactions in the charmed baryon sector, and showcases the power ofmodernmachine learning techniques in experimental high-energy physics.
作者机构：
[Yu, B. X.; Yu, G.; Hu, T.; Ning, Z.; Zhang, P.; Wen, S. P.; Shi, X.; Sun, G. X.; Ma, M. M.; Chen, T.; Hou, X. T.; Zhu, Z. A.; Xu, G. F.; Wang, K.; Zhou, L. P.; Heng, Y. K.; Ji, Q.; Zhang, J. W.; Chen, Z. Y.; Rong, G.; Guan, C. Y.; Qi, F. Z.; Wang, Y. F.; Wang, L. L.; Ouyang, Q.; Jiang, D.; Che, Y. Z.; Liao, Y. P.; Zhang, A. Q.; Ji, X. B.; Qian, S.; Dong, M. Y.; Fang, S. S.; Chang, J. F.; Liu, Z. A.; Yang, T.; Yan, X. Q.; Sun, Z. Q.; Han, T. T.; Wu, J. F.; Sun, S. S.; Ding, B.; Fu, C. D.; Zhang, Y.; Lou, X. C.; Lin, T.; Zhang, B. X.; Xing, T. Y.; Cao, G. F.; Ji, W.; Wu, L. H.; Zhao, Y. B.; Fu, Y. W.; Zheng, J. P.; Jiang, X. S.; Kiuchi, R.; Fang, Y. Q.; Gu, M. H.; Lu, Y. P.; Dong, L. Y.; Zhang, H. Q.; Zhao, G.; Wu, L. J.; Li, L. J.; Yuan, Y.; Lu, X. L.; Wu, Z.; Fang, Y.; Luo, X. L.; Ji, X. L.; Zhang, X. M.; Li, X. Y.; Li, L. K.; Li, H. B.; Liu, F.; Liang, H.; Huang, Y. P.; Zhang, J. Y.; Zhao, L.; Yin, J. H.; Yang, Y. F.; Batozskaya, V.; Song, W. M.; Chen, X. T.; Zhang, J. Z.; He, K. L.; Chen, G.; Ablikim, M.; Liu, C. X.; Li, X.; Zhu, K.; Liu, H. H.; Zhao, J. Z.; Mao, Z. P.; Xiao, S. Y.; Lu, J. G.; Liu, P. L.; Jing, M. Q.; Sun, H. K.; Chen, Y. B.; Du, M. C.; Wang, Z.; Ablikim, M; Zhao, J. Y.; Dong, J.; Shi, J. Y.; Ruan, M. Q.; Yuan, C. Z.; Tang, G. Y.; Yuan, S. C.; Zhang, H. Y.; Chen, M. L.; Zhang, Z. H.; Hou, G. Y.; Shen, H. F.; Shao, L. G.; Hou, Z. L.; Sun, Y. Z.; Liu, B. J.; Xiang, B. H.; Zhu, K. J.; Liu, H. M.; Xu, C. F.; Ma, H. L.; Ye, M.; Xie, Y. G.; Chen, H. S.; Cao, N.; Ma, X. T.; Deng, Z. Y.; Ma, Q. M.; Wang, Z. Y.; Cai, X.; Zhang, Y. H.; Ma, R. Q.; Zheng, W. J.; Zou, J. H.; Liu, J. Y.; Wang, X. N.; Kui, X.; Li, W. G.; Wang, Y. Q.; Mo, X. H.; Fang, J.; Li, Q. M.; Shen, X. Y.; Ma, X. Y.; Hu, H. M.; Li, K.; Gong, W. X.; Xu, W.; Hu, Y.; Wang, B.; Zhang, B. L.; Ma, J. L.; Yang, Y. X.; Miao, H.; Zhang, S. H.; Li, F.; Lu, Z. H.; Yang, H. X.; Qin, Z. H.; Li, G.; Ping, R. G.; Qiu, J. F.; Zhang, Z. D.; Zhang, H. C.; Dai, H. L.; Li, W. D.; Fang, W. X.; Zeng, Y. J.] Inst High Energy Phys, Beijing 100049, Peoples R China.;[Xu, H. Y.; Yuan, L.] Beihang Univ, Beijing 100191, Peoples R China.;[Afedulidis, O.; Fritsch, M.; Heinsius, F. H.; Kuessner, M.; Hanisch, F.; Pelizaeus, M.; Kopf, B.; Wollenberg, L.; Holtmann, T.; de Boer, R. E.; Feldbauer, F.; Wiedner, U.; Hoelzken, F.] Bochum Ruhr Univ, D-44780 Bochum, Germany.;[Achasov, M. N.; Nikolaev, I. B.; Muchnoi, N. Yu.] Budker Inst Nucl Phys SB RAS BINP, Novosibirsk 630090, Russia.;[Briere, R. A.] Carnegie Mellon Univ, Pittsburgh, PA 15213 USA.
通讯机构：
[Ablikim, M ] I;Inst High Energy Phys, Beijing 100049, Peoples R China.
摘要：
The CP-even fractions (F+) of the decays D-0 -> pi(+) pi(-) pi(0) and D-0 -> K+ K- pi(0) are measured with a quantum-correlated psi(3770) -> D (D) over bar data sample collected by the BESIII experiment corresponding to an integrated luminosity of 7.93 fb(-1). The results are F+pi(+) pi(-) pi(0) = 0.9406 +/- 0.0055 +/- 0.0033 and F-+(K+ K- pi 0) = 0.631 +/- 0.014 +/- 0.011, where the first uncertainties are statistical and the second systematic. These measurements are consistent with the previous determinations, and the uncertainties for F+pi(+) pi(-) pi(0) and F-+(K+ K- pi 0) are reduced by factors of 2.6 and 2.6, respectively. The reported results provide important inputs for the precise measurement of the angle gamma of the Cabibbo-Kobayashi-Maskawa matrix and indirect CP violation in charm mixing.
作者机构：
[Yu, B. X.; Yu, G.; Hu, T.; Ning, Z.; Zhang, P.; Wen, S. P.; Shi, X.; Sun, G. X.; Ma, M. M.; Chen, T.; Hou, X. T.; Zhu, Z. A.; Xu, G. F.; Wang, K.; Zhou, L. P.; Heng, Y. K.; Ji, Q.; Zhang, J. W.; Chen, Z. Y.; Rong, G.; Guan, C. Y.; Qi, F. Z.; Wang, Y. F.; Wang, L. L.; Ouyang, Q.; Jiang, D.; Che, Y. Z.; Liao, Y. P.; Zhang, A. Q.; Ji, X. B.; Qian, S.; Dong, M. Y.; Fang, S. S.; Chang, J. F.; Liu, Z. A.; Yang, T.; Yan, X. Q.; Sun, Z. Q.; Han, T. T.; Wu, J. F.; Sun, S. S.; Ding, B.; Fu, C. D.; Zhang, Y.; Lou, X. C.; Lin, T.; Zhang, B. X.; Xing, T. Y.; Cao, G. F.; Ji, W.; Wu, L. H.; Zhao, Y. B.; Fu, Y. W.; Zheng, J. P.; Jiang, X. S.; Kiuchi, R.; Fang, Y. Q.; Gu, M. H.; Lu, Y. P.; Dong, L. Y.; Zhang, H. Q.; Zhao, G.; Wu, L. J.; Li, L. J.; Yuan, Y.; Lu, X. L.; Wu, Z.; Fang, Y.; Luo, X. L.; Ji, X. L.; Zhang, X. M.; Li, X. Y.; Li, L. K.; Li, H. B.; Liu, F.; Liang, H.; Huang, Y. P.; Zhang, J. Y.; Zhao, L.; Yin, J. H.; Yang, Y. F.; Song, W. M.; Chen, X. T.; Zhang, J. Z.; He, K. L.; Chen, G.; Ablikim, M.; Liu, C. X.; Li, X.; Zhu, K.; Liu, H. H.; Zhao, J. Z.; Mao, Z. P.; Xiao, S. Y.; Lu, J. G.; Liu, P. L.; Jing, M. Q.; Sun, H. K.; Chen, Y. B.; Du, M. C.; Wang, Z.; Ablikim, M; Zhao, J. Y.; Dong, J.; Shi, J. Y.; Ruan, M. Q.; Yuan, C. Z.; Tang, G. Y.; Yuan, S. C.; Zhang, H. Y.; Chen, M. L.; Zhang, Z. H.; Hou, G. Y.; Shen, H. F.; Shao, L. G.; Hou, Z. L.; Sun, Y. Z.; Liu, B. J.; Xiang, B. H.; Zhu, K. J.; Liu, H. M.; Xu, C. F.; Ma, H. L.; Ye, M.; Xie, Y. G.; Chen, H. S.; Cao, N.; Ma, X. T.; Deng, Z. Y.; Ma, Q. M.; Wang, Z. Y.; Cai, X.; Zhang, Y. H.; Batozskay, V.; Ma, R. Q.; Zheng, W. J.; Zou, J. H.; Liu, J. Y.; Wang, X. N.; Kui, X.; Li, W. G.; Wang, Y. Q.; Mo, X. H.; Fang, J.; Li, Q. M.; Shen, X. Y.; Ma, X. Y.; Hu, H. M.; Li, K.; Gong, W. X.; Xu, W.; Hu, Y.; Wang, B.; Zhang, B. L.; Ma, J. L.; Yang, Y. X.; Miao, H.; Zhang, S. H.; Li, F.; Lu, Z. H.; Yang, H. X.; Qin, Z. H.; Li, G.; Ping, R. G.; Qiu, J. F.; Zhang, Z. D.; Zhang, H. C.; Dai, H. L.; Li, W. D.; Fang, W. X.; Zeng, Y. J.] Inst High Energy Phys, Beijing 100049, Peoples R China.;[Xu, H. Y.; Yuan, L.] Beihang Univ, Beijing 100191, Peoples R China.;[Afedulidis, O.; Fritsch, M.; Heinsius, F. H.; Kuessner, M.; Hanisch, F.; Pelizaeus, M.; Kopf, B.; Wollenberg, L.; Holtmann, T.; de Boer, R. E.; Feldbauer, F.; Wiedner, U.; Hoelzken, F.] Bochum Ruhr Univ, D-44780 Bochum, Germany.;[Achasov, M. N.; Nikolaev, I. B.; Muchnoi, N. Yu.] Budker Inst Nucl Phys SB RAS BINP, Novosibirsk 630090, Russia.;[Briere, R. A.] Carnegie Mellon Univ, Pittsburgh, PA 15213 USA.
通讯机构：
[Ablikim, M ] I;Inst High Energy Phys, Beijing 100049, Peoples R China.
摘要：
Utilizing a dataset of 6.7 fb(-1) from electron-positron collisions recorded by the BESIII detector at the BEPCII storage ring, a search is conducted for the processes e(+)e(-) -> phi chi(c0) and phi eta(c2)(1D) across centerof-mass energies from 4.47 to 4.95 GeV. In the absence of any significant signals, upper limits are set. These include limits on the dressed cross sections for e(+)e(-) -> phi chi(c0), as well as the product of the dressed cross section for e(+)e(-) -> phi eta(c2)(1D) and a sum of five branching fractions. Furthermore, the product of the electronic width of Y(4660) and the branching fraction of the Y(4660) ->phi chi(c0), denoted as Gamma Y-e+e-((4660)) B-Y(4660)->phi chi(c0), is determined to be <0.35 eV at the 90% confidence level.
作者：
Ablikim, M.;Achasov, M. N.;Adlarson, P.;Afedulidis, O.;Ai, X. C.;...
