$Analysis of the dynamics of the decay D + → K S 0 π 0 e + ν e $$ {D}^{+}\to {K}_S^0{\pi}^0{e}^{+}{\nu}_e $$$

Analysis of the dynamics of the decay D + → K S 0 π 0 e + ν e $$ {D}^{+}\to {K}_S^0{\pi}^0{e}^{+}{\nu}_e $$

Abstract The branching fraction of D + → K S 0 π 0 e + ν e $$ {D}^{+}\to {K}_S^0{\pi}^0{e}^{+}{\nu}_e $$ is measured for the first time using 7.93 fb −1 of e + e − annihilation data collected at the center-of-mass energy s $$ \sqrt{s} $$ = 3.773 GeV with the BESIII detector operating at the BEPCII c...

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Main Authors:	The BESIII collaboration, M. Ablikim, M. N. Achasov, P. Adlarson, O. Afedulidis, X. C. Ai, R. Aliberti, A. Amoroso, Q. An, Y. Bai, O. Bakina, I. Balossino, Y. Ban, H.-R. Bao, V. Batozskaya, K. Begzsuren, N. Berger, M. Berlowski, M. Bertani, D. Bettoni, F. Bianchi, E. Bianco, A. Bortone, I. Boyko, R. A. Briere, A. Brueggemann, H. Cai, X. Cai, A. Calcaterra, G. F. Cao, N. Cao, S. A. Cetin, X. Y. Chai, J. F. Chang, G. R. Che, G. Chelkov, 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. Chen, S. K. Choi, G. Cibinetto, F. Cossio, J. J. Cui, H. L. Dai, J. P. Dai, A. Dbeyssi, R. E. de Boer, D. Dedovich, C. Q. Deng, Z. Y. Deng, A. Denig, I. Denysenko, M. Destefanis, F. De Mori, B. Ding, X. X. Ding, Y. Ding, J. Dong, L. Y. Dong, M. Y. Dong, X. Dong, M. C. Du, S. X. Du, Y. Y. Duan, Z. H. Duan, P. Egorov, Y. H. Fan, J. Fang, S. S. Fang, W. X. Fang, Y. Fang, Y. Q. Fang, R. Farinelli, L. Fava, F. Feldbauer, G. Felici, C. Q. Feng, J. H. Feng, Y. T. Feng, M. Fritsch, C. D. Fu, J. L. Fu, Y. W. Fu, H. Gao, X. B. Gao, Y. N. Gao, Yang Gao, S. Garbolino, I. Garzia, L. Ge, P. T. Ge, Z. W. Ge, C. Geng, E. M. Gersabeck, A. Gilman, K. Goetzen, L. Gong, W. X. Gong, W. Gradl, S. Gramigna, M. Greco, M. H. Gu, Y. T. Gu, C. Y. Guan, A. Q. Guo, L. B. Guo, M. J. Guo, R. P. Guo, Y. P. Guo, A. Guskov, J. Gutierrez, K. L. Han, T. T. Han, F. Hanisch, X. Q. Hao, F. A. Harris, K. K. He, K. L. He, F. H. Heinsius, C. H. Heinz, Y. K. Heng, C. Herold, T. Holtmann, P. C. Hong, G. Y. Hou, X. T. Hou, Y. R. Hou, Z. L. Hou, B. Y. Hu, H. M. Hu, J. F. Hu, S. L. Hu, T. Hu, Y. Hu, G. S. Huang, K. X. Huang, L. Q. Huang, X. T. Huang, Y. P. Huang, Y. S. Huang, T. Hussain, F. Hölzken, N. Hüsken, N. in der Wiesche, J. Jackson, S. Janchiv, J. H. Jeong, Q. Ji, Q. P. Ji, W. Ji, X. B. Ji, X. L. Ji, Y. Y. Ji, X. Q. Jia, Z. K. Jia, D. Jiang, H. B. Jiang, P. C. Jiang, S. S. Jiang, T. J. Jiang, X. S. Jiang, Y. Jiang, J. B. Jiao, J. K. Jiao, Z. Jiao, S. Jin, Y. Jin, M. Q. Jing, X. M. Jing, T. Johansson, S. Kabana, N. Kalantar-Nayestanaki, X. L. Kang, X. S. Kang, M. Kavatsyuk, B. C. Ke, V. Khachatryan, A. Khoukaz, R. Kiuchi, O. B. Kolcu, B. Kopf, M. Kuessner, X. Kui, N. Kumar, A. Kupsc, W. Kühn, J. J. Lane, L. Lavezzi, T. T. Lei, Z. H. Lei, M. Lellmann, T. Lenz, C. Li, C. H. Li, Cheng Li, D. M. Li, F. Li, G. Li, H. B. Li, H. J. Li, H. N. Li, Hui Li, J. R. Li, J. S. Li, K. Li, K. L. Li, L. J. Li, L. K. Li, Lei Li, M. H. Li, P. R. Li, Q. M. Li, Q. X. Li, R. Li, S. X. Li, T. Li, W. D. Li, W. G. Li, X. Li, X. H. Li, X. L. Li, X. Y. Li, X. Z. Li, Y. G. Li, Z. J. Li, Z. Y. Li, C. Liang, H. Liang, Y. F. Liang, Y. T. Liang, G. R. Liao, Y. P. Liao, J. Libby, A. Limphirat, C. C. Lin, D. X. Lin, T. Lin, B. J. Liu, B. X. Liu, C. Liu, C. X. Liu, F. Liu, F. H. Liu, Feng Liu, G. M. Liu, H. Liu, H. B. Liu, H. H. Liu, H. M. Liu, Huihui Liu, J. B. Liu, J. Y. Liu, K. Liu, K. Y. Liu, Ke Liu, L. Liu, L. C. Liu, Lu Liu, M. H. Liu, P. L. Liu, Q. Liu, S. B. Liu, T. Liu, W. K. Liu, W. M. Liu, X. Liu, Y. Liu, Y. B. Liu, Z. A. Liu, Z. D. Liu, Z. Q. Liu, X. C. Lou, F. X. Lu, H. J. Lu, J. G. Lu, X. L. Lu, Y. Lu, Y. P. Lu, Z. H. Lu, C. L. Luo, J. R. Luo, M. X. Luo, T. Luo, X. L. Luo, X. R. Lyu, Y. F. Lyu, F. C. Ma, H. Ma, H. L. Ma, J. L. Ma, L. L. Ma, L. R. Ma, M. M. Ma, Q. M. Ma, R. Q. Ma, T. Ma, X. T. Ma, X. Y. Ma, Y. M. Ma, F. E. Maas, I. MacKay, M. Maggiora, S. Malde, Y. J. Mao, Z. P. Mao, S. Marcello, Z. X. Meng, J. G. Messchendorp, G. Mezzadri, H. Miao, T. J. Min, R. E. Mitchell, X. H. Mo, B. Moses, N. Yu. Muchnoi, J. Muskalla, Y. Nefedov, F. Nerling, L. S. Nie, I. B. Nikolaev, Z. Ning, S. Nisar, Q. L. Niu, W. D. Niu, Y. Niu, S. L. Olsen, Q. Ouyang, S. Pacetti, X. Pan, Y. Pan, A. Pathak, Y. P. Pei, M. Pelizaeus, H. P. Peng, Y. Y. Peng, K. Peters, J. L. Ping, R. G. Ping, S. Plura, V. Prasad, F. Z. Qi, H. Qi, H. R. Qi, M. Qi, T. Y. Qi, S. Qian, W. B. Qian, C. F. Qiao, X. K. Qiao, J. J. Qin, L. Q. Qin, L. Y. Qin, X. P. Qin, X. S. Qin, Z. H. Qin, J. F. Qiu, Z. H. Qu, C. F. Redmer, K. J. Ren, A. Rivetti, M. Rolo, G. Rong, Ch. Rosner, S. N. Ruan, N. Salone, A. Sarantsev, Y. Schelhaas, K. Schoenning, M. Scodeggio, K. Y. Shan, W. Shan, X. Y. Shan, Z. J. Shang, J. F. Shangguan, L. G. Shao, M. Shao, C. P. Shen, H. F. Shen, W. H. Shen, X. Y. Shen, B. A. Shi, H. Shi, H. C. Shi, J. L. Shi, J. Y. Shi, Q. Q. Shi, S. Y. Shi, X. Shi, J. J. Song, T. Z. Song, W. M. Song, Y. J. Song, Y. X. Song, S. Sosio, S. Spataro, F. Stieler, S. S