2026
article
First evidence of $X(3872)\toπ^0χ_{c0}(1P)$ and search for $X(3915)\toπ^0χ_{c1}(1P)$
M Abumusabh, I Adachi, N Althubiti, T Fillinger, C Finck, G. Finocchiaro, F. Forti, A Frey, B. G. Fulsom, A Gabrielli, P. Gagneja, E Ganiev, R Garg, K Amos, A. Garmash, G Gaudino, V. Gaur, V Gautam, A. Gaz, A Gellrich, G Ghevondyan, D Ghosh, H Ghumaryan, R. Giordano, M. Angelsmark, A Giri, P. Gironella Gironell, B Gobbo, R Godang, O Gogota, W Gradl, E Graziani, D Greenwald, K Gudkova, Y Han, N. Anh Ky, K Hayasaka, H Hayashii, S. Hazra, C. Hearty, M. T. Hedges, A Heidelbach, G Heine, I. Heredia de la Cruz, T Higuchi, M. Hoek, C. Antonioli, M Hohmann, R Hoppe, P Horak, X. T. Hou, C.-L. Hsu, T Humair, T Iijima, K Inami, N Ipsita, A Ishikawa, K. Arai, R Itoh, M Iwasaki, P Jackson, D Jacobi, W W Jacobs, E.-J. Jang, S Jia, Y Jin, A Johnson, K. K. Joo, H Atmacan, H. Kakuno, K. H. Kang, G Karyan, T. Kawasaki, F. Keil, C. Ketter, C Kiesling, C Kim, D. Y. Kim, H Kim, T. Aushev, J.-Y. Kim, K.-H. Kim, H. Kindo, K Kinoshita, P Kodyš, T Koga, S Kohani, A Korobov, S. Korpar, E. Kovalenko, T. Aushev, R. Kowalewski, P Križan, P Krokovny, T Kuhr, Y Kulii, R Kumar, K. Kumara, T Kunigo, S Kurokawa, A. Kuzmin, R Ayad, Y. Kwon, S. Lacaprara, Y.-T. Lai, T Lam, C. Lange, T. S. Lau, R Leboucher, H Lee, M. J. Lee, P Leo, A. Aggarwal, V Babu, P. M. Lewis, C Li, L. K. Li, Q. M