期刊：
PHYSICAL REVIEW D,2025年111(3) ISSN：2470-0010
通讯作者：
Ablikim, M
作者机构：
[Yu, B. X.; Yu, G.; Hu, T.; Ning, Z.; Zhang, P.; Wen, S. P.; Shi, X.; Sun, G. X.; Ma, M. M.; Chen, T.; Hou, X. T.; Zhu, Z. A.; Xu, G. F.; Wang, K.; Zhou, L. P.; Heng, Y. K.; Ji, Q.; Zhang, J. W.; Chen, Z. Y.; Rong, G.; Guan, C. Y.; Qi, F. Z.; Wang, Y. F.; Wang, L. L.; Ouyang, Q.; Jiang, D.; Liao, Y. P.; Zhang, A. Q.; Ji, X. B.; Qian, S.; Dong, M. Y.; Fang, S. S.; Chang, J. F.; Liu, Z. A.; Yang, T.; Yan, X. Q.; Sun, Z. Q.; Han, T. T.; Wu, J. F.; Sun, S. S.; Ding, B.; Fu, C. D.; Zhang, Y.; Lou, X. C.; Lin, T.; Zhang, B. X.; Xing, T. Y.; Cao, G. F.; Ji, W.; Wu, L. H.; Zhao, Y. B.; Fu, Y. W.; Zheng, J. P.; Jiang, X. S.; Kiuchi, R.; Fang, Y. Q.; Gu, M. H.; Lu, Y. P.; Dong, L. Y.; Zhang, H. Q.; Zhao, G.; Wu, L. J.; Li, L. J.; Yuan, Y.; Lu, X. L.; Wu, Z.; Fang, Y.; Luo, X. L.; Ji, X. L.; Zhang, X. M.; Li, X. Y.; Li, L. K.; Li, H. B.; Liu, F.; Liang, H.; Huang, Y. P.; Zhang, J. Y.; Zhao, L.; Yin, J. H.; Yang, Y. F.; Batozskaya, V.; Song, W. M.; Chen, X. T.; Zhang, J. Z.; He, K. L.; Ablikim, M.; Liu, C. X.; Li, X.; Zhu, K.; Liu, H. H.; Zhao, J. Z.; Mao, Z. P.; Xiao, S. Y.; Lu, J. G.; Liu, P. L.; Jing, M. Q.; Sun, H. K.; Chen, Y. B.; Du, M. C.; Wang, Z.; Ablikim, M; Zhao, J. Y.; Dong, J.; Shi, J. Y.; Yuan, C. Z.; Tang, G. Y.; Yuan, S. C.; Zhang, H. Y.; Chen, M. L.; Zhang, Z. H.; Hou, G. Y.; Shen, H. F.; Shao, L. G.; Hou, Z. L.; Sun, Y. Z.; Liu, B. J.; Xiang, B. H.; Zhu, K. J.; Liu, H. M.; Xu, C. F.; Ma, H. L.; Ye, M.; Xie, Y. G.; Chen, H. S.; Cao, N.; Ma, X. T.; Deng, Z. Y.; Ma, Q. M.; Wang, Z. Y.; Cai, X.; Zhang, Y. H.; Ma, R. Q.; Zheng, W. J.; Zou, J. H.; Liu, J. Y.; Wang, X. N.; Kui, X.; Li, W. G.; Wang, Y. Q.; Mo, X. H.; Fang, J.; Li, Q. M.; Shen, X. Y.; Ma, X. Y.; Hu, H. M.; Li, K.; Gong, W. X.; Xu, W.; Hu, Y.; Wang, B.; Zhang, B. L.; Ma, J. L.; Yang, Y. X.; Miao, H.; Zhang, S. H.; Li, F.; Lu, Z. H.; Yang, H. X.; Qin, Z. H.; Li, G.; Ping, R. G.; Qiu, J. F.; Zhang, Z. D.; Zhang, H. C.; Dai, H. L.; Li, W. D.; Fang, W. X.; Zeng, Y. J.] Inst High Energy Phys, Beijing 100049, Peoples R China.;[Xu, H. Y.; Yuan, L.] Beihang Univ, Beijing 100191, Peoples R China.;[Afedulidis, O.; Fritsch, M.; Heinsius, F. H.; Kuessner, M.; Hanisch, F.; Pelizaeus, M.; Kopf, B.; Wollenberg, L.; Holtmann, T.; de Boer, R. E.; Feldbauer, F.; Wiedner, U.; Hoelzken, F.] Bochum Ruhr Univ, D-44780 Bochum, Germany.;[Achasov, M. N.; Nikolaev, I. B.; Muchnoi, N. Yu.] Budker Inst Nucl Phys SB RAS BINP, Novosibirsk 630090, Russia.;[Fang, J.; Briere, R. A.] Carnegie Mellon Univ, Pittsburgh, PA 15213 USA.
通讯机构：
[Ablikim, M ] I;Inst High Energy Phys, Beijing 100049, Peoples R China.
摘要：
Using (2712 +/- 14) x 10(6) psi(2S) events collected with the BESIII detector at the BEPCII collider, we search for the decays eta(c) (2S) -> omega omega and eta(c) (2S) -> omega phi via the process psi(2S) -> gamma eta(c)(2S). No statistically significant signals are observed. The upper limits of their product branching fractions at the 90% confidence level are determined to be B(psi(2S) -> gamma eta(c)(2S), eta(c) (2S) -> omega omega) < 1.04 x 10(-6) and B(psi(2S) -> gamma eta(c)(2S),eta(c) (2S) -> omega phi) < 1.85 x 10(-7), respectively. We also update the branching fractions of chi(cJ) -> omega omega and chi(cJ) -> omega phi via the psi(2S) ->gamma chi(cJ) transition. Their branching fractions are determined to be B(chi(co) -> omega omega) = (10.66 +/- 0.11 +/- 0.57)x10(-4), B(chi(c1) -> omega omega) = (6.43 +/- 0.07 +/- 0.31)x10(-4), B(chi(c2) -> omega omega) = (8.75 +/- 0.08 +/- 0.42)x10(-4), B(chi(c0) -> omega phi) = (1.18 +/- 0.03 +/- 0.07) x 10(-4), B(chi(c1) -> omega phi) = (2.04 +/- 0.15 +/- 0.11) x 10(-5), and B(chi(c2) -> omega phi) = (9.58 +/- 1.07 +/- 0.76) x 10(-6), where the first uncertainties are statistical and the second are systematic.
作者机构：
[Yu, B. X.; Yu, G.; Hu, T.; Ning, Z.; Zhang, P.; Wen, S. P.; Shi, X.; Sun, G. X.; Ma, M. M.; Chen, T.; Hou, X. T.; Zhu, Z. A.; Xu, G. F.; Wang, K.; Zhou, L. P.; Heng, Y. K.; Ji, Q.; Zhang, J. W.; Chen, Z. Y.; Rong, G.; Guan, C. Y.; Qi, F. Z.; Wang, Y. F.; Wang, L. L.; Ouyang, Q.; Jiang, D.; Che, Y. Z.; Liao, Y. P.; Zhang, A. Q.; Ji, X. B.; Qian, S.; Dong, M. Y.; Fang, S. S.; Chang, J. F.; Liu, Z. A.; Yang, T.; Yan, X. Q.; Sun, Z. Q.; Han, T. T.; Wu, J. F.; Sun, S. S.; Ding, B.; Fu, C. D.; Zhang, Y.; Lou, X. C.; Lin, T.; Zhang, B. X.; Xing, T. Y.; Cao, G. F.; Ji, W.; Wu, L. H.; Zhao, Y. B.; Fu, Y. W.; Zheng, J. P.; Jiang, X. S.; Kiuchi, R.; Fang, Y. Q.; Gu, M. H.; Lu, Y. P.; Dong, L. Y.; Zhang, H. Q.; Zhao, G.; Wu, L. J.; Li, L. J.; Yuan, Y.; Lu, X. L.; Wu, Z.; Fang, Y.; Luo, X. L.; Ji, X. L.; Zhang, X. M.; Li, X. Y.; Li, L. K.; Li, H. B.; Liu, F.; Liang, H.; Huang, Y. P.; Zhang, J. Y.; Zhao, L.; Yin, J. H.; Yang, Y. F.; Batozskaya, V.; Song, W. M.; Chen, X. T.; Zhang, J. Z.; He, K. L.; Chen, G.; Ablikim, M.; Liu, C. X.; Li, X.; Zhu, K.; Liu, H. H.; Zhao, J. Z.; Mao, Z. P.; Xiao, S. Y.; Lu, J. G.; Liu, P. L.; Jing, M. Q.; Sun, H. K.; Chen, Y. B.; Du, M. C.; Wang, Z.; Ablikim, M; Zhao, J. Y.; Dong, J.; Shi, J. Y.; Ruan, M. Q.; Yuan, C. Z.; Tang, G. Y.; Yuan, S. C.; Zhang, H. Y.; Chen, M. L.; Zhang, Z. H.; Hou, G. Y.; Shen, H. F.; Shao, L. G.; Hou, Z. L.; Sun, Y. Z.; Liu, B. J.; Xiang, B. H.; Zhu, K. J.; Liu, H. M.; Xu, C. F.; Ma, H. L.; Ye, M.; Xie, Y. G.; Chen, H. S.; Cao, N.; Ma, X. T.; Deng, Z. Y.; Ma, Q. M.; Wang, Z. Y.; Cai, X.; Zhang, Y. H.; Ma, R. Q.; Zheng, W. J.; Zou, J. H.; Liu, J. Y.; Wang, X. N.; Kui, X.; Li, W. G.; Wang, Y. Q.; Mo, X. H.; Fang, J.; Li, Q. M.; Shen, X. Y.; Ma, X. Y.; Hu, H. M.; Li, K.; Gong, W. X.; Xu, W.; Hu, Y.; Wang, B.; Zhang, B. L.; Ma, J. L.; Yang, Y. X.; Miao, H.; Zhang, S. H.; Li, F.; Lu, Z. H.; Yang, H. X.; Qin, Z. H.; Li, G.; Ping, R. G.; Qiu, J. F.; Zhang, Z. D.; Zhang, H. C.; Dai, H. L.; Li, W. D.; Fang, W. X.; Zeng, Y. J.] Inst High Energy Phys, Beijing 100049, Peoples R China.;[Xu, H. Y.; Yuan, L.] Beihang Univ, Beijing 100191, Peoples R China.;[Afedulidis, O.; Fritsch, M.; Heinsius, F. H.; Kuessner, M.; Hanisch, F.; Pelizaeus, M.; Kopf, B.; Wollenberg, L.; Holtmann, T.; de Boer, R. E.; Feldbauer, F.; Wiedner, U.; Hoelzken, F.] Bochum Ruhr Univ, D-44780 Bochum, Germany.;[Achasov, M. N.; Nikolaev, I. B.; Muchnoi, N. Yu.] RAS BINP, SB, Budker Inst Nucl Phys, Novosibirsk 630090, Russia.;[Briere, R. A.] Carnegie Mellon Univ, Pittsburgh, PA 15213 USA.
通讯机构：
[Ablikim, M ] I;Inst High Energy Phys, Beijing 100049, Peoples R China.
摘要：
Using 7.9fb(-1) of e(+)e(-) collision data collected at root s = 3.773 GeV with the BESIII detector at the BEPCII collider, we search for the massless dark photon with the flavor-changing neutral current processes D-0 -> omega gamma' and D-0 -> gamma gamma' for the first time. No significant signals are observed, and the upper limits at the 90% confidence level on the massless dark photon branching fraction are set to be 1.1 x 10(-5) and 2.0 x 10(-6) for D-0 -> omega gamma' and D-0 gamma gamma', respectively. These results provide the most stringent constraint on the new physics energy scale associated with cu gamma' coupling in the world, with the new physics energy scale related parameter |C|(2) + |C-5|(2) < 8.2 x 10(-17) GeV-2 at the 90% confidence level.
作者：
Ablikim, M.;Achasov, M. N.;Adlarson, P.;Ai, X. C.;Aliberti, R.;...