Su, Y. J. Su, G. B. Sun, G. X. Sun, H. Sun, H. K. Sun, J. F. Sun, K. Sun, L. Sun, S. S. Sun, T. Sun, W. Y. Sun, Y. Sun, Y. J. Sun, Y. Z. Sun, Z. Q. Sun, Z. T. Sun, C. J. Tang, G. Y. Tang, J. Tang, M. Tang, Y. A. Tang, L. Y. Tao, Q. T. Tao, M. Tat, J. X. Teng, V. Thoren, W. H. Tian, Y. Tian, Z. F. Tian, I. Uman, Y. Wan, S. J. Wang, B. Wang, B. L. Wang, Bo Wang, D. Y. Wang, F. Wang, H. J. Wang, J. J. Wang, J. P. Wang, K. Wang, L. L. Wang, M. Wang, N. Y. Wang, S. Wang, T. Wang, T. J. Wang, W. Wang, W. P. Wang, X. Wang, X. F. Wang, X. J. Wang, X. L. Wang, X. N. Wang, Y. Wang, Y. D. Wang, Y. F. Wang, Y. L. Wang, Y. N. Wang, Y. Q. Wang, Yaqian Wang, Yi Wang, Z. Wang, Z. L. Wang, Z. Y. Wang, Ziyi Wang, D. H. Wei, F. Weidner, S. P. Wen, Y. R. Wen, U. Wiedner, G. Wilkinson, M. Wolke, L. Wollenberg, C. Wu, J. F. Wu, L. H. Wu, L. J. Wu, X. Wu, X. H. Wu, Y. Wu, Y. H. Wu, Y. J. Wu, Z. Wu, L. Xia, X. M. Xian, B. H. Xiang, T. Xiang, D. Xiao, G. Y. Xiao, S. Y. Xiao, Y. L. Xiao, Z. J. Xiao, C. Xie, X. H. Xie, Y. Xie, Y. G. Xie, Y. H. Xie, Z. P. Xie, T. Y. Xing, C. F. Xu, C. J. Xu, G. F. Xu, H. Y. Xu, M. Xu, Q. J. Xu, Q. N. Xu, W. Xu, W. L. Xu, X. P. Xu, Y. Xu, Y. C. Xu, Z. S. Xu, F. Yan, L. Yan, W. B. Yan, W. C. Yan, X. Q. Yan, H. J. Yang, H. L. Yang, H. X. Yang, T. Yang, Y. Yang, Y. F. Yang, Y. X. Yang, Z. W. Yang, Z. P. Yao, M. Ye, M. H. Ye, J. H. Yin, Junhao Yin, Z. Y. You, B. X. Yu, C. X. Yu, G. Yu, J. S. Yu, M. C. Yu, T. Yu, X. D. Yu, Y. C. Yu, C. Z. Yuan, J. Yuan, L. Yuan, S. C. Yuan, Y. Yuan, Z. Y. Yuan, C. X. Yue, A. A. Zafar, F. R. Zeng, S. H. Zeng, X. Zeng, Y. Zeng, Y. J. Zeng, X. Y. Zhai, Y. C. Zhai, Y. H. Zhan, A. Q. Zhang, B. L. Zhang, B. X. Zhang, D. H. Zhang, G. Y. Zhang, H. Zhang, H. C. Zhang, H. H. Zhang, H. Q. Zhang, H. R. Zhang, H. Y. Zhang, J. Zhang, J. J. Zhang, J. L. Zhang, J. Q. Zhang, J. S. Zhang, J. W. Zhang, J. X. Zhang, J. Y. Zhang, J. Z. Zhang, Jianyu Zhang, L. M. Zhang, Lei Zhang, P. Zhang, Q. Y. Zhang, R. Y. Zhang, S. H. Zhang, Shulei Zhang, X. M. Zhang, X. Y Zhang, X. Y. Zhang, Y. Zhang, Y. T. Zhang, Y. H. Zhang, Y. M. Zhang, Yan Zhang, Z. D. Zhang, Z. H. Zhang, Z. L. Zhang, Z. Y. Zhang, Z. Z. Zhang, G. Zhao, J. Y. Zhao, J. Z. Zhao, L. Zhao, Lei Zhao, M. G. Zhao, N. Zhao, R. P. Zhao, S. J. Zhao, Y. B. Zhao, Y. X. Zhao, Z. G. Zhao, A. Zhemchugov, B. Zheng, B. M. Zheng, J. P. Zheng, W. J. Zheng, Y. H. Zheng, B. Zhong, X. Zhong, H. Zhou, J. Y. Zhou, L. P. Zhou, S. Zhou, X. Zhou, X. K. Zhou, X. R. Zhou, X. Y. Zhou, Y. Z. Zhou, Z. C. Zhou, A. N. Zhu, J. Zhu, K. Zhu, K. J. Zhu, K. S. Zhu, L. Zhu, L. X. Zhu, S. H. Zhu, T. J. Zhu, W. D. Zhu, Y. C. Zhu, Z. A. Zhu, J. H. Zou, J. Zu
Format:	Article
Language:	English
Published:	SpringerOpen 2024-10-01
Series:	Journal of High Energy Physics
Subjects:	Branching fraction Charm Physics e +-e − Experiments
Online Access:	https://doi.org/10.1007/JHEP10(2024)199
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_version_	1850169969285791744
author	The BESIII collaboration M. Ablikim M. N. Achasov P. Adlarson O. Afedulidis X. C. Ai R. Aliberti A. Amoroso Q. An Y. Bai O. Bakina I. Balossino Y. Ban H.-R. Bao V. Batozskaya K. Begzsuren N. Berger M. Berlowski M. Bertani D. Bettoni F. Bianchi E. Bianco A. Bortone I. Boyko R. A. Briere A. Brueggemann H. Cai X. Cai A. Calcaterra G. F. Cao N. Cao S. A. Cetin X. Y. Chai J. F. Chang G. R. Che G. Chelkov 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. Chen S. K. Choi G. Cibinetto F. Cossio J. J. Cui H. L. Dai J. P. Dai A. Dbeyssi R. E. de Boer D. Dedovich C. Q. Deng Z. Y. Deng A. Denig I. Denysenko M. Destefanis F. De Mori B. Ding X. X. Ding Y. Ding Y. Ding J. Dong L. Y. Dong M. Y. Dong X. Dong M. C. Du S. X. Du Y. Y. Duan Z. H. Duan P. Egorov Y. H. Fan J. Fang J. Fang S. S. Fang W. X. Fang Y. Fang Y. Q. Fang R. Farinelli L. Fava F. Feldbauer G. Felici C. Q. Feng J. H. Feng Y. T. Feng M. Fritsch C. D. Fu J. L. Fu Y. W. Fu H. Gao X. B. Gao Y. N. Gao Yang Gao S. Garbolino I. Garzia L. Ge P. T. Ge Z. W. Ge C. Geng E. M. Gersabeck A. Gilman K. Goetzen L. Gong W. X. Gong W. Gradl S. Gramigna M. Greco M. H. Gu Y. T. Gu C. Y. Guan A. Q. Guo L. B. Guo M. J. Guo R. P. Guo Y. P. Guo A. Guskov J. Gutierrez K. L. Han T. T. Han F. Hanisch X. Q. Hao F. A. Harris K. K. He K. L. He F. H. Heinsius C. H. Heinz Y. K. Heng C. Herold T. Holtmann P. C. Hong G. Y. Hou X. T. Hou Y. R. Hou Z. L. Hou B. Y. Hu H. M. Hu J. F. Hu S. L. Hu T. Hu Y. Hu G. S. Huang K. X. Huang L. Q. Huang X. T. Huang Y. P. Huang Y. S. Huang T. Hussain F. Hölzken N. Hüsken N. in der Wiesche J. Jackson S. Janchiv J. H. Jeong Q. Ji Q. P. Ji W. Ji X. B. Ji X. L. Ji Y. Y. Ji X. Q. Jia Z. K. Jia D. Jiang H. B. Jiang P. C. Jiang S. S. Jiang T. J. Jiang X. S. Jiang Y. Jiang J. B. Jiao J. K. Jiao Z. Jiao S. Jin Y. Jin M. Q. Jing X. M. Jing T. Johansson S. Kabana N. Kalantar-Nayestanaki X. L. Kang X. S. Kang M. Kavatsyuk B. C. Ke V. Khachatryan A. Khoukaz R. Kiuchi O. B. Kolcu B. Kopf M. Kuessner X. Kui N. Kumar A. Kupsc W. Kühn J. J. Lane L. Lavezzi T. T. Lei Z. H. Lei M. Lellmann T. Lenz C. Li C. Li C. H. Li Cheng Li D. M. Li F. Li G. Li H. B. Li H. J. Li H. N. Li Hui Li J. R. Li J. S. Li K. Li K. L. Li L. J. Li L. K. Li Lei Li M. H. Li P. R. Li Q. M. Li Q. X. Li R. Li S. X. Li T. Li W. D. Li W. G. Li X. Li X. H. Li X. L. Li X. Y. Li X. Z. Li Y. G. Li Z. J. Li Z. Y. Li C. Liang H. Liang H. Liang Y. F. Liang Y. T. Liang G. R. Liao Y. P. Liao J. Libby A. Limphirat C. C. Lin D. X. Lin T. Lin B. J. Liu B. X. Liu C. Liu C. X. Liu F. Liu F. H. Liu Feng Liu G. M. Liu H. Liu H. B. Liu H. H. Liu H. M. Liu Huihui Liu J. B. Liu J. Y. Liu K. Liu K. Y. Liu Ke Liu L. Liu L. C. Liu Lu Liu M. H. Liu P. L. Liu Q. Liu S. B. Liu T. Liu W. K. Liu W. M. Liu X. Liu X. Liu Y. Liu Y. Liu Y. B. Liu Z. A. Liu Z. D. Liu Z. Q. Liu X. C. Lou F. X. Lu H. J. Lu J. G. Lu X. L. Lu Y. Lu Y. P. Lu Z. H. Lu C. L. Luo J. R. Luo M. X. Luo T. Luo X. L. Luo X. R. Lyu Y. F. Lyu F. C. Ma H. Ma H. L. Ma J. L. Ma L. L. Ma L. R. Ma M. M. Ma Q. M. Ma R. Q. Ma T. Ma X. T. Ma X. Y. Ma Y. M. Ma F. E. Maas I. MacKay M. Maggiora S. Malde Y. J. Mao Z. P. Mao S. Marcello Z. X. Meng J. G. Messchendorp G. Mezzadri H. Miao T. J. Min R. E. Mitchell X. H. Mo B. Moses N. Yu. Muchnoi J. Muskalla Y. Nefedov F. Nerling L. S. Nie I. B. Nikolaev Z. Ning S. Nisar Q. L. Niu W. D. Niu Y. Niu S. L. Olsen S. L. Olsen Q. Ouyang S. Pacetti X. Pan Y. Pan A. Pathak Y. P. Pei M. Pelizaeus H. P. Peng Y. Y. Peng K. Peters J. L. Ping R. G. Ping S. Plura V. Prasad F. Z. Qi H. Qi H. R. Qi M. Qi T. Y. Qi S. Qian W. B. Qian C. F. Qiao X. K. Qiao J. J. Qin L. Q. Qin L. Y. Qin X. P. Qin X. S. Qin Z. H. Qin J. F. Qiu Z. H. Qu C. F. Redmer K. J. Ren A. Rivetti M. Rolo G. Rong Ch. Rosner S. N. Ruan N. Salone A. Sarantsev Y. Schelhaas K. Schoenning M. Scodeggio K. Y. Shan W. Shan X. Y. Shan Z. J. Shang J. F. Shangguan L. G. Shao M. Shao C. P. Shen H. F. Shen W. H. Shen X. Y. Shen B. A. Shi H. Shi H. C. Shi J. L. Shi J. Y. Shi Q. Q. Shi S. Y. Shi X. Shi J. J. Song T. Z. Song W. M. Song Y. J. Song Y. X. Song S. Sosio S. Spataro F. Stieler S. S Su Y. J. Su G. B. Sun G. X. Sun H. Sun H. K. Sun J. F. Sun K. Sun L. Sun S. S. Sun T. Sun W. Y. Sun Y. Sun Y. J. Sun Y. Z. Sun Z. Q. Sun Z. T. Sun C. J. Tang G. Y. Tang J. Tang M. Tang Y. A. Tang L. Y. Tao Q. T. Tao M. Tat J. X. Teng V. Thoren W. H. Tian Y. Tian Z. F. Tian I. Uman Y. Wan S. J. Wang B. Wang B. L. Wang Bo Wang D. Y. Wang F. Wang H. J. Wang J. J. Wang J. P. Wang K. Wang L. L. Wang M. Wang N. Y. Wang S. Wang S. Wang T. Wang T. J. Wang W. Wang W. Wang W. P. Wang X. Wang X. F. Wang X. J. Wang X. L. Wang X. N. Wang Y. Wang Y. D. Wang Y. F. Wang Y. L. Wang Y. N. Wang Y. Q. Wang Yaqian Wang Yi Wang Z. Wang Z. L. Wang Z. Y. Wang Ziyi Wang D. H. Wei F. Weidner S. P. Wen Y. R. Wen U. Wiedner G. Wilkinson M. Wolke L. Wollenberg C. Wu J. F. Wu L. H. Wu L. J. Wu X. Wu X. H. Wu Y. Wu Y. H. Wu Y. J. Wu Z. Wu L. Xia X. M. Xian B. H. Xiang T. Xiang D. Xiao G. Y. Xiao S. Y. Xiao Y. L. Xiao Z. J. Xiao C. Xie X. H. Xie Y. Xie Y. G. Xie Y. H. Xie Z. P. Xie T. Y. Xing C. F. Xu C. J. Xu G. F. Xu H. Y. Xu M. Xu Q. J. Xu Q. N. Xu W. Xu W. L. Xu X. P. Xu Y. Xu Y. C. Xu Z. S. Xu F. Yan L. Yan W. B. Yan W. C. Yan X. Q. Yan H. J. Yang H. L. Yang H. X. Yang T. Yang Y. Yang Y. F. Yang Y. F. Yang Y. X. Yang Z. W. Yang Z. P. Yao M. Ye M. H. Ye J. H. Yin Junhao Yin Z. Y. You B. X. Yu C. X. Yu G. Yu J. S. Yu M. C. Yu T. Yu X. D. Yu Y. C. Yu C. Z. Yuan J. Yuan J. Yuan L. Yuan S. C. Yuan Y. Yuan Z. Y. Yuan C. X. Yue A. A. Zafar F. R. Zeng S. H. Zeng X. Zeng Y. Zeng Y. J. Zeng Y. J. Zeng X. Y. Zhai Y. C. Zhai Y. H. Zhan A. Q. Zhang B. L. Zhang B. X. Zhang D. H. Zhang G. Y. Zhang H. Zhang H. Zhang H. C. Zhang H. H. Zhang H. H. Zhang H. Q. Zhang H. R. Zhang H. Y. Zhang J. Zhang J. Zhang J. J. Zhang J. L. Zhang J. Q. Zhang J. S. Zhang J. W. Zhang J. X. Zhang J. Y. Zhang J. Z. Zhang Jianyu Zhang L. M. Zhang Lei Zhang P. Zhang Q. Y. Zhang R. Y. Zhang S. H. Zhang Shulei Zhang X. M. Zhang X. Y Zhang X. Y. Zhang Y. Zhang Y. Zhang Y. T. Zhang Y. H. Zhang Y. M. Zhang Yan Zhang Z. D. Zhang Z. H. Zhang Z. L. Zhang Z. Y. Zhang Z. Y. Zhang Z. Z. Zhang G. Zhao J. Y. Zhao J. Z. Zhao L. Zhao Lei Zhao M. G. Zhao N. Zhao R. P. Zhao S. J. Zhao Y. B. Zhao Y. X. Zhao Z. G. Zhao A. Zhemchugov B. Zheng B. M. Zheng J. P. Zheng W. J. Zheng Y. H. Zheng B. Zhong X. Zhong H. Zhou J. Y. Zhou L. P. Zhou S. Zhou X. Zhou X. K. Zhou X. R. Zhou X. Y. Zhou Y. Z. Zhou Z. C. Zhou A. N. Zhu J. Zhu K. Zhu K. J. Zhu K. S. Zhu L. Zhu L. X. Zhu S. H. Zhu T. J. Zhu W. D. Zhu Y. C. Zhu Z. A. Zhu J. H. Zou J. Zu