期刊：
EUROPEAN PHYSICAL JOURNAL C,2025年85(1) ISSN：1434-6044
通讯作者：
Ablikim, M
作者机构：
[Yu, B. X.; Yu, G.; Li, Xiaoyu; Hu, T.; Ning, Z.; Zhang, P.; Wen, S. P.; Shi, X.; Sun, G. X.; Ma, M. M.; Zhao, Ling; Chen, T.; Hou, X. T.; Zhu, Z. A.; Xu, G. F.; Wang, K.; Zhou, L. P.; Heng, Y. K.; Ji, Q.; Zhang, J. W.; Rong, G.; Guan, C. Y.; Qi, F. Z.; Wang, Y. F.; Wang, L. L.; Ouyang, Q.; Liao, Y. P.; Zhang, A. Q.; Ji, X. B.; Qian, S.; Dong, M. Y.; Fang, S. S.; Chang, J. F.; Liu, Z. A.; Han, T. T.; Wu, J. F.; Wang, Yaqian; Sun, S. S.; Ding, B.; Fu, C. D.; Lou, X. C.; Lin, T.; Zhang, B. X.; Hu, J. F.; Xing, T. Y.; Cao, G. F.; Wu, L. H.; Zhao, Y. B.; Fu, Y. W.; Zheng, J. P.; Jiang, X. S.; Kiuchi, R.; Fang, Y. Q.; Gu, M. H.; Lu, Y. P.; Dong, L. Y.; Zhang, H. Q.; Zhao, G.; Wu, L. J.; Li, L. J.; Yang, Yifan; Yuan, Y.; Lu, X. L.; Wu, Z.; Fang, Y.; Luo, X. L.; Ji, X. L.; Zhang, X. M.; Li, L. K.; Li, H. B.; Liang, H.; Huang, Y. P.; Zhang, J. Y.; Yin, J. H.; Batozskaya, V.; Liu, Huanhuan; Song, W. M.; Chen, X. T.; Zhang, J. Z.; He, K. L.; Chen, G.; Ablikim, M.; Liu, C. X.; Chang, W. L.; Zhu, K.; Zhao, J. Z.; Yang, Tao; Mao, Z. P.; Xiao, S. Y.; Lu, J. G.; Liu, P. L.; Jing, M. Q.; Sun, H. K.; Chen, Y. B.; Zhang, Shuihan; Du, M. C.; Wang, Z.; Ablikim, M; Liu, Fang; Zhao, J. Y.; Dong, J.; Shi, J. Y.; Yuan, C. Z.; Tang, G. Y.; Yuan, S. C.; Zhang, H. Y.; Chen, M. L.; Zhang, Z. H.; Hou, G. Y.; Shen, H. F.; Shao, L. G.; Hou, Z. L.; Sun, Y. Z.; Liu, B. J.; Li, Ke; Zhu, K. J.; Liu, H. M.; Xu, C. F.; Ma, H. L.; Ye, M.; Xie, Y. G.; Chen, H. S.; Cao, N.; Deng, Z. Y.; Ma, Q. M.; Wang, Z. Y.; Cai, X.; Zhang, Y. H.; Ma, R. Q.; Shi, R. S.; Zheng, W. J.; Zou, J. H.; Zhang, Yao; Liu, J. Y.; Kui, X.; Li, W. G.; Wang, Y. Q.; Mo, X. H.; Fang, J.; Shen, X. Y.; Ma, X. Y.; Hu, H. M.; Gong, W. X.; Xu, W.; Hu, Y.; Wang, B.; Zhang, B. L.; Ma, J. L.; Wang, Meng; Yang, Y. X.; Miao, H.; Li, F.; Lu, Z. H.; Yang, H. X.; Qin, Z. H.; Li, G.; Ping, R. G.; Qiu, J. F.; Zhang, Z. D.; Zhang, H. C.; Dai, H. L.; Li, W. D.; Fang, W. X.; Zeng, Y. J.] Inst High Energy Phys, Beijing 100049, Peoples R China.;[Yuan, L.] Beihang Univ, Beijing 100191, Peoples R China.;[Jaeger, S.; Fritsch, M.; Kuessner, M.; Pelizaeus, M.; Kopf, B.; Wollenberg, L.; Holtmann, T.; de Boer, R. E.; Feldbauer, F.; Wiedner, U.; Heinsius, F. H. H.; Coen, S. C.; Wenzel, C. W.] Bochum Ruhr Univ, D-44780 Bochum, Germany.;[Achasov, M. N.; Nikolaev, I. B.; Muchnoi, N. Yu.] Budker Inst Nucl Phys SB RAS BINP, Novosibirsk 630090, Russia.;[Briere, R. A.] Carnegie Mellon Univ, Pittsburgh, PA 15213 USA.
通讯机构：
[Ablikim, M ] I;Inst High Energy Phys, Beijing 100049, Peoples R China.
摘要：
AbstractCharged-particle trajectories are usually reconstructed with the LHCb detector using combined information from the tracking devices placed upstream and downstream of the 4 T m dipole magnet. Trajectories reconstructed using only information from the tracker downstream of the dipole magnet, which are referred to as T tracks, have not been used for physics analysis to date. The challenges of the reconstruction of long-lived particles with T tracks for physics use are discussed and solutions are proposed. The feasibility and the tracking performance are studied using samples of long-lived $$\varvec{\Lambda }$$ Λ and $$K_S^0$$ K S 0 hadrons decaying between 6.0 and 7.6 m downstream of the proton–proton collision point, thereby traversing most of the magnetic field region and providing maximal sensitivity to magnetic and electric dipole moments. The reconstruction can be expanded upstream to about 2.5 m for use in direct searches of exotic long-lived particles. The data used in this analysis have been recorded between 2015 and 2018 and correspond to an integrated luminosity of 6 $$\hbox {fb}^{-1}$$ fb - 1 . The results obtained demonstrate the possibility to further extend the decay volume and the physics reach of the LHCb experiment.
作者机构：
[Yu, B. X.; Yu, G.; Hu, T.; Ning, Z.; Zhang, P.; Wen, S. P.; Shi, X.; Sun, G. X.; Ma, M. M.; Chen, T.; Hou, X. T.; Zhu, Z. A.; Xu, G. F.; Wang, K.; Zhou, L. P.; Heng, Y. K.; Ji, Q.; Zhang, J. W.; Chen, Z. Y.; Rong, G.; Guan, C. Y.; Qi, F. Z.; Wang, Y. F.; Wang, L. L.; Ouyang, Q.; Jiang, D.; Liao, Y. P.; Zhang, A. Q.; Ji, X. B.; Qian, S.; Dong, M. Y.; Fang, S. S.; Chang, J. F.; Liu, Z. A.; Yang, T.; Yan, X. Q.; Sun, Z. Q.; Han, T. T.; Wu, J. F.; Sun, S. S.; Ding, B.; Fu, C. D.; Zhang, Y.; Lou, X. C.; Lin, T.; Zhang, B. X.; Xing, T. Y.; Cao, G. F.; Ji, W.; Wu, L. H.; Zhao, Y. B.; Fu, Y. W.; Zheng, J. P.; Jiang, X. S.; Kiuchi, R.; Fang, Y. Q.; Gu, M. H.; Lu, Y. P.; Dong, L. Y.; Zhang, H. Q.; Zhao, G.; Wu, L. J.; Li, L. J.; Yuan, Y.; Lu, X. L.; Wu, Z.; Fang, Y.; Luo, X. L.; Ji, X. L.; Zhang, X. M.; Li, X. Y.; Li, L. K.; Li, H. B.; Liu, F.; Liang, H.; Huang, Y. P.; Zhang, J. Y.; Zhao, L.; Yin, J. H.; Yang, Y. F.; Batozskaya, V.; Song, W. M.; Chen, X. T.; Zhang, J. Z.; He, K. L.; Chen, G.; Ablikim, M.; Liu, C. X.; Li, X.; Zhu, K.; Liu, H. H.; Zhao, J. Z.; Mao, Z. P.; Xiao, S. Y.; Lu, J. G.; Liu, P. L.; Jing, M. Q.; Sun, H. K.; Chen, Y. B.; Du, M. C.; Wang, Z.; Ablikim, M; Zhao, J. Y.; Dong, J.; Shi, J. Y.; Yuan, C. Z.; Tang, G. Y.; Yuan, S. C.; Zhang, H. Y.; Chen, M. L.; Zhang, Z. H.; Hou, G. Y.; Shen, H. F.; Shao, L. G.; Hou, Z. L.; Sun, Y. Z.; Liu, B. J.; Xiang, B. H.; Zhu, K. J.; Liu, H. M.; Xu, C. F.; Ma, H. L.; Ye, M.; Xie, Y. G.; Chen, H. S.; Cao, N.; Ma, X. T.; Deng, Z. Y.; Ma, Q. M.; Wang, Z. Y.; Cai, X.; Zhang, Y. H.; Ma, R. Q.; Zheng, W. J.; Zou, J. H.; Liu, J. Y.; Wang, X. N.; Kui, X.; Li, W. G.; Wang, Y. Q.; Mo, X. H.; Fang, J.; Li, Q. M.; Shen, X. Y.; Ma, X. Y.; Hu, H. M.; Li, K.; Gong, W. X.; Xu, W.; Hu, Y.; Wang, B.; Zhang, B. L.; Ma, J. L.; Yang, Y. X.; Miao, H.; Zhang, S. H.; Li, F.; Lu, Z. H.; Yang, H. X.; Qin, Z. H.; Li, G.; Ping, R. G.; Qiu, J. F.; Zhang, Z. D.; Zhang, H. C.; Dai, H. L.; Li, W. D.; Fang, W. X.; Zeng, Y. J.] Inst High Energy Phys, Beijing 100049, Peoples R China.;[Xu, H. Y.; Yuan, L.] Beihang Univ, Beijing 100191, Peoples R China.;[Afedulidis, O.; Fritsch, M.; Heinsius, F. H.; Kuessner, M.; Hanisch, F.; Pelizaeus, M.; Kopf, B.; Wollenberg, L.; Holtmann, T.; de Boer, R. E.; Feldbauer, F.; Wiedner, U.; Hoelzken, F.] Bochum Ruhr Univ, D-44780 Bochum, Germany.;[Achasov, M. N.; Nikolaev, I. B.; Muchnoi, N. Yu.] Budker Inst Nucl Phys SB RAS BINP, Novosibirsk 630090, Russia.;[Briere, R. A.] Carnegie Mellon Univ, Pittsburgh, PA 15213 USA.
通讯机构：
[Ablikim, M ] I;Inst High Energy Phys, Beijing 100049, Peoples R China.
摘要：
Studies are performed of the Cabibbo-favored decay Lambda(+)(c) -> Lambda(KSK+)-K-0 and the singly Cabibbosuppressed decay Lambda(+)(c) -> Lambda K-S(0)pi(+), based on a sample of e(+)e(-) collision data, corresponding to an integrated luminosity of 4.5 fb(-1), accumulated at center-of-mass energies between 4599.53 MeV and 4698.82 MeV with the BESIII detector. The decay Lambda(+)(c) -> Lambda K-S(0)pi(+) is observed for the first time. The branching fractions of Lambda(+)(c) -> Lambda(KSK+)-K-0 and Lambda(+)(c) -> Lambda K-S(0)pi(+) are measured to be (3.04 +/- 0.30 +/- 0.16) x 10(-3) and o1.73 +/- 0.27 +/- 0.10) x 10(-3), respectively, where the first uncertainties are statistical and the second are systematic. These results correspond to the most precise measurement of these quantities for both decays. Evidence of a K*(+) contribution in the Lambda(+)(c) -> Lambda K-S(0)pi(+) decay is found with a statistical significance of 4.71 sigma. The branching fraction of Lambda(+)(c) -> Lambda K*+ is calculated under three possible interference scenarios, with the significance increasing to 5.03 sigma when interference is taken into account.
作者：
Ablikim, M.;Achasov, M. N.;Adlarson, P.;Afedulidis, O.;Ai, X. C.;...