author_facet	The BESIII collaboration M. Ablikim M. N. Achasov P. Adlarson O. Afedulidis X. C. Ai R. Aliberti A. Amoroso Q. An Y. Bai O. Bakina I. Balossino Y. Ban H.-R. Bao V. Batozskaya K. Begzsuren N. Berger M. Berlowski M. Bertani D. Bettoni F. Bianchi E. Bianco A. Bortone I. Boyko R. A. Briere A. Brueggemann H. Cai X. Cai A. Calcaterra G. F. Cao N. Cao S. A. Cetin X. Y. Chai J. F. Chang G. R. Che G. Chelkov 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. Chen S. K. Choi G. Cibinetto F. Cossio J. J. Cui H. L. Dai J. P. Dai A. Dbeyssi R. E. de Boer D. Dedovich C. Q. Deng Z. Y. Deng A. Denig I. Denysenko M. Destefanis F. De Mori B. Ding X. X. Ding Y. Ding Y. Ding J. Dong L. Y. Dong M. Y. Dong X. Dong M. C. Du S. X. Du Y. Y. Duan Z. H. Duan P. Egorov Y. H. Fan J. Fang J. Fang S. S. Fang W. X. Fang Y. Fang Y. Q. Fang R. Farinelli L. Fava F. Feldbauer G. Felici C. Q. Feng J. H. Feng Y. T. Feng M. Fritsch C. D. Fu J. L. Fu Y. W. Fu H. Gao X. B. Gao Y. N. Gao Yang Gao S. Garbolino I. Garzia L. Ge P. T. Ge Z. W. Ge C. Geng E. M. Gersabeck A. Gilman K. Goetzen L. Gong W. X. Gong W. Gradl S. Gramigna M. Greco M. H. Gu Y. T. Gu C. Y. Guan A. Q. Guo L. B. Guo M. J. Guo R. P. Guo Y. P. Guo A. Guskov J. Gutierrez K. L. Han T. T. Han F. Hanisch X. Q. Hao F. A. Harris K. K. He K. L. He F. H. Heinsius C. H. Heinz Y. K. Heng C. Herold T. Holtmann P. C. Hong G. Y. Hou X. T. Hou Y. R. Hou Z. L. Hou B. Y. Hu H. M. Hu J. F. Hu S. L. Hu T. Hu Y. Hu G. S. Huang K. X. Huang L. Q. Huang X. T. Huang Y. P. Huang Y. S. Huang T. Hussain F. Hölzken N. Hüsken N. in der Wiesche J. Jackson S. Janchiv J. H. Jeong Q. Ji Q. P. Ji W. Ji X. B. Ji X. L. Ji Y. Y. Ji X. Q. Jia Z. K. Jia D. Jiang H. B. Jiang P. C. Jiang S. S. Jiang T. J. Jiang X. S. Jiang Y. Jiang J. B. Jiao J. K. Jiao Z. Jiao S. Jin Y. Jin M. Q. Jing X. M. Jing T. Johansson S. Kabana N. Kalantar-Nayestanaki X. L. Kang X. S. Kang M. Kavatsyuk B. C. Ke V. Khachatryan A. Khoukaz R. Kiuchi O. B. Kolcu B. Kopf M. Kuessner X. Kui N. Kumar A. Kupsc W. Kühn J. J. Lane L. Lavezzi T. T. Lei Z. H. Lei M. Lellmann T. Lenz C. Li C. Li C. H. Li Cheng Li D. M. Li F. Li G. Li H. B. Li H. J. Li H. N. Li Hui Li J. R. Li J. S. Li K. Li K. L. Li L. J. Li L. K. Li Lei Li M. H. Li P. R. Li Q. M. Li Q. X. Li R. Li S. X. Li T. Li W. D. Li W. G. Li X. Li X. H. Li X. L. Li X. Y. Li X. Z. Li Y. G. Li Z. J. Li Z. Y. Li C. Liang H. Liang H. Liang Y. F. Liang Y. T. Liang G. R. Liao Y. P. Liao J. Libby A. Limphirat C. C. Lin D. X. Lin T. Lin B. J. Liu B. X. Liu C. Liu C. X. Liu F. Liu F. H. Liu Feng Liu G. M. Liu H. Liu H. B. Liu H. H. Liu H. M. Liu Huihui Liu J. B. Liu J. Y. Liu K. Liu K. Y. Liu Ke Liu L. Liu L. C. Liu Lu Liu M. H. Liu P. L. Liu Q. Liu S. B. Liu T. Liu W. K. Liu W. M. Liu X. Liu X. Liu Y. Liu Y. Liu Y. B. Liu Z. A. Liu Z. D. Liu Z. Q. Liu X. C. Lou F. X. Lu H. J. Lu J. G. Lu X. L. Lu Y. Lu Y. P. Lu Z. H. Lu C. L. Luo J. R. Luo M. X. Luo T. Luo X. L. Luo X. R. Lyu Y. F. Lyu F. C. Ma H. Ma H. L. Ma J. L. Ma L. L. Ma L. R. Ma M. M. Ma Q. M. Ma R. Q. Ma T. Ma X. T. Ma X. Y. Ma Y. M. Ma F. E. Maas I. MacKay M. Maggiora S. Malde Y. J. Mao Z. P. Mao S. Marcello Z. X. Meng J. G. Messchendorp G. Mezzadri H. Miao T. J. Min R. E. Mitchell X. H. Mo B. Moses N. Yu. Muchnoi J. Muskalla Y. Nefedov F. Nerling L. S. Nie I. B. Nikolaev Z. Ning S. Nisar Q. L. Niu W. D. Niu Y. Niu S. L. Olsen S. L. Olsen Q. Ouyang S. Pacetti X. Pan Y. Pan A. Pathak Y. P. Pei M. Pelizaeus H. P. Peng Y. Y. Peng K. Peters J. L. Ping R. G. Ping S. Plura V. Prasad F. Z. Qi H. Qi H. R. Qi M. Qi T. Y. Qi S. Qian W. B. Qian C. F. Qiao X. K. Qiao J. J. Qin L. Q. Qin L. Y. Qin X. P. Qin X. S. Qin Z. H. Qin J. F. Qiu Z. H. Qu C. F. Redmer K. J. Ren A. Rivetti M. Rolo G. Rong Ch. Rosner S. N. Ruan N. Salone A. Sarantsev Y. Schelhaas K. Schoenning M. Scodeggio K. Y. Shan W. Shan X. Y. Shan Z. J. Shang J. F. Shangguan L. G. Shao M. Shao C. P. Shen H. F. Shen W. H. Shen X. Y. Shen B. A. Shi H. Shi H. C. Shi J. L. Shi J. Y. Shi Q. Q. Shi S. Y. Shi X. Shi J. J. Song T. Z. Song W. M. Song Y. J. Song Y. X. Song S. Sosio S. Spataro F. Stieler S. S Su Y. J. Su G. B. Sun G. X. Sun H. Sun H. K. Sun J. F. Sun K. Sun L. Sun S. S. Sun T. Sun W. Y. Sun Y. Sun Y. J. Sun Y. Z. Sun Z. Q. Sun Z. T. Sun C. J. Tang G. Y. Tang J. Tang M. Tang Y. A. Tang L. Y. Tao Q. T. Tao M. Tat J. X. Teng V. Thoren W. H. Tian Y. Tian Z. F. Tian I. Uman Y. Wan S. J. Wang B. Wang B. L. Wang Bo Wang D. Y. Wang F. Wang H. J. Wang J. J. Wang J. P. Wang K. Wang L. L. Wang M. Wang N. Y. Wang S. Wang S. Wang T. Wang T. J. Wang W. Wang W. Wang W. P. Wang X. Wang X. F. Wang X. J. Wang X. L. Wang X. N. Wang Y. Wang Y. D. Wang Y. F. Wang Y. L. Wang Y. N. Wang Y. Q. Wang Yaqian Wang Yi Wang Z. Wang Z. L. Wang Z. Y. Wang Ziyi Wang D. H. Wei F. Weidner S. P. Wen Y. R. Wen U. Wiedner G. Wilkinson M. Wolke L. Wollenberg C. Wu J. F. Wu L. H. Wu L. J. Wu X. Wu X. H. Wu Y. Wu Y. H. Wu Y. J. Wu Z. Wu L. Xia X. M. Xian B. H. Xiang T. Xiang D. Xiao G. Y. Xiao S. Y. Xiao Y. L. Xiao Z. J. Xiao C. Xie X. H. Xie Y. Xie Y. G. Xie Y. H. Xie Z. P. Xie T. Y. Xing C. F. Xu C. J. Xu G. F. Xu H. Y. Xu M. Xu Q. J. Xu Q. N. Xu W. Xu W. L. Xu X. P. Xu Y. Xu Y. C. Xu Z. S. Xu F. Yan L. Yan W. B. Yan W. C. Yan X. Q. Yan H. J. Yang H. L. Yang H. X. Yang T. Yang Y. Yang Y. F. Yang Y. F. Yang Y. X. Yang Z. W. Yang Z. P. Yao M. Ye M. H. Ye J. H. Yin Junhao Yin Z. Y. You B. X. Yu C. X. Yu G. Yu J. S. Yu M. C. Yu T. Yu X. D. Yu Y. C. Yu C. Z. Yuan J. Yuan J. Yuan L. Yuan S. C. Yuan Y. Yuan Z. Y. Yuan C. X. Yue A. A. Zafar F. R. Zeng S. H. Zeng X. Zeng Y. Zeng Y. J. Zeng Y. J. Zeng X. Y. Zhai Y. C. Zhai Y. H. Zhan A. Q. Zhang B. L. Zhang B. X. Zhang D. H. Zhang G. Y. Zhang H. Zhang H. Zhang H. C. Zhang H. H. Zhang H. H. Zhang H. Q. Zhang H. R. Zhang H. Y. Zhang J. Zhang J. Zhang J. J. Zhang J. L. Zhang J. Q. Zhang J. S. Zhang J. W. Zhang J. X. Zhang J. Y. Zhang J. Z. Zhang Jianyu Zhang L. M. Zhang Lei Zhang P. Zhang Q. Y. Zhang R. Y. Zhang S. H. Zhang Shulei Zhang X. M. Zhang X. Y Zhang X. Y. Zhang Y. Zhang Y. Zhang Y. T. Zhang Y. H. Zhang Y. M. Zhang Yan Zhang Z. D. Zhang Z. H. Zhang Z. L. Zhang Z. Y. Zhang Z. Y. Zhang Z. Z. Zhang G. Zhao J. Y. Zhao J. Z. Zhao L. Zhao Lei Zhao M. G. Zhao N. Zhao R. P. Zhao S. J. Zhao Y. B. Zhao Y. X. Zhao Z. G. Zhao A. Zhemchugov B. Zheng B. M. Zheng J. P. Zheng W. J. Zheng Y. H. Zheng B. Zhong X. Zhong H. Zhou J. Y. Zhou L. P. Zhou S. Zhou X. Zhou X. K. Zhou X. R. Zhou X. Y. Zhou Y. Z. Zhou Z. C. Zhou A. N. Zhu J. Zhu K. Zhu K. J. Zhu K. S. Zhu L. Zhu L. X. Zhu S. H. Zhu T. J. Zhu W. D. Zhu Y. C. Zhu Z. A. Zhu J. H. Zou J. Zu
author_sort	The BESIII collaboration
collection	DOAJ
description	Abstract The branching fraction of D + → K S 0 π 0 e + ν e $$ {D}^{+}\to {K}_S^0{\pi}^0{e}^{+}{\nu}_e $$ is measured for the first time using 7.93 fb −1 of e + e − annihilation data collected at the center-of-mass energy s $$ \sqrt{s} $$ = 3.773 GeV with the BESIII detector operating at the BEPCII collider, and is determined to be B D + → K S 0 π 0 e + ν e = 0.881 ± 0.017 stat . ± 0.016 syst . % $$ \mathcal{B}\left({D}^{+}\to {K}_S^0{\pi}^0{e}^{+}{\nu}_e\right)=\left(0.881\pm {0.017}_{\textrm{stat}.}\pm {0.016}_{\textrm{syst}.}\right)\% $$ . Based on an analysis of the D + → K S 0 π 0 e + ν e $$ {D}^{+}\to {K}_S^0{\pi}^0{e}^{+}{\nu}_e $$ decay dynamics, we observe the S-wave and P-wave components with fractions of f S-wave = (6.13 ± 0.27stat. ± 0.30syst. )% and f K ¯ ∗ 892 0 = 93.88 ± 0.27 stat . ± 0.29 syst . % $$ {f}_{{\overline{K}}^{\ast }{(892)}^0}=\left(93.88\pm {0.27}_{\textrm{stat}.}\pm {0.29}_{\textrm{syst}.}\right)\% $$ , respectively. From these results, we obtain the branching fractions B D + → K S 0 π 0 S − wave e + ν e = 5.41 ± 0.35 stat . ± 0.37 syst . × 10 − 4 $$ \mathcal{B}\left({D}^{+}\to {\left({K}_S^0{\pi}^0\right)}_{S-\textrm{wave}}{e}^{+}{\nu}_e\right)=\left(5.41\pm {0.35}_{\textrm{stat}.}\pm {0.37}_{\textrm{syst}.}\right)\times {10}^{-4} $$ and B D + → K ¯ ∗ 892 0 e + ν e = 4.97 ± 0.11 stat . ± 0.12 syst . % $$ \mathcal{B}\left({D}^{+}\to {\overline{K}}^{\ast }{(892)}^0{e}^{+}{\nu}_e\right)=\left(4.97\pm {0.11}_{\textrm{stat}.}\pm {0.12}_{\textrm{syst}.}\right)\% $$ . In addition, the hadronic form-factor ratios of D + → K ¯ ∗ 892 0 e + ν e $$ {D}^{+}\to {\overline{K}}^{\ast }{(892)}^0{e}^{+}{\nu}_e $$ at q 2 = 0, assuming a single-pole dominance parameterization, are determined to be r V = V 0 A 1 0 = 1.43 ± 0.07 stat . ± 0.03 syst . $$ {r}_V=\frac{V(0)}{A_1(0)}=1.43\pm {0.07}_{\textrm{stat}.}\pm {0.03}_{\textrm{syst}.} $$ and r 2 = A 2 0 A 1 0 = 0.72 ± 0.06 stat . ± 0.02 syst . $$ {r}_2=\frac{A_2(0)}{A_1(0)}=0.72\pm {0.06}_{\textrm{stat}.}\pm {0.02}_{\textrm{syst}.} $$ .