期刊：
PHYSICAL REVIEW D,2025年111(3) ISSN：2470-0010
通讯作者：
Ablikim, M
作者机构：
[Yu, B. X.; Yu, G.; Hu, T.; Ning, Z.; Zhang, P.; Wen, S. P.; Shi, X.; Sun, G. X.; Ma, M. M.; Guskov, A.; Chen, T.; Hou, X. T.; Zhu, Z. A.; Xu, G. F.; Wang, K.; Zhou, L. P.; Heng, Y. K.; Ji, Q.; Zhang, J. W.; Chen, Z. Y.; Rong, G.; Guan, C. Y.; Qi, F. Z.; Wang, Y. F.; Wang, L. L.; Ouyang, Q.; Jiang, D.; Liao, Y. P.; Zhang, A. Q.; Ji, X. B.; Qian, S.; Dong, M. Y.; Fang, S. S.; Chang, J. F.; Liu, Z. A.; Yang, T.; Yan, X. Q.; Sun, Z. Q.; Han, T. T.; Wu, J. F.; Rivetti, A.; Sun, S. S.; Ding, B.; Fu, C. D.; Zhang, Y.; Lou, X. C.; Lin, T.; Zhang, B. X.; Xing, T. Y.; Cao, G. F.; Ji, W.; Wu, L. H.; Zhao, Y. B.; Fu, Y. W.; Zheng, J. P.; Jiang, X. S.; Kiuchi, R.; Fang, Y. Q.; Gu, M. H.; Lu, Y. P.; Dong, L. Y.; Zhang, H. Q.; Zhao, G.; Wu, L. J.; Li, L. J.; Yuan, Y.; Lu, X. L.; Wu, Z.; Fang, Y.; Luo, X. L.; Ji, X. L.; Zhang, X. M.; Li, X. Y.; Li, L. K.; Li, H. B.; Liu, F.; Liang, H.; Huang, Y. P.; Zhang, J. Y.; Zhao, L.; Yin, J. H.; Yang, Y. F.; Batozskaya, V.; Song, W. M.; Chen, X. T.; Zhang, J. Z.; He, K. L.; Chen, G.; Ablikim, M.; Liu, C. X.; Li, X.; Zhu, K.; Liu, H. H.; Zhao, J. Z.; Mao, Z. P.; Xiao, S. Y.; Lu, J. G.; Liu, P. L.; Jing, M. Q.; Sun, H. K.; Chen, Y. B.; Du, M. C.; Wang, Z.; Ablikim, M; Zhao, J. Y.; Dong, J.; Shi, J. Y.; Zhemchugov, A.; Yuan, C. Z.; Tang, G. Y.; Yuan, S. C.; Zhang, H. Y.; Chen, M. L.; Zhang, Z. H.; Hou, G. Y.; Shen, H. F.; Shao, L. G.; Hou, Z. L.; Sun, Y. Z.; Liu, B. J.; Xiang, B. H.; Zhu, K. J.; Liu, H. M.; Xu, C. F.; Ma, H. L.; Dedovich, D.; Ye, M.; Xie, Y. G.; Chen, H. S.; Cao, N.; Ma, X. T.; Deng, Z. Y.; Ma, Q. M.; Wang, Z. Y.; Cai, X.; Zhang, Y. H.; Ma, R. Q.; Zheng, W. J.; Zou, J. H.; Liu, J. Y.; Wang, X. N.; Kui, X.; Li, W. G.; Wang, Y. Q.; Mo, X. H.; Fang, J.; Li, Q. M.; Shen, X. Y.; Ma, X. Y.; Hu, H. M.; Li, K.; Gong, W. X.; Xu, W.; Hu, Y.; Wang, B.; Zhang, B. L.; Ma, J. L.; Yang, Y. X.; Miao, H.; Zhang, S. H.; Li, F.; Lu, Z. H.; Yang, H. X.; Qin, Z. H.; Li, G.; Ping, R. G.; Sarantsev, A.; Qiu, J. F.; Zhang, Z. D.; Zhang, H. C.; Dai, H. L.; Li, W. D.; Fang, W. X.; Zeng, Y. J.] Inst High Energy Phys, Beijing 100049, Peoples R China.;[Xu, H. Y.; Yuan, L.] Beihang Univ, Beijing 100191, Peoples R China.;[Afedulidis, O.; Guskov, A.; Nikolaev, I. B.; Fritsch, M.; Heinsius, F. H.; Kuessner, M.; Rivetti, A.; Hanisch, F.; Pelizaeus, M.; Chelkov, G.; Kopf, B.; Wollenberg, L.; Holtmann, T.; Fava, L.; Zhemchugov, A.; de Boer, R. E.; Dedovich, D.; Feldbauer, F.; Wiedner, U.; Holzken, F.; Sarantsev, A.] Bochum Ruhr Univ, D-44780 Bochum, Germany.;[Achasov, M. N.; Nikolaev, I. B.; Muchnoi, N. Yu.] Budker Inst Nucl Phys SB RAS BINP, Novosibirsk 630090, Russia.;[Briere, R. A.] Carnegie Mellon Univ, Pittsburgh, PA 15213 USA.
通讯机构：
[Ablikim, M ] I;Inst High Energy Phys, Beijing 100049, Peoples R China.
摘要：
Using a sample of (2712 +/- 14) x 10(6) psi(3686) events collected with the BESIII detector, we perform partial wave analyses of the decays psi(3686) -> p (p) over bar pi(0) and psi(3686) -> p (p) over bar eta. The branching fractions of psi(3686) -> p (p) over bar pi(0) and psi(3686) -> p (p) over bar eta. are determined to be (133.9 +/- 11.2 +/- 2.3) x 10(-6) or (183.7 +/- 13.7 +/- 3.2) x 10(-6) and (61.5 +/- 6.5 +/- 1.1) x 10(-6) or (84.4 +/- 6.9 +/- 1.4) x 10(-6), respectively, where the two solutions are caused by an ambiguous phase angle between resonant and continuum processes. Several well-established N* states are observed in the p pi(0) and p eta systems, and the corresponding branching fractions are measured. The ratio of decay widths Gamma(N(1535)-> N eta)/Gamma(N(1535)-> N pi) is determined to be 0.99 +/- 0.05 +/- 0.19.
作者机构：
[Yu, B. X.; Yu, G.; Hu, T.; Ning, Z.; Zhang, P.; Wen, S. P.; Shi, X.; Sun, G. X.; Ma, M. M.; Chen, T.; Hou, X. T.; Zhu, Z. A.; Xu, G. F.; Wang, K.; Zhou, L. P.; Heng, Y. K.; Ji, Q.; Zhang, J. W.; Chen, Z. Y.; Rong, G.; Guan, C. Y.; Qi, F. Z.; Wang, Y. F.; Wang, L. L.; Ouyang, Q.; Jiang, D.; Liao, Y. P.; Zhang, A. Q.; Ji, X. B.; Qian, S.; Dong, M. Y.; Fang, S. S.; Chang, J. F.; Liu, Z. A.; Yang, T.; Yan, X. Q.; Sun, Z. Q.; Han, T. T.; Wu, J. F.; Sun, S. S.; Ding, B.; Fu, C. D.; Zhang, Y.; Lou, X. C.; Lin, T.; Zhang, B. X.; Xing, T. Y.; Cao, G. F.; Ji, W.; Wu, L. H.; Zhao, Y. B.; Fu, Y. W.; Zheng, J. P.; Jiang, X. S.; Kiuchi, R.; Fang, Y. Q.; Gu, M. H.; Lu, Y. P.; Dong, L. Y.; Zhang, H. Q.; Zhao, G.; Wu, L. J.; Li, L. J.; Yuan, Y.; Lu, X. L.; Wu, Z.; Fang, Y.; Luo, X. L.; Ji, X. L.; Zhang, X. M.; Li, X. Y.; Li, L. K.; Li, H. B.; Liu, F.; Liang, H.; Huang, Y. P.; Zhang, J. Y.; Zhao, L.; Yin, J. H.; Yang, Y. F.; Batozskaya, V.; Song, W. M.; Chen, X. T.; Zhang, J. Z.; He, K. L.; Chen, G.; Ablikim, M.; Liu, C. X.; Li, X.; Zhu, K.; Liu, H. H.; Zhao, J. Z.; Mao, Z. P.; Xiao, S. Y.; Lu, J. G.; Liu, P. L.; Jing, M. Q.; Sun, H. K.; Chen, Y. B.; Du, M. C.; Wang, Z.; Ablikim, M; Zhao, J. Y.; Dong, J.; Shi, J. Y.; Yuan, C. Z.; Tang, G. Y.; Yuan, S. C.; Zhang, H. Y.; Chen, M. L.; Zhang, Z. H.; Hou, G. Y.; Shen, H. F.; Shao, L. G.; Hou, Z. L.; Sun, Y. Z.; Liu, B. J.; Xiang, B. H.; Zhu, K. J.; Liu, H. M.; Xu, C. F.; Ma, H. L.; Ye, M.; Xie, Y. G.; Chen, H. S.; Cao, N.; Ma, X. T.; Deng, Z. Y.; Ma, Q. M.; Wang, Z. Y.; Cai, X.; Zhang, Y. H.; Ma, R. Q.; Zheng, W. J.; Zou, J. H.; Liu, J. Y.; Wang, X. N.; Kui, X.; Li, W. G.; Wang, Y. Q.; Mo, X. H.; Fang, J.; Li, Q. M.; Shen, X. Y.; Ma, X. Y.; Hu, H. M.; Li, K.; Gong, W. X.; Xu, W.; Hu, Y.; Wang, B.; Zhang, B. L.; Ma, J. L.; Yang, Y. X.; Miao, H.; Zhang, S. H.; Li, F.; Lu, Z. H.; Yang, H. X.; Qin, Z. H.; Li, G.; Ping, R. G.; Qiu, J. F.; Zhang, Z. D.; Zhang, H. C.; Dai, H. L.; Li, W. D.; Fang, W. X.; Zeng, Y. J.] Inst High Energy Phys, Beijing 100049, Peoples R China.;[Xu, H. Y.; Liu, Ke; Yuan, L.] Beihang Univ, Beijing 100191, Peoples R China.;[Afedulidis, O.; Fritsch, M.; Heinsius, F. H.; Kuessner, M.; Hanisch, F.; Pelizaeus, M.; Kopf, B.; Wollenberg, L.; Holtmann, T.; de Boer, R. E.; Feldbauer, F.; Wiedner, U.; Hoelzken, F.] Bochum Ruhr Univ, D-44780 Bochum, Germany.;[Achasov, M. N.; Nikolaev, I. B.; Muchnoi, N. Yu.] Budker Inst Nucl Phys SB RAS BINP, Novosibirsk 630090, Russia.;[Briere, R. A.] Carnegie Mellon Univ, Pittsburgh, PA 15213 USA.
通讯机构：
[Ablikim, M ] I;Inst High Energy Phys, Beijing 100049, Peoples R China.
摘要：
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.
作者机构：
[Yu, B. X.; Yu, G.; Hu, T.; Ning, Z.; Zhang, P.; Wen, S. P.; Shi, X.; Sun, G. X.; Ma, M. M.; Chen, T.; Hou, X. T.; Zhu, Z. A.; Xu, G. F.; Wang, K.; Zhou, L. P.; Heng, Y. K.; Ji, Q.; Zhang, J. W.; Chen, Z. Y.; Rong, G.; Guan, C. Y.; Qi, F. Z.; Wang, Y. F.; Wang, L. L.; Ouyang, Q.; Jiang, D.; Liao, Y. P.; Zhang, A. Q.; Ji, X. B.; Qian, S.; Dong, M. Y.; Fang, S. S.; Chang, J. F.; Liu, Z. A.; Yang, T.; Yan, X. Q.; Sun, Z. Q.; Han, T. T.; Wu, J. F.; Sun, S. S.; Ding, B.; Fu, C. D.; Zhang, Y.; Lou, X. C.; Lin, T.; Zhang, B. X.; Xing, T. Y.; Cao, G. F.; Ji, W.; Wu, L. H.; Zhao, Y. B.; Fu, Y. W.; Zheng, J. P.; Jiang, X. S.; Kiuchi, R.; Fang, Y. Q.; Gu, M. H.; Lu, Y. P.; Dong, L. Y.; Zhang, H. Q.; Zhao, G.; Wu, L. J.; Li, L. J.; Yuan, Y.; Lu, X. L.; Wu, Z.; Fang, Y.; Luo, X. L.; Ji, X. L.; Zhang, X. M.; Li, X. Y.; Li, L. K.; Li, H. B.; Liu, F.; Liang, H.; Huang, Y. P.; Zhang, J. Y.; Zhao, L.; Yin, J. H.; Yang, Y. F.; Batozskaya, V.; Song, W. M.; Chen, X. T.; Zhang, J. Z.; He, K. L.; Chen, G.; Ablikim, M.; Liu, C. X.; Li, X.; Zhu, K.; Liu, H. H.; Zhao, J. Z.; Mao, Z. P.; Xiao, S. Y.; Lu, J. G.; Liu, P. L.; Jing, M. Q.; Sun, H. K.; Chen, Y. B.; Du, M. C.; Wang, Z.; Ablikim, M; Zhao, J. Y.; Dong, J.; Shi, J. Y.; Yuan, C. Z.; Tang, G. Y.; Yuan, S. C.; Zhang, H. Y.; Chen, M. L.; Zhang, Z. H.; Hou, G. Y.; Shen, H. F.; Shao, L. G.; Hou, Z. L.; Sun, Y. Z.; Liu, B. J.; Xiang, B. H.; Zhu, K. J.; Liu, H. M.; Xu, C. F.; Ma, H. L.; Ye, M.; Xie, Y. G.; Chen, H. S.; Cao, N.; Ma, X. T.; Deng, Z. Y.; Ma, Q. M.; Wang, Z. Y.; Cai, X.; Zhang, Y. H.; Ma, R. Q.; Zheng, W. J.; Zou, J. H.; Liu, J. Y.; Wang, X. N.; Kui, X.; Li, W. G.; Wang, Y. Q.; Mo, X. H.; Fang, J.; Li, Q. M.; Shen, X. Y.; Ma, X. Y.; Hu, H. M.; Li, K.; Gong, W. X.; Xu, W.; Hu, Y.; Wang, B.; Zhang, B. L.; Ma, J. L.; Yang, Y. X.; Miao, H.; Zhang, S. H.; Li, F.; Lu, Z. H.; Yang, H. X.; Qin, Z. H.; Li, G.; Ping, R. G.; Qiu, J. F.; Zhang, Z. D.; Zhang, H. C.; Dai, H. L.; Li, W. D.; Fang, W. X.; Zeng, Y. J.] Inst High Energy Phys, Beijing 100049, Peoples R China.;[Xu, H. Y.; Liu, Ke; Yuan, L.] Beihang Univ, Beijing 100191, Peoples R China.;[Afedulidis, O.; Fritsch, M.; Heinsius, F. H.; Kuessner, M.; Hanisch, F.; Pelizaeus, M.; Kopf, B.; Wollenberg, L.; Holtmann, T.; de Boer, R. E.; Feldbauer, F.; Wiedner, U.; Hoelzken, F.] Bochum Ruhr Univ, D-44780 Bochum, Germany.;[Achasov, M. N.; Nikolaev, I. B.; Muchnoi, N. Yu.] Budker Inst Nucl Phys SB RAS BINP, Novosibirsk 630090, Russia.;[Briere, R. A.] Carnegie Mellon Univ, Pittsburgh, PA 15213 USA.
通讯机构：
[Ablikim, M ] I;Inst High Energy Phys, Beijing 100049, Peoples R China.
摘要：
One of the main goals of studying semileptonic decays in flavor physics is to gain a better understanding of hadronic transitions in the nonperturbative region of Quantum Chromodynamics. This involves measuring Cabibbo-Kobayashi-Maskawa matrix elements, understanding form factors, and comparing them with theoretical predictions. We report a first study of the semileptonic decay D^{0}→K^{-}π^{0}μ^{+}ν_{μ} by analyzing an e^{+}e^{-} annihilation data sample of 7.93 fb^{-1} collected at the center-of-mass energy of 3.773GeV with the BESIII detector. The absolute branching fraction of D^{0}→K^{-}π^{0}μ^{+}ν_{μ} is measured for the first time, providing necessary input for extracting the c→s Cabibbo-Kobayashi-Maskawa matrix element through this process. This measurement allows us to test lepton flavor universality, with no indication of violation found. Furthermore, a series of hadronic form factors have been determined and compared with theoretical predictions, which will impose stricter constraints on theoretical models.
作者机构：
[Yu, B. X.; Hu, T.; Ning, Z.; Zhang, P.; Wen, S. P.; Shi, X.; Sun, G. X.; Chen, T.; Hou, X. T.; Zhu, Z. A.; Xu, G. F.; Wang, K.; Heng, Y. K.; Ji, Q.; Zhang, J. W.; Amoroso, A.; Rong, G.; Guan, C. Y.; Qi, F. Z.; Wang, Y. F.; Wang, L. L.; Ouyang, Q.; Jiang, D.; Che, Y. Z.; Liao, Y. P.; Zhang, A. Q.; Ji, X. B.; Qian, S.; Dong, M. Y.; Fang, S. S.; Chang, J. F.; Liu, Z. A.; Yang, T.; Yan, X. Q.; Sun, Z. Q.; Han, T. T.; Wu, J. F.; Sun, S. S.; Ding, B.; Fu, C. D.; Zhang, Y.; Lou, X. C.; Lin, T.; Zhang, B. X.; Xing, T. Y.; Cao, G. F.; Ji, W.; Wu, L. H.; Zhao, Y. B.; Fu, Y. W.; Zheng, J. P.; Jiang, X. S.; Kiuchi, R.; Fang, Y. Q.; Gu, M. H.; Lu, Y. P.; Dong, L. Y.; Zhang, H. Q.; Zhao, G.; Wu, L. J.; Li, L. J.; Yuan, Y.; Wu, Z.; Luo, X. L.; Ji, X. L.; Zhang, X. M.; Li, X. Y.; Li, H. B.; Liu, F.; Huang, Y. P.; Zhang, J. Y.; Zhao, L.; Batozskaya, V.; Song, W. M.; Chen, X. T.; Zhang, J. Z.; He, K. L.; Chen, G.; Ma, H.; Ablikim, M.; Bortone, A.; Liu, C. X.; Li, X.; Zhu, K.; Liu, H. H.; Zhao, J. Z.; Mao, Z. P.; Lu, J. G.; Liu, P. L.; Jing, M. Q.; Sun, H. K.; Chen, Y. B.; Du, M. C.; Wang, Z.; Ablikim, M; Zhao, J. Y.; Dong, J.; Shi, J. Y.; Ruan, M. Q.; Yuan, C. Z.; Tang, G. Y.; Yuan, S. C.; Zhang, H. Y.; Chen, M. L.; Zhang, Z. H.; Hou, G. Y.; Shen, H. F.; Shao, L. G.; Hou, Z. L.; Sun, Y. Z.; Liu, B. J.; Xiang, B. H.; Brueggemann, A.; Zhu, K. J.; Liu, H. M.; Xu, C. F.; Ma, H. L.; Ye, M.; Xie, Y. G.; Chen, H. S.; Cao, N.; Ma, X. T.; Deng, Z. Y.; Ma, Q. M.; Wang, Z. Y.; Cai, X.; Zhang, Y. H.; Ma, R. Q.; Zheng, W. J.; Zou, J. H.; Wang, X. N.; Kui, X.; Li, W. G.; Wang, Y. Q.; Mo, X. H.; Fang, J.; Li, Q. M.; Shen, X. Y.; Ma, X. Y.; Hu, H. M.; Li, K.; Gong, W. X.; Hu, Y.; Wang, B.; Zhang, B. L.; Ma, J. L.; Yang, Y. X.; Miao, H.; Zhang, S. H.; Li, F.; Lu, Z. H.; Yang, H. X.; Qin, Z. H.; Li, G.; Ping, R. G.; Qiu, J. F.; Zhang, Z. D.; Zhang, H. C.; Dai, H. L.; Li, W. D.; Fang, W. X.; Zeng, Y. J.] Inst High Energy Phys, Beijing 100049, Peoples R China.;[Wollenberg, L.; Yuan, L.] Beihang Univ, Beijing 100191, Peoples R China.;[Afedulidis, O.; Fritsch, M.; Heinsius, F. H.; Kuessner, M.; Hanisch, F.; Pelizaeus, M.; Kopf, B.; Holtmann, T.; de Boer, R. E.; Feldbauer, F.; Wiedner, U.; Holzken, F.] Bochum Ruhr Univ, D-44780 Bochum, Germany.;[Achasov, M. N.; Nikolaev, I. B.; Muchnoi, N. Yu.] Budker Inst Nucl Phys SB RAS BINP, Novosibirsk 630090, Russia.;[Briere, R. A.] Carnegie Mellon Univ, Pittsburgh, PA 15213 USA.
通讯机构：
[Ablikim, M ] I;Inst High Energy Phys, Beijing 100049, Peoples R China.
摘要：
Using (27.12 +/- 0.14) x 10(8) psi(2S) events collected by the BESIII detector operating at BEPCII, we search for the decay eta(c) (2S) -> p (p) over bar via the process psi(2S) -> gamma eta(c)(2S) and only find a signal with a significance of 1.7 sigma. The upper limit of the product branching fraction at the 90% confidence level is determined to be B(psi(2S) -> gamma eta(c)(2S)) B(eta(c) (2S) -> p (p) over bar)< 2.4 x 10(-7). The branching fractions of chi(cJ) -> p<(p)over bar> (J = 0, 1, 2) are also measured to be B(chi(c0) -> p (p) over bar) = (2.51 +/- 0.02 +/- 0.08) x 10(-4), B(chi(c1) -> p (p) over bar) = (8.16 +/- 0.09 +/- 0.25) x 10(-4), and B(chi(c2) -> p (p) over bar) = (8.33 +/- 0.09 +/- 0.22) x 10(-4), where the first uncertainty is statistical and the second systematic.
作者机构：
[Sun, Z Q; Wen, S P; Hou, G Y; Liang, H; Dai, H L; Yuan, C Z; Zhao, G; Xu, W; Zhao, L; Xiao, S Y; Ma, Q M; Lou, X C; Hou, X T; Zhang, P; Zhang, Y; Tang, G Y; Liu, F; Batozskaya, V; Liu, P L; Wang, X N; Xiang, B H; Zhang, Z D; Cao, G F; Sun, H K; Yan, X Q; Wang, Y F; Kiuchi, R; Li, Q M; Wang, Y Q; Sun, Y Z; Zhang, J Z; Zhang, J W; Zhang, J Y; Zhang, Z H; Han, T T; Yang, T; Liu, C X; Mo, X H; Hu, Y; Fang, Y Q; Hu, T; Song, W M; Zhu, Z A; Wu, Z; Zheng, W J; Chang, J F; Yuan, Y; Deng, Z Y; Lu, J G; Yu, G; Hu, H M; Zheng, J P; Zeng, Y J; Ma, R Q; Ouyang, Q; Fang, W X; Chen, T; Yuan, S C; Fu, Y W; Rong, G; Chen, G; Ding, B; Liu, B J; Zhu, K J; Hou, Z L; Ablikim, M; Xu, C F; Cai, X; Li, L K; Li, L J; Ma, H L; Qiu, J F; Jiang, D; Ma, X T; Ma, X Y; Lu, Y P; Heng, Y K; Qin, Z H; Fang, S S; Wang, B; Sun, S S; Wang, K; Ping, R G; Du, M C; Wang, Z; Liu, H M; Liao, Y P; Zhang, S H; Mao, Z P; Yin, J H; Yu, B X; Liu, H H; Gong, W X; Kui, X; Lu, Z H; Chen, M L; Zhu, K; Chen, Z Y; Ji, X L; Zhang, B X; Ji, X B; Zhang, B L; Guan, C Y; Jing, M Q; Li, K; Li, G; Shi, J Y; Li, F; Lin, T; Zhang, A Q; Li, X; Li, H B; Lu, X L; Xu, G F; Chen, X T; Yang, H X; Gu, M H; Wang, Z Y; Zhang, Y H; Zou, J H; Li, X Y; Wu, L H; Wu, L J; Zhang, H Q; Zhou, L P; Chen, H S; Shao, L G; Fu, C D; Zhang, H C; Zhao, J Y; Zhao, J Z; Xing, T Y; Yang, Y F; Li, W D; Li, W G; He, K L; Ma, M M; Qi, F Z; Qian, S; Yang, Y X; Zhang, X M; Zhang, H Y; Zhao, Y B; Chen, Y B; Sun, G X; Wang, L L; Ning, Z; Huang, Y P; Ma, J L; Dong, L Y; Luo, X L; Jiang, X S; Fang, Y; Fang, J; Ye, M; Shen, X Y; Dong, M Y; Cao, N; Miao, H; Shi, X; Ji, Q; Wu, J F; Liu, Z A; Ji, W; Shen, H F; Xie, Y G; Dong, J; Liu, J Y] Institute of High Energy Physics, Beijing 100049, People's Republic of China;[Achasov, M N; Muchnoi, N Yu; Nikolaev, I B] Budker Institute of Nuclear Physics SB RAS (BINP), Novosibirsk 630090, Russia;[Adlarson, P; Schoenning, K; Thoren, V; Kupsc, A; Wolke, M; Johansson, T] Uppsala University, Box 516, SE-75120 Uppsala, Sweden;[Fritsch, M; Heinsius, F H; Wiedner, U; Wollenberg, L; Feldbauer, F; Hölzken, F; Afedulidis, O; Holtmann, T; Hanisch, F; Pelizaeus, M; de Boer, R E; Kopf, B; Kuessner, M] Bochum Ruhr-University, D-44780 Bochum, Germany;[Li, D M; Liu, Y; Zhang, H; Zhang, J; Du, S X; Yu, Y C; Yan, W C; Ai, X C; Zhao, S J; Ke, B C; Zhang, Y T; Ge, L; Qiao, X K] Zhengzhou University, Zhengzhou 450001, People's Republic of China
摘要：
Using 20.3 fb^{-1} of e^{+}e^{-} collision data collected at the center-of-mass energy 3.773GeV with the BESIII detector, we report the first observation of the semileptonic decay D^{+}→η^{'}μ^{+}ν_{μ} with significance of 8.6σ including systematic uncertainties, and an improved measurement of D^{+}→η^{'}e^{+}ν_{e}. The branching fractions of D^{+}→η^{'}μ^{+}ν_{μ} and D^{+}→η^{'}e^{+}ν_{e} are determined to be (1.92±0.28_{stat}±0.08_{syst})×10^{-4} and (1.79±0.19_{stat}±0.07_{syst})×10^{-4}, respectively. The ratio of the two branching fractions is determined to be R_{μ/e}=1.07±0.19_{stat}±0.03_{syst}, which agrees with the theoretical expectation of lepton flavor universality within the standard model. From an analysis of the D^{+}→η^{'}ℓ^{+}ν_{ℓ} decay dynamics, the product of the hadronic form factor f_{+}^{η^{'}}(0) and the Cabibbo-Kobayashi-Maskawa matrix element |V_{cd}| is measured for the first time, giving f_{+}^{η^{'}}(0)|V_{cd}|=(5.92±0.56_{stat}±0.13_{syst})×10^{-2}. The η-η^{'} mixing angle in the quark flavor basis is determined to be ϕ_{P}=(39.8±0.8_{stat}±0.3_{syst})°.
作者：
Ablikim, M;Achasov, M N;Adlarson, P;Afedulidis, O;Ai, X C;...
期刊：
科学通报(英文版),2025年70(4):454-459 ISSN：2095-9273
作者机构：
Institute of High Energy Physics, Beijing 100049, People's Republic of China;Budker Institute of Nuclear Physics SB RAS (BINP), Novosibirsk 630090, Russia;Uppsala University, Box 516, SE-75120, Uppsala, Sweden;Bochum Ruhr-University, D-44780, Bochum, Germany;Zhengzhou University, Zhengzhou 450001, People's Republic of China
摘要：
<正>The ground-state hyperons have played a crucial role in the understanding of weak interactions. However, numerous unanswered questions persist regarding the weak decay mechanisms and the role of hyperons in non-perturbative quantum chromodynamics(QCD). Specifically, weak radiative hyperon decays(WRHDs) provide valuable insights into the nature of nonleptonic weak interactions.
作者机构：
[Yu, B. X.; Yu, G.; Hu, T.; Ning, Z.; Zhang, P.; Wen, S. P.; Shi, X.; Sun, G. X.; Ma, M. M.; Chen, T.; Hou, X. T.; Zhu, Z. A.; Xu, G. F.; Wang, K.; Zhou, L. P.; Heng, Y. K.; Ji, Q.; Zhang, J. W.; Chen, Z. Y.; Rong, G.; Guan, C. Y.; Qi, F. Z.; Wang, Y. F.; Wang, L. L.; Ouyang, Q.; Jiang, D.; Liao, Y. P.; Zhang, A. Q.; Ji, X. B.; Qian, S.; Dong, M. Y.; Fang, S. S.; Chang, J. F.; Liu, Z. A.; Yang, T.; Yan, X. Q.; Sun, Z. Q.; Han, T. T.; Wu, J. F.; Sun, S. S.; Ding, B.; Fu, C. D.; Zhang, Y.; Lou, X. C.; Lin, T.; Zhang, B. X.; Xing, T. Y.; Cao, G. F.; Ji, W.; Wu, L. H.; Zhao, Y. B.; Fu, Y. W.; Zheng, J. P.; Jiang, X. S.; Kiuchi, R.; Fang, Y. Q.; Gu, M. H.; Lu, Y. P.; Dong, L. Y.; Zhang, H. Q.; Zhao, G.; Wu, L. J.; Li, L. J.; Yuan, Y.; Lu, X. L.; Wu, Z.; Fang, Y.; Luo, X. L.; Ji, X. L.; Zhang, X. M.; Li, X. Y.; Li, L. K.; Li, H. B.; Liu, F.; Liang, H.; Huang, Y. P.; Zhang, J. Y.; Zhao, L.; Yin, J. H.; Yang, Y. F.; Batozskaya, V.; Song, W. M.; Chen, X. T.; Zhang, J. Z.; He, K. L.; Chen, G.; Ablikim, M.; Liu, C. X.; Li, X.; Zhu, K.; Liu, H. H.; Zhao, J. Z.; Mao, Z. P.; Xiao, S. Y.; Lu, J. G.; Liu, P. L.; Jing, M. Q.; Sun, H. K.; Chen, Y. B.; Du, M. C.; Wang, Z.; Ablikim, M; Zhao, J. Y.; Dong, J.; Shi, J. Y.; Yuan, C. Z.; Tang, G. Y.; Yuan, S. C.; Zhang, H. Y.; Chen, M. L.; Zhang, Z. H.; Hou, G. Y.; Shen, H. F.; Shao, L. G.; Hou, Z. L.; Sun, Y. Z.; Liu, B. J.; Xiang, B. H.; Zhu, K. J.; Liu, H. M.; Xu, C. F.; Ma, H. L.; Ye, M.; Xie, Y. G.; Chen, H. S.; Cao, N.; Ma, X. T.; Deng, Z. Y.; Ma, Q. M.; Wang, Z. Y.; Cai, X.; Zhang, Y. H.; Ma, R. Q.; Zheng, W. J.; Zou, J. H.; Liu, J. Y.; Wang, X. N.; Kui, X.; Li, W. G.; Wang, Y. Q.; Mo, X. H.; Fang, J.; Li, Q. M.; Shen, X. Y.; Ma, X. Y.; Hu, H. M.; Li, K.; Gong, W. X.; Xu, W.; Hu, Y.; Wang, B.; Zhang, B. L.; Ma, J. L.; Yang, Y. X.; Miao, H.; Zhang, S. H.; Li, F.; Lu, Z. H.; Yang, H. X.; Qin, Z. H.; Li, G.; Ping, R. G.; Qiu, J. F.; Zhang, Z. D.; Zhang, H. C.; Dai, H. L.; Li, W. D.; Fang, W. X.; Zeng, Y. J.] Inst High Energy Phys, Beijing 100049, Peoples R China.;[Xu, H. Y.; Liu, Ke; Yuan, L.] Beihang Univ, Beijing 100191, Peoples R China.;[Afedulidis, O.; Fritsch, M.; Heinsius, F. H.; Kuessner, M.; Hanisch, F.; Pelizaeus, M.; Kopf, B.; Wollenberg, L.; Holtmann, T.; de Boer, R. E.; Feldbauer, F.; Wiedner, U.; Hoelzken, F.] Bochum Ruhr Univ, D-44780 Bochum, Germany.;[Achasov, M. N.; Nikolaev, I. B.; Muchnoi, N. Yu.] Budker Inst Nucl Phys SB RAS BINP, Novosibirsk 630090, Russia.;[Briere, R. A.] Carnegie Mellon Univ, Pittsburgh, PA 15213 USA.
通讯机构：
[Ablikim, M ] I;Inst High Energy Phys, Beijing 100049, Peoples R China.
摘要：
We perform the first amplitude analysis of D s + → π + π + π − π 0 decays based on data samples of electron-positron collisions recorded with the BESIII detector at center-of-mass energies between 4.128 and 4.226 GeV, corresponding to an integrated luminosity of 7.33 fb − 1 . We report the observation of D s + → f 0 ( 980 ) ρ ( 770 ) + with a statistical significance greater than 10 σ and determine the branching fractions B ( D s + → π + π + π − π 0 | non − η ) = ( 2.04 ± 0.0 8 stat ± 0.0 5 syst ) % and B ( D s + → η π + ) = ( 1.56 ± 0.0 9 stat ± 0.0 4 syst ) % . Moreover, we measure the relative branching fraction between ϕ → π + π − π 0 and ϕ → K + K − to be [ B ( ϕ ( 1020 ) → π + π − π 0 ) / B ( ϕ ( 1020 ) → K + K − ) ] = 0.230 ± 0.01 4 stat ± 0.01 0 syst ., which deviates from the world average value by more than 4 σ .
作者机构：
[Sun, Z Q; Wen, S P; Hou, G Y; Liang, H; Dai, H L; Yuan, C Z; Zhao, G; Xu, W; Zhao, L; Xiao, S Y; Ma, Q M; Lou, X C; Hou, X T; Zhang, P; Zhang, Y; Tang, G Y; Liu, F; Batozskaya, V; Liu, P L; Wang, X N; Xiang, B H; Zhang, Z D; Cao, G F; Sun, H K; Yan, X Q; Wang, Y F; Kiuchi, R; Li, Q M; Wang, Y Q; Sun, Y Z; Zhang, J Z; Zhang, J W; Zhang, J Y; Zhang, Z H; Han, T T; Yang, T; Liu, C X; Mo, X H; Hu, Y; Fang, Y Q; Hu, T; Song, W M; Zhu, Z A; Wu, Z; Zheng, W J; Chang, J F; Yuan, Y; Deng, Z Y; Lu, J G; Yu, G; Hu, H M; Zheng, J P; Zeng, Y J; Ma, R Q; Ouyang, Q; Fang, W X; Chen, T; Yuan, S C; Fu, Y W; Rong, G; Chen, G; Ding, B; Liu, B J; Zhu, K J; Hou, Z L; Ablikim, M; Xu, C F; Cai, X; Li, L K; Li, L J; Ma, H L; Qiu, J F; Jiang, D; Ma, X T; Ma, X Y; Lu, Y P; Heng, Y K; Ruan, M Q; Qin, Z H; Fang, S S; Wang, B; Sun, S S; Wang, K; Ping, R G; Du, M C; Wang, Z; Liu, H M; Liao, Y P; Zhang, S H; Mao, Z P; Yin, J H; Yu, B X; Liu, H H; Gong, W X; Kui, X; Lu, Z H; Chen, M L; Zhu, K; Chen, Z Y; Ji, X L; Zhang, B X; Ji, X B; Zhang, B L; Guan, C Y; Jing, M Q; Li, K; Li, G; Shi, J Y; Li, F; Lin, T; Zhang, A Q; Li, X; Li, H B; Lu, X L; Xu, G F; Chen, X T; Yang, H X; Gu, M H; Wang, Z Y; Zhang, Y H; Zou, J H; Li, X Y; Wu, L H; Wu, L J; Zhang, H Q; Zhou, L P; Chen, H S; Shao, L G; Fu, C D; Zhang, H C; Zhao, J Y; Zhao, J Z; Xing, T Y; Yang, Y F; Li, W D; Li, W G; He, K L; Ma, M M; Qi, F Z; Qian, S; Yang, Y X; Zhang, X M; Zhang, H Y; Zhao, Y B; Chen, Y B; Sun, G X; Wang, L L; Ning, Z; Huang, Y P; Ma, J L; Dong, L Y; Luo, X L; Che, Y Z; Jiang, X S; Fang, Y; Fang, J; Ye, M; Shen, X Y; Dong, M Y; Cao, N; Miao, H; Shi, X; Ji, Q; Wu, J F; Liu, Z A; Ji, W; Shen, H F; Xie, Y G; Dong, J; Liu, J Y] Institute of High Energy Physics, Beijing 100049, People's Republic of China;[Achasov, M N; Muchnoi, N Yu; Nikolaev, I B] Budker Institute of Nuclear Physics SB RAS (BINP), Novosibirsk 630090, Russia;[Adlarson, P; Schoenning, K; Thoren, V; Kupsc, A; Wolke, M; Johansson, T] Uppsala University, Box 516, SE-75120 Uppsala, Sweden;[Fritsch, M; Heinsius, F H; Wiedner, U; Wollenberg, L; Feldbauer, F; Hölzken, F; Afedulidis, O; Holtmann, T; Hanisch, F; Pelizaeus, M; de Boer, R E; Kopf, B; Kuessner, M] Bochum Ruhr-University, D-44780 Bochum, Germany;[Li, D M; Liu, Y; Zhang, H; Zhang, J; Du, S X; Yu, Y C; Yan, W C; Ai, X C; Zhao, S J; Ke, B C; Zhang, Y T; Ge, L; Qiao, X K] Zhengzhou University, Zhengzhou 450001, People's Republic of China
摘要：
Using e^{+}e^{-} collision data corresponding to an integrated luminosity of 19 fb^{-1} collected by the BESIII detector at center-of-mass energies ranging from 4.13 to 4.70GeV, we report the first evidence for a new excited Ω^{-} hyperon, the Ω(2109)^{-}, through the process e^{+}e^{-}→Ω(2109)^{-}Ω[over ¯]^{+}+c. c. with a significance of 4.1σ. The mass and width of Ω(2109)^{-} are measured to be 2108.5±5.2_{stat}±0.9_{syst} MeV/c^{2} and 18.3±16.4_{stat}±5.7_{syst} MeV, respectively. We also present evidence for a new production mechanism for the previously identified Ω(2012)^{-} via the process e^{+}e^{-}→Ω(2012)^{-}Ω[over ¯]^{+}+c. c. with a significance of 3.5σ.
摘要：
INTRODUCTION: The effect of diffusion-weighted magnetic resonance imaging (DWI)-guided dose-painting intensity-modulated radiation therapy (DP-IMRT) on locally advanced recurrent nasopharyngeal carcinoma (NPC) remains unclear. This study aimed to compare the outcomes and toxicities of DWI-guided DP-IMRT in patients with locally recurrent NPC. METHODS: In this prospective trial, 150 patients with locally advanced recurrent NPC were randomly assigned (1:1) to receive reirradiation with DWI-guided DP-IMRT (DWI group, n = 75) or conventional MRI-based IMRT (MRI group, n = 75). In the DWI group, DWI-guided gross tumor volume received escalation to 65.4Gy/30 fx in 2.18Gy per fraction, while in the MRI group, the planning target volume was irradiated at 60Gy/30fx in 2.0Gy per fraction. The trial was registered at Chictr.org.cn (ChiCTR2100052340) on October 24, 2021. Survival rates were compared, and multivariate analyses were conducted. RESULTS: The median follow-up duration was 16 months. Compared with the MRI group, patients in the DWI group had better 18-month progression-free survival (PFS) 75.1% vs. 53.6%; P = 0.006), local recurrence-free survival (LRFS) (83.4% vs. 61.8%; P = 0.010), and locoregional recurrence-free survival (73.1% vs. 64.9%; P = 0.025). Grade 3-4 toxicities between the two groups showed no significant difference. Multivariate analysis revealed that DWI-guided DP-IMRT was an independent prognostic factor for PFS and LRFS. CONCLUSION: Compared with conventional MRI-based IMRT, DWI-guided DP-IMRT improved PFS in patients with recurrent NPC without increasing acute and late toxic effects.
作者：
Ablikim, M.;Achasov, M. N.;Adlarson, P.;Afedulidis, O.;Ai, X. C.;...
期刊：
Journal of High Energy Physics,2025年2024(12):1-23 ISSN：1029-8479
通讯作者：
Ablikim, M
作者机构：
[Yu, B. X.; Yu, G.; Hu, T.; Ning, Z.; Zhang, P.; Wen, S. P.; Shi, X.; Sun, G. X.; Ma, M. M.; Chen, T.; Hou, X. T.; Zhu, Z. A.; Xu, G. F.; Wang, K.; Zhou, L. P.; Heng, Y. K.; Ji, Q.; Zhang, J. W.; Chen, Z. Y.; Rong, G.; Guan, C. Y.; Qi, F. Z.; Wang, Y. F.; Wang, L. L.; Ouyang, Q.; Jiang, D.; Liao, Y. P.; Zhang, A. Q.; Ji, X. B.; Qian, S.; Dong, M. Y.; Fang, S. S.; Chang, J. F.; Liu, Z. A.; Yang, T.; Yan, X. Q.; Sun, Z. Q.; Han, T. T.; Wu, J. F.; Sun, S. S.; Ding, B.; Fu, C. D.; Zhang, Y.; Lou, X. C.; Lin, T.; Zhang, B. X.; Xing, T. Y.; Cao, G. F.; Ji, W.; Wu, L. H.; Zhao, Y. B.; Fu, Y. W.; Zheng, J. P.; Jiang, X. S.; Kiuchi, R.; Fang, Y. Q.; Gu, M. H.; Lu, Y. P.; Dong, L. Y.; Zhang, H. Q.; Zhao, G.; Wu, L. J.; Li, L. J.; Yuan, Y.; Lu, X. L.; Wu, Z.; Fang, Y.; Luo, X. L.; Ji, X. L.; Zhang, X. M.; Li, X. Y.; Li, L. K.; Li, H. B.; Liu, F.; Liang, H.; Huang, Y. P.; Zhang, J. Y.; Zhao, L.; Yin, J. H.; Yang, Y. F.; Batozskaya, V.; Song, W. M.; Chen, X. T.; Zhang, J. Z.; He, K. L.; Chen, G.; Ablikim, M.; Liu, C. X.; Li, X.; Zhu, K.; Liu, H. H.; Zhao, J. Z.; Mao, Z. P.; Xiao, S. Y.; Lu, J. G.; Liu, P. L.; Jing, M. Q.; Sun, H. K.; Chen, Y. B.; Du, M. C.; Wang, Z.; Ablikim, M; Zhao, J. Y.; Dong, J.; Shi, J. Y.; Yuan, C. Z.; Tang, G. Y.; Yuan, S. C.; Zhang, H. Y.; Chen, M. L.; Zhang, Z. H.; Hou, G. Y.; Shen, H. F.; Shao, L. G.; Hou, Z. L.; Sun, Y. Z.; Liu, B. J.; Xiang, B. H.; Zhu, K. J.; Liu, H. M.; Xu, C. F.; Ma, H. L.; Ye, M.; Xie, Y. G.; Chen, H. S.; Cao, N.; Ma, X. T.; Deng, Z. Y.; Ma, Q. M.; Wang, Z. Y.; Cai, X.; Zhang, Y. H.; Ma, R. Q.; Zheng, W. J.; Zou, J. H.; Liu, J. Y.; Wang, X. N.; Kui, X.; Li, W. G.; Wang, Y. Q.; Mo, X. H.; Fang, J.; Li, Q. M.; Shen, X. Y.; Ma, X. Y.; Hu, H. M.; Li, K.; Gong, W. X.; Xu, W.; Hu, Y.; Wang, B.; Zhang, B. L.; Ma, J. L.; Yang, Y. X.; Miao, H.; Zhang, S. H.; Li, F.; Lu, Z. H.; Yang, H. X.; Qin, Z. H.; Li, G.; Ping, R. G.; Qiu, J. F.; Zhang, Z. D.; Zhang, H. C.; Dai, H. L.; Li, W. D.; Fang, W. X.; Zeng, Y. J.] Inst High Energy Phys, Beijing 100049, Peoples R China.;[Xu, H. Y.; Yuan, L.] Beihang Univ, Beijing 100191, Peoples R China.;[Afedulidis, O.; Fritsch, M.; Heinsius, F. H.; Kuessner, M.; Hanisch, F.; Pelizaeus, M.; Kopf, B.; Wollenberg, L.; Holtmann, T.; de Boer, R. E.; Feldbauer, F.; Wiedner, U.; Hoelzken, F.] Bochum Ruhr Univ, D-44780 Bochum, Germany.;[Achasov, M. N.; Nikolaev, I. B.; Muchnoi, N. Yu.] SB RAS BINP, Budker Inst Nucl Phys, Novosibirsk 630090, Russia.;[Briere, R. A.] Carnegie Mellon Univ, Pittsburgh, PA 15213 USA.
通讯机构：
[Ablikim, M ] I;Inst High Energy Phys, Beijing 100049, Peoples R China.
关键词：
e(+)-e(-) Experiments;Polarization;QCD
摘要：
Using e+e− collision data collected with the BESIII detector at seven energy points ranging from 3.68 to 3.71 GeV and corresponding to an integrated luminosity of 652.1 pb−1, we present an energy-dependent measurement of the transverse polarization, relative phase and modulus ratio of the electromagnetic form factors of the Σ+ hyperon in the e+e− →
$$ {\Sigma}^{+}{\overline{\Sigma}}^{-} $$
reaction. At each energy point, no evident polarization is observed. These results are helpful to understand the production mechanism of the Σ+-
$$ {\overline{\Sigma}}^{-} $$
pairs.
作者机构：
[Yu, B. X.; Yu, G.; Hu, T.; Ning, Z.; Zhang, P.; Wen, S. P.; Shi, X.; Sun, G. X.; Ma, M. M.; Guskov, A.; Chen, T.; Hou, X. T.; Zhu, Z. A.; Xu, G. F.; Wang, K.; Zhou, L. P.; Heng, Y. K.; Ji, Q.; Zhang, J. W.; Chen, Z. Y.; Rong, G.; Guan, C. Y.; Qi, F. Z.; Wang, Y. F.; Wang, L. L.; Ouyang, Q.; Jiang, D.; Liao, Y. P.; Zhang, A. Q.; Ji, X. B.; Qian, S.; Dong, M. Y.; Fang, S. S.; Chang, J. F.; Liu, Z. A.; Yang, T.; Yan, X. Q.; Sun, Z. Q.; Han, T. T.; Wu, J. F.; Sun, S. S.; Ding, B.; Fu, C. D.; Zhang, Y.; Lou, X. C.; Lin, T.; Zhang, B. X.; Xing, T. Y.; Cao, G. F.; Ji, W.; Wu, L. H.; Zhao, Y. B.; Fu, Y. W.; Zheng, J. P.; Jiang, X. S.; Kiuchi, R.; Fang, Y. Q.; Gu, M. H.; Lu, Y. P.; Dong, L. Y.; Zhang, H. Q.; Zhao, G.; Wu, L. J.; Li, L. J.; Yuan, Y.; Lu, X. L.; Wu, Z.; Fang, Y.; Luo, X. L.; Ji, X. L.; Zhang, X. M.; Li, X. Y.; Li, L. K.; Li, H. B.; Liu, F.; Liang, H.; Huang, Y. P.; Zhang, J. Y.; Zhao, L.; Yin, J. H.; Yang, Y. F.; Batozskaya, V.; Song, W. M.; Chen, X. T.; Zhang, J. Z.; He, K. L.; Chen, G.; Ablikim, M.; Liu, C. X.; Li, X.; Zhu, K.; Liu, H. H.; Zhao, J. Z.; Mao, Z. P.; Xiao, S. Y.; Lu, J. G.; Liu, P. L.; Jing, M. Q.; Sun, H. K.; Chen, Y. B.; Du, M. C.; Wang, Z.; Ablikim, M; Zhao, J. Y.; Dong, J.; Shi, J. Y.; Yuan, C. Z.; Tang, G. Y.; Yuan, S. C.; Zhang, H. Y.; Chen, M. L.; Zhang, Z. H.; Hou, G. Y.; Shen, H. F.; Shao, L. G.; Hou, Z. L.; Sun, Y. Z.; Liu, B. J.; Xiang, B. H.; Zhu, K. J.; Liu, H. M.; Xu, C. F.; Ma, H. L.; Ye, M.; Xie, Y. G.; Chen, H. S.; Cao, N.; Ma, X. T.; Deng, Z. Y.; Ma, Q. M.; Wang, Z. Y.; Cai, X.; Zhang, Y. H.; Ma, R. Q.; Zheng, W. J.; Zou, J. H.; Liu, J. Y.; Wang, X. N.; Kui, X.; Li, W. G.; Wang, Y. Q.; Mo, X. H.; Fang, J.; Li, Q. M.; Shen, X. Y.; Ma, X. Y.; Hu, H. M.; Li, K.; Gong, W. X.; Xu, W.; Hu, Y.; Wang, B.; Zhang, B. L.; Ma, J. L.; Yang, Y. X.; Miao, H.; Zhang, S. H.; Li, F.; Lu, Z. H.; Yang, H. X.; Qin, Z. H.; Li, G.; Ping, R. G.; Qiu, J. F.; Zhang, Z. D.; Zhang, H. C.; Dai, H. L.; Li, W. D.; Fang, W. X.; Zeng, Y. J.] Inst High Energy Phys, Beijing 100049, Peoples R China.;[Xu, H. Y.; Yuan, L.] Beihang Univ, Beijing 100191, Peoples R China.;[Afedulidis, O.; Fritsch, M.; Heinsius, F. H.; Kuessner, M.; Hanisch, F.; Pelizaeus, M.; Kopf, B.; Wollenberg, L.; Holtmann, T.; de Boer, R. E.; Feldbauer, F.; Wiedner, U.; Hoelzken, F.] Bochum Ruhr Univ, D-44780 Bochum, Germany.;[Achasov, M. N.; Nikolaev, I. B.; Muchnoi, N. Yu.] Budker Inst Nucl Phys SB RAS BINP, Novosibirsk 630090, Russia.;[Briere, R. A.] Carnegie Mellon Univ, Pittsburgh, PA 15213 USA.
通讯机构：
[Ablikim, M ] I;Inst High Energy Phys, Beijing 100049, Peoples R China.
摘要：
Based on 6.1 fb(-1) of ethorne- annihilation data collected at center-of-mass energies from 4.600 to 4.843 GeV with the BESIII detector at the BEPCII collider, a partial wave analysis of Lambda(+)(c) -> Lambda pi(+)eta is performed, and branching fractions and decay asymmetry parameters of intermediate processes are determined. The process Lambda(+)(c) -> Lambda a(0)(980)(+) is observed for the first time, and evidence for the pentaquark candidate Sigma(1380)(+) decaying into Lambda pi(+) is found with statistical significance larger than 3 sigma with mass and width fixed to theoretical predictions. The branching fraction product B[ Lambda(+)(c) -> Lambda a(0) (980)(+)]B[a(0)(980)(+) -> pi(+)eta] is determined to be (1.05 +/- 0.16(stat) +/- 0.05(syst) +/- 0.07(ext) )%, which is larger than theoretical calculations by 1-2 orders of magnitude. Here the third (external) systematic is from B(Lambda(+)(c) -> Lambda pi(+)eta). Finally, we precisely obtain the absolute branching fraction B(Lambda(+)(c) -> Lambda pi(+)eta) = (1.94 +/- 0.07(stat) +/- 0.11(syst))%.
作者：
Ablikim, M.;Achasov, M. N.;Adlarson, P.;Afedulidis, O.;Ai, X. C.;...
期刊：
Journal of High Energy Physics,2025年2025(1) ISSN：1029-8479
通讯作者：
Ablikim, M
作者机构：
[Yu, B. X.; Yu, G.; Hu, T.; Ning, Z.; Zhang, P.; Wen, S. P.; Shi, X.; Sun, G. X.; Ma, M. M.; Chen, T.; Hou, X. T.; Zhu, Z. A.; Xu, G. F.; Wang, K.; Zhou, L. P.; Heng, Y. K.; Ji, Q.; Zhang, J. W.; Chen, Z. Y.; Rong, G.; Guan, C. Y.; Qi, F. Z.; Wang, Y. F.; Wang, L. L.; Ouyang, Q.; Jiang, D.; Che, Y. Z.; Liao, Y. P.; Zhang, A. Q.; Ji, X. B.; Qian, S.; Dong, M. Y.; Fang, S. S.; Chang, J. F.; Liu, Z. A.; Yang, T.; Yan, X. Q.; Sun, Z. Q.; Han, T. T.; Wu, J. F.; Sun, S. S.; Ding, B.; Fu, C. D.; Zhang, Y.; Lou, X. C.; Lin, T.; Zhang, B. X.; Xing, T. Y.; Cao, G. F.; Ji, W.; Wu, L. H.; Zhao, Y. B.; Fu, Y. W.; Zheng, J. P.; Jiang, X. S.; Kiuchi, R.; Fang, Y. Q.; Gu, M. H.; Lu, Y. P.; Dong, L. Y.; Zhang, H. Q.; Zhao, G.; Wu, L. J.; Li, L. J.; Yuan, Y.; Lu, X. L.; Wu, Z.; Fang, Y.; Luo, X. L.; Ji, X. L.; Zhang, X. M.; Li, X. Y.; Li, L. K.; Li, H. B.; Liu, F.; Liang, H.; Huang, Y. P.; Zhang, J. Y.; Zhao, L.; Yin, J. H.; Yang, Y. F.; Batozskaya, V.; Song, W. M.; Chen, X. T.; Zhang, J. Z.; He, K. L.; Chen, G.; Ablikim, M.; Liu, C. X.; Li, X.; Zhu, K.; Liu, H. H.; Zhao, J. Z.; Mao, Z. P.; Xiao, S. Y.; Lu, J. G.; Liu, P. L.; Jing, M. Q.; Sun, H. K.; Chen, Y. B.; Du, M. C.; Wang, Z.; Ablikim, M; Zhao, J. Y.; Dong, J.; Shi, J. Y.; Ruan, M. Q.; Yuan, C. Z.; Tang, G. Y.; Yuan, S. C.; Zhang, H. Y.; Chen, M. L.; Zhang, Z. H.; Hou, G. Y.; Shen, H. F.; Shao, L. G.; Hou, Z. L.; Sun, Y. Z.; Liu, B. J.; Xiang, B. H.; Zhu, K. J.; Liu, H. M.; Xu, C. F.; Ma, H. L.; Ye, M.; Xie, Y. G.; Chen, H. S.; Cao, N.; Ma, X. T.; Deng, Z. Y.; Ma, Q. M.; Wang, Z. Y.; Cai, X.; Zhang, Y. H.; Ma, R. Q.; Zheng, W. J.; Zou, J. H.; Liu, J. Y.; Wang, X. N.; Kui, X.; Li, W. G.; Wang, Y. Q.; Mo, X. H.; Fang, J.; Li, Q. M.; Shen, X. Y.; Ma, X. Y.; Hu, H. M.; Li, K.; Gong, W. X.; Xu, W.; Hu, Y.; Wang, B.; Zhang, B. L.; Ma, J. L.; Yang, Y. X.; Miao, H.; Zhang, S. H.; Li, F.; Lu, Z. H.; Yang, H. X.; Qin, Z. H.; Li, G.; Ping, R. G.; Qiu, J. F.; Zhang, Z. D.; Zhang, H. C.; Dai, H. L.; Li, W. D.; Fang, W. X.; Zeng, Y. J.] Inst High Energy Phys, Beijing 100049, Peoples R China.;[Xu, H. Y.; Yuan, L.] Beihang Univ, Beijing 100191, Peoples R China.;[Afedulidis, O.; Fritsch, M.; Heinsius, F. H.; Kuessner, M.; Hanisch, F.; Pelizaeus, M.; Kopf, B.; Wollenberg, L.; Holtmann, T.; de Boer, R. E.; Feldbauer, F.; Wiedner, U.; Hoelzken, F.] Bochum Ruhr Univ, D-44780 Bochum, Germany.;[Achasov, M. N.; Nikolaev, I. B.; Muchnoi, N. Yu.] Budker Inst Nucl Phys SB RAS BINP, Novosibirsk 630090, Russia.;[Briere, R. A.] Carnegie Mellon Univ, Pittsburgh, PA 15213 USA.
通讯机构：
[Ablikim, M ] I;Inst High Energy Phys, Beijing 100049, Peoples R China.
关键词：
Charm Physics;e(+)-e(-) Experiments
摘要：
Abstract Based on 7.33 fb −1 of e + e − collision data collected by the BESIII detector operating at the BEPCII collider at center-of-mass energies from 4.128 to 4.226 GeV, a search for the Majorana neutrino ν m is conducted in the lepton-number-violating decays of $$ {D}_{\textrm{s}}^{+} $$ D s + → h − h 0 e + e +. Here, h − represents a K − or π − , and h 0 represents a π 0, $$ {K}_S^0 $$ K S 0 or ϕ. No significant signal is observed, and the upper limits of their branching fractions at the 90% confidence level are determined to be $$ \mathcal{B} $$ B ( $$ {D}_{\textrm{s}}^{+} $$ D s + → ϕπ − e + e +) < 6.9 × 10 −5, $$ \mathcal{B} $$ B ( $$ {D}_{\textrm{s}}^{+} $$ D s + → ϕK − e + e +) < 9.9 × 10 −5, $$ \mathcal{B} $$ B ( $$ {D}_{\textrm{s}}^{+} $$ D s + → $$ {K}_S^0 $$ K S 0 π − e + e +) < 1.3 × 10 −5, $$ \mathcal{B} $$ B ( $$ {D}_{\textrm{s}}^{+} $$ D s + → $$ {K}_S^0 $$ K S 0 K − e + e +) < 2.9 × 10 −5, $$ \mathcal{B} $$ B ( $$ {D}_{\textrm{s}}^{+} $$ D s + → π − π 0 e + e +) < 2.9 × 10 −5 and $$ \mathcal{B} $$ B ( $$ {D}_{\textrm{s}}^{+} $$ D s + → K − π 0 e + e +) < 3.4 × 10 −5. The Majorana neutrino is searched for with different mass assumptions within the range [0.20, 0.80] GeV/c 2 in the decay of $$ {D}_{\textrm{s}}^{+} $$ D s + → ϕe + ν m with ν m → π − e +, and the upper limits of the branching fractions at the 90% confidence level are at the level of 10 −5–10 −2, depending on the mass of the Majorana neutrino.