format	Article
id	doaj-art-5cfdc5247fe5411a9c839c6c321bd20e
institution	OA Journals
issn	1029-8479
language	English
publishDate	2024-10-01
publisher	SpringerOpen
record_format	Article
series	Journal of High Energy Physics
spelling	doaj-art-5cfdc5247fe5411a9c839c6c321bd20e2025-08-20T02:20:37ZengSpringerOpenJournal of High Energy Physics1029-84792024-10-0120241012710.1007/JHEP10(2024)199Analysis of the dynamics of the decay D + → K S 0 π 0 e + ν e $$ {D}^{+}\to {K}_S^0{\pi}^0{e}^{+}{\nu}_e $$The BESIII collaborationM. Ablikim0M. N. Achasov1P. Adlarson2O. Afedulidis3X. C. Ai4R. Aliberti5A. Amoroso6Q. An7Y. Bai8O. Bakina9I. Balossino10Y. Ban11H.-R. Bao12V. Batozskaya13K. Begzsuren14N. Berger15M. Berlowski16M. Bertani17D. Bettoni18F. Bianchi19E. Bianco20A. Bortone21I. Boyko22R. A. Briere23A. Brueggemann24H. Cai25X. Cai26A. Calcaterra27G. F. Cao28N. Cao29S. A. Cetin30X. Y. Chai31J. F. Chang32G. R. Che33G. Chelkov34C. Chen35C. H. Chen36Chao Chen37G. Chen38H. S. Chen39H. Y. Chen40M. L. Chen41S. J. Chen42S. L. Chen43S. M. Chen44T. Chen45X. R. Chen46X. T. Chen47Y. B. Chen48Y. Q. Chen49Z. J. Chen50Z. Y. Chen51S. K. Choi52G. Cibinetto53F. Cossio54J. J. Cui55H. L. Dai56J. P. Dai57A. Dbeyssi58R. E. de Boer59D. Dedovich60C. Q. Deng61Z. Y. Deng62A. Denig63I. Denysenko64M. Destefanis65F. De Mori66B. Ding67X. X. Ding68Y. Ding69Y. Ding70J. Dong71L. Y. Dong72M. Y. Dong73X. Dong74M. C. Du75S. X. Du76Y. Y. Duan77Z. H. Duan78P. Egorov79Y. H. Fan80J. Fang81J. Fang82S. S. Fang83W. X. Fang84Y. Fang85Y. Q. Fang86R. Farinelli87L. Fava88F. Feldbauer89G. Felici90C. Q. Feng91J. H. Feng92Y. T. Feng93M. Fritsch94C. D. Fu95J. L. Fu96Y. W. Fu97H. Gao98X. B. Gao99Y. N. Gao100Yang Gao101S. Garbolino102I. Garzia103L. Ge104P. T. Ge105Z. W. Ge106C. Geng107E. M. Gersabeck108A. Gilman109K. Goetzen110L. Gong111W. X. Gong112W. Gradl113S. Gramigna114M. Greco115M. H. Gu116Y. T. Gu117C. Y. Guan118A. Q. Guo119L. B. Guo120M. J. Guo121R. P. Guo122Y. P. Guo123A. Guskov124J. Gutierrez125K. L. Han126T. T. Han127F. Hanisch128X. Q. Hao129F. A. Harris130K. K. He131K. L. He132F. H. Heinsius133C. H. Heinz134Y. K. Heng135C. Herold136T. Holtmann137P. C. Hong138G. Y. Hou139X. T. Hou140Y. R. Hou141Z. L. Hou142B. Y. Hu143H. M. Hu144J. F. Hu145S. L. Hu146T. Hu147Y. Hu148G. S. Huang149K. X. Huang150L. Q. Huang151X. T. Huang152Y. P. Huang153Y. S. Huang154T. Hussain155F. Hölzken156N. Hüsken157N. in der Wiesche158J. Jackson159S. Janchiv160J. H. Jeong161Q. Ji162Q. P. Ji163W. Ji164X. B. Ji165X. L. Ji166Y. Y. Ji167X. Q. Jia168Z. K. Jia169D. Jiang170H. B. Jiang171P. C. Jiang172S. S. Jiang173T. J. Jiang174X. S. Jiang175Y. Jiang176J. B. Jiao177J. K. Jiao178Z. Jiao179S. Jin180Y. Jin181M. Q. Jing182X. M. Jing183T. Johansson184S. Kabana185N. Kalantar-Nayestanaki186X. L. Kang187X. S. Kang188M. Kavatsyuk189B. C. Ke190V. Khachatryan191A. Khoukaz192R. Kiuchi193O. B. Kolcu194B. Kopf195M. Kuessner196X. Kui197N. Kumar198A. Kupsc199W. Kühn200J. J. Lane201L. Lavezzi202T. T. Lei203Z. H. Lei204M. Lellmann205T. Lenz206C. Li207C. Li208C. H. Li209Cheng Li210D. M. Li211F. Li212G. Li213H. B. Li214H. J. Li215H. N. Li216Hui Li217J. R. Li218J. S. Li219K. Li220K. L. Li221L. J. Li222L. K. Li223Lei Li224M. H. Li225P. R. Li226Q. M. Li227Q. X. Li228R. 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MacKay319M. Maggiora320S. Malde321Y. J. Mao322Z. P. Mao323S. Marcello324Z. X. Meng325J. G. Messchendorp326G. Mezzadri327H. Miao328T. J. Min329R. E. Mitchell330X. H. Mo331B. Moses332N. Yu. Muchnoi333J. Muskalla334Y. Nefedov335F. Nerling336L. S. Nie337I. B. Nikolaev338Z. Ning339S. Nisar340Q. L. Niu341W. D. Niu342Y. Niu343S. L. Olsen344S. L. Olsen345Q. Ouyang346S. Pacetti347X. Pan348Y. Pan349A. Pathak350Y. P. Pei351M. Pelizaeus352H. P. Peng353Y. Y. Peng354K. Peters355J. L. Ping356R. G. Ping357S. Plura358V. Prasad359F. Z. Qi360H. Qi361H. R. Qi362M. Qi363T. Y. Qi364S. Qian365W. B. Qian366C. F. Qiao367X. K. Qiao368J. J. Qin369L. Q. Qin370L. Y. Qin371X. P. Qin372X. S. Qin373Z. H. Qin374J. F. Qiu375Z. H. Qu376C. F. Redmer377K. J. Ren378A. Rivetti379M. Rolo380G. Rong381Ch. Rosner382S. N. Ruan383N. Salone384A. Sarantsev385Y. Schelhaas386K. Schoenning387M. Scodeggio388K. Y. Shan389W. Shan390X. Y. Shan391Z. J. Shang392J. F. Shangguan393L. G. Shao394M. Shao395C. P. Shen396H. F. Shen397W. H. 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Zu667Institute of High Energy PhysicsBudker Institute of Nuclear Physics SB RAS (BINP)Uppsala UniversityBochum Ruhr-UniversityZhengzhou UniversityJohannes Gutenberg University of MainzUniversity of TurinUniversity of Science and Technology of ChinaSoutheast UniversityJoint Institute for Nuclear ResearchINFN Sezione di FerraraPeking UniversityUniversity of Chinese Academy of SciencesInstitute of High Energy PhysicsInstitute of Physics and TechnologyJohannes Gutenberg University of MainzNational Centre for Nuclear ResearchINFN Laboratori Nazionali di FrascatiINFN Sezione di FerraraUniversity of TurinUniversity of TurinUniversity of TurinJoint Institute for Nuclear ResearchCarnegie Mellon UniversityUniversity of MuensterWuhan UniversityInstitute of High Energy PhysicsINFN Laboratori Nazionali di FrascatiInstitute of High Energy PhysicsInstitute of High Energy PhysicsTurkish Accelerator Center Particle Factory Group, Istinye UniversityPeking UniversityInstitute of High Energy PhysicsNankai 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LaboratoryFudan UniversityHunan UniversityInstitute of High Energy PhysicsSun Yat-Sen UniversityJilin UniversityShandong UniversitySun Yat-Sen UniversityInstitute of High Energy PhysicsInstitute of High Energy PhysicsInstitute of High Energy PhysicsNankai UniversityHenan Normal UniversityZhengzhou UniversityUniversity of Science and Technology of ChinaInstitute of High Energy PhysicsJilin UniversitySun Yat-Sen UniversityInstitute of High Energy PhysicsUniversity of Science and Technology of ChinaInstitute of High Energy PhysicsZhengzhou UniversitySun Yat-Sen UniversityShanxi Normal UniversityHenan UniversityNanjing Normal UniversityFudan UniversityInstitute of High Energy PhysicsLanzhou UniversityInstitute of High Energy PhysicsInstitute of High Energy PhysicsUniversity of Chinese Academy of SciencesTsinghua UniversityNanjing UniversityInstitute of High Energy PhysicsJilin UniversityLanzhou UniversityInstitute of High Energy PhysicsHunan UniversityInstitute of High Energy PhysicsLiaoning UniversityShandong UniversityUniversity of South ChinaInstitute of High Energy PhysicsZhengzhou UniversityInstitute of High Energy PhysicsLiaoning Normal UniversityUniversity of Science and Technology of ChinaInstitute of High Energy PhysicsInstitute of High Energy PhysicsJilin UniversityNankai UniversityWuhan UniversityNorth China Electric Power UniversityInstitute of High Energy PhysicsInstitute of High Energy PhysicsInstitute of High Energy PhysicsInstitute of High Energy PhysicsUniversity of Science and Technology of ChinaNankai UniversityYunnan UniversityUniversity of Chinese Academy of SciencesZhengzhou UniversityInstitute of High Energy PhysicsInstitute of Modern PhysicsUniversity of Science and Technology of ChinaJoint Institute for Nuclear ResearchUniversity of South ChinaJilin UniversityInstitute of High Energy PhysicsInstitute of High Energy PhysicsUniversity of Chinese Academy of SciencesNanjing Normal UniversitySun Yat-Sen UniversityShandong UniversityJilin UniversityInstitute of High Energy PhysicsCentral China Normal UniversityWuhan UniversityCentral China Normal UniversityUniversity of Science and Technology of ChinaLiaoning Normal UniversityFudan UniversityHenan UniversityUniversity of Chinese Academy of SciencesNankai UniversityInstitute of High Energy PhysicsInstitute of High Energy PhysicsFudan UniversityJilin UniversityUniversity of Chinese Academy of SciencesUniversity of Science and Technology LiaoningFudan UniversityNanjing Normal UniversityUniversity of Science and Technology of ChinaInstitute of High Energy PhysicsInstitute of High Energy PhysicsUniversity of Science and Technology of ChinaAbstract The branching fraction of D + → K S 0 π 0 e + ν e $$ {D}^{+}\to {K}_S^0{\pi}^0{e}^{+}{\nu}_e $$ is measured for the first time using 7.93 fb −1 of e + e − annihilation data collected at the center-of-mass energy s $$ \sqrt{s} $$ = 3.773 GeV with the BESIII detector operating at the BEPCII collider, and is determined to be B D + → K S 0 π 0 e + ν e = 0.881 ± 0.017 stat . ± 0.016 syst . % $$ \mathcal{B}\left({D}^{+}\to {K}_S^0{\pi}^0{e}^{+}{\nu}_e\right)=\left(0.881\pm {0.017}_{\textrm{stat}.}\pm {0.016}_{\textrm{syst}.}\right)\% $$ . Based on an analysis of the D + → K S 0 π 0 e + ν e $$ {D}^{+}\to {K}_S^0{\pi}^0{e}^{+}{\nu}_e $$ decay dynamics, we observe the S-wave and P-wave components with fractions of f S-wave = (6.13 ± 0.27stat. ± 0.30syst. )% and f K ¯ ∗ 892 0 = 93.88 ± 0.27 stat . ± 0.29 syst . % $$ {f}_{{\overline{K}}^{\ast }{(892)}^0}=\left(93.88\pm {0.27}_{\textrm{stat}.}\pm {0.29}_{\textrm{syst}.}\right)\% $$ , respectively. From these results, we obtain the branching fractions B D + → K S 0 π 0 S − wave e + ν e = 5.41 ± 0.35 stat . ± 0.37 syst . × 10 − 4 $$ \mathcal{B}\left({D}^{+}\to {\left({K}_S^0{\pi}^0\right)}_{S-\textrm{wave}}{e}^{+}{\nu}_e\right)=\left(5.41\pm {0.35}_{\textrm{stat}.}\pm {0.37}_{\textrm{syst}.}\right)\times {10}^{-4} $$ and B D + → K ¯ ∗ 892 0 e + ν e = 4.97 ± 0.11 stat . ± 0.12 syst . % $$ \mathcal{B}\left({D}^{+}\to {\overline{K}}^{\ast }{(892)}^0{e}^{+}{\nu}_e\right)=\left(4.97\pm {0.11}_{\textrm{stat}.}\pm {0.12}_{\textrm{syst}.}\right)\% $$ . In addition, the hadronic form-factor ratios of D + → K ¯ ∗ 892 0 e + ν e $$ {D}^{+}\to {\overline{K}}^{\ast }{(892)}^0{e}^{+}{\nu}_e $$ at q 2 = 0, assuming a single-pole dominance parameterization, are determined to be r V = V 0 A 1 0 = 1.43 ± 0.07 stat . ± 0.03 syst . $$ {r}_V=\frac{V(0)}{A_1(0)}=1.43\pm {0.07}_{\textrm{stat}.}\pm {0.03}_{\textrm{syst}.} $$ and r 2 = A 2 0 A 1 0 = 0.72 ± 0.06 stat . ± 0.02 syst . $$ {r}_2=\frac{A_2(0)}{A_1(0)}=0.72\pm {0.06}_{\textrm{stat}.}\pm {0.02}_{\textrm{syst}.} $$ .https://doi.org/10.1007/JHEP10(2024)199Branching fractionCharm Physicse +-e − Experiments
spellingShingle	The BESIII collaboration M. Ablikim M. N. Achasov P. Adlarson O. Afedulidis X. C. Ai R. Aliberti A. Amoroso Q. An Y. Bai O. Bakina I. Balossino Y. Ban H.-R. Bao V. Batozskaya K. Begzsuren N. Berger M. Berlowski M. Bertani D. Bettoni F. Bianchi E. Bianco A. Bortone I. Boyko R. A. Briere A. Brueggemann H. Cai X. Cai A. Calcaterra G. F. Cao N. Cao S. A. Cetin X. Y. Chai J. F. Chang G. R. Che G. Chelkov 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. Chen S. K. Choi G. Cibinetto F. Cossio J. J. Cui H. L. Dai J. P. Dai A. Dbeyssi R. E. de Boer D. Dedovich C. Q. Deng Z. Y. Deng A. Denig I. Denysenko M. Destefanis F. De Mori B. Ding X. X. Ding Y. Ding Y. Ding J. Dong L. Y. Dong M. Y. Dong X. Dong M. C. Du S. X. Du Y. Y. Duan Z. H. Duan P. Egorov Y. H. Fan J. Fang J. Fang S. S. Fang W. X. Fang Y. Fang Y. Q. Fang R. Farinelli L. Fava F. Feldbauer G. 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Zhang J. Y. Zhang J. Z. Zhang Jianyu Zhang L. M. Zhang Lei Zhang P. Zhang Q. Y. Zhang R. Y. Zhang S. H. Zhang Shulei Zhang X. M. Zhang X. Y Zhang X. Y. Zhang Y. Zhang Y. Zhang Y. T. Zhang Y. H. Zhang Y. M. Zhang Yan Zhang Z. D. Zhang Z. H. Zhang Z. L. Zhang Z. Y. Zhang Z. Y. Zhang Z. Z. Zhang G. Zhao J. Y. Zhao J. Z. Zhao L. Zhao Lei Zhao M. G. Zhao N. Zhao R. P. Zhao S. J. Zhao Y. B. Zhao Y. X. Zhao Z. G. Zhao A. Zhemchugov B. Zheng B. M. Zheng J. P. Zheng W. J. Zheng Y. H. Zheng B. Zhong X. Zhong H. Zhou J. Y. Zhou L. P. Zhou S. Zhou X. Zhou X. K. Zhou X. R. Zhou X. Y. Zhou Y. Z. Zhou Z. C. Zhou A. N. Zhu J. Zhu K. Zhu K. J. Zhu K. S. Zhu L. Zhu L. X. Zhu S. H. Zhu T. J. Zhu W. D. Zhu Y. C. Zhu Z. A. Zhu J. H. Zou J. Zu Analysis of the dynamics of the decay D + → K S 0 π 0 e + ν e $$ {D}^{+}\to {K}_S^0{\pi}^0{e}^{+}{\nu}_e $$ Journal of High Energy Physics Branching fraction Charm Physics e +-e − Experiments
title	Analysis of the dynamics of the decay D + → K S 0 π 0 e + ν e $$ {D}^{+}\to {K}_S^0{\pi}^0{e}^{+}{\nu}_e $$
title_full	Analysis of the dynamics of the decay D + → K S 0 π 0 e + ν e $$ {D}^{+}\to {K}_S^0{\pi}^0{e}^{+}{\nu}_e $$
title_fullStr	Analysis of the dynamics of the decay D + → K S 0 π 0 e + ν e $$ {D}^{+}\to {K}_S^0{\pi}^0{e}^{+}{\nu}_e $$
title_full_unstemmed	Analysis of the dynamics of the decay D + → K S 0 π 0 e + ν e $$ {D}^{+}\to {K}_S^0{\pi}^0{e}^{+}{\nu}_e $$
title_short	Analysis of the dynamics of the decay D + → K S 0 π 0 e + ν e $$ {D}^{+}\to {K}_S^0{\pi}^0{e}^{+}{\nu}_e $$
title_sort	analysis of the dynamics of the decay d k s 0 π 0 e ν e d to k s 0 pi 0 e nu e
topic	Branching fraction Charm Physics e +-e − Experiments
url	https://doi.org/10.1007/JHEP10(2024)199
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analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT prli analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT qmli analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT qxli analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT rli analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT sxli analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT tli analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT wdli analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT wgli analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xli analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xhli analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xlli analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xyli analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xzli analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ygli analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zjli analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zyli analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT cliang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hliang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hliang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yfliang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ytliang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT grliao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ypliao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jlibby analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT alimphirat analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT cclin analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT dxlin analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT tlin analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT bjliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT bxliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT cliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT cxliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT fliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT fhliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT fengliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT gmliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hbliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hhliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hmliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT huihuiliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jbliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jyliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT kliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT kyliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT keliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT lliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT lcliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT luliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT mhliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT plliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT qliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT sbliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT tliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT wkliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT wmliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ybliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zaliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zdliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zqliu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xclou analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT fxlu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hjlu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jglu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xllu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ylu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yplu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zhlu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT clluo analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jrluo analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT mxluo analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT tluo analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xlluo analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xrlyu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yflyu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT fcma analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hma analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hlma analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jlma analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT llma analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT lrma analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT mmma analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT qmma analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT rqma analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT tma analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xtma analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xyma analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ymma analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT femaas analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT imackay analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT mmaggiora analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT smalde analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yjmao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zpmao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT smarcello analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zxmeng analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jgmesschendorp analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT gmezzadri analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hmiao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT tjmin analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT remitchell analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xhmo analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT bmoses analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT nyumuchnoi analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jmuskalla analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ynefedov analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT fnerling analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT lsnie analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ibnikolaev analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zning analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT snisar analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT qlniu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT wdniu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yniu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT slolsen analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT slolsen analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT qouyang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT spacetti analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xpan analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ypan analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT apathak analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yppei analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT mpelizaeus analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hppeng analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yypeng analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT kpeters analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jlping analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT rgping analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT splura analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT vprasad analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT fzqi analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hqi analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hrqi analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT mqi analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT tyqi analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT sqian analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT wbqian analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT cfqiao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xkqiao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jjqin analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT lqqin analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT lyqin analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xpqin analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xsqin analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zhqin analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jfqiu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zhqu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT cfredmer analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT kjren analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT arivetti analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT mrolo analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT grong analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT chrosner analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT snruan analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT nsalone analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT asarantsev analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yschelhaas analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT kschoenning analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT mscodeggio analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT kyshan analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT wshan analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xyshan analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zjshang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jfshangguan analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT lgshao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT mshao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT cpshen analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hfshen analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT whshen analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xyshen analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT bashi analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hshi analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hcshi analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jlshi analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jyshi analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT qqshi analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT syshi analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xshi analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jjsong analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT tzsong analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT wmsong analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yjsong analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yxsong analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ssosio analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT sspataro analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT fstieler analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT sssu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yjsu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT gbsun analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT gxsun analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hsun analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hksun analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jfsun analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ksun analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT lsun analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT sssun analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT tsun analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT wysun analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ysun analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yjsun analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yzsun analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zqsun analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ztsun analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT cjtang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT gytang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jtang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT mtang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yatang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT lytao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT qttao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT mtat analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jxteng analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT vthoren analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT whtian analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ytian analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zftian analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT iuman analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ywan analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT sjwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT bwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT blwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT bowang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT dywang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT fwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hjwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jjwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jpwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT kwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT llwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT mwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT nywang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT swang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT swang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT twang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT tjwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT wwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT wwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT wpwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xfwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xjwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xlwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xnwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ywang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ydwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yfwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ylwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ynwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yqwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yaqianwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yiwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zlwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zywang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ziyiwang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT dhwei analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT fweidner analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT spwen analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yrwen analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT uwiedner analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT gwilkinson analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT mwolke analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT lwollenberg analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT cwu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jfwu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT lhwu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ljwu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xwu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xhwu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ywu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yhwu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yjwu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zwu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT lxia analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xmxian analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT bhxiang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT txiang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT dxiao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT gyxiao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT syxiao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ylxiao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zjxiao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT cxie analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xhxie analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yxie analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ygxie analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yhxie analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zpxie analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT tyxing analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT cfxu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT cjxu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT gfxu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hyxu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT mxu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT qjxu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT qnxu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT wxu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT wlxu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xpxu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yxu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ycxu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zsxu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT fyan 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analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT mhye analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jhyin analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT junhaoyin analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zyyou analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT bxyu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT cxyu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT gyu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jsyu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT mcyu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT tyu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xdyu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ycyu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT czyuan analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jyuan analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jyuan analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT lyuan analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT scyuan analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yyuan analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zyyuan analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT cxyue analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT aazafar analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT frzeng analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT shzeng analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xzeng analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yzeng analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yjzeng analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yjzeng analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xyzhai analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yczhai analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yhzhan analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT aqzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT blzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT bxzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT dhzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT gyzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hczhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hhzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hhzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hqzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hrzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hyzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jjzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jlzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jqzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jszhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jwzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jxzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jyzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jzzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jianyuzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT lmzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT leizhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT pzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT qyzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ryzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT shzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT shuleizhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xmzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xyzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xyzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ytzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yhzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ymzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yanzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zdzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zhzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zlzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zyzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zyzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zzzhang analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT gzhao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jyzhao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jzzhao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT lzhao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT leizhao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT mgzhao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT nzhao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT rpzhao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT sjzhao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT ybzhao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yxzhao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zgzhao analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT azhemchugov analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT bzheng analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT bmzheng analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jpzheng analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT wjzheng analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yhzheng analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT bzhong analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xzhong analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT hzhou analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jyzhou analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT lpzhou analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT szhou analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xzhou analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xkzhou analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xrzhou analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT xyzhou analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yzzhou analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zczhou analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT anzhu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jzhu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT kzhu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT kjzhu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT kszhu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT lzhu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT lxzhu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT shzhu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT tjzhu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT wdzhu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT yczhu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT zazhu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jhzou analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue AT jzu analysisofthedynamicsofthedecaydks0p0enedtoks0pi0enue

Analysis of the dynamics of the decay D + → K S 0 π 0 e + ν e $$ {D}^{+}\to {K}_S^0{\pi}^0{e}^{+}{\nu}_e $$

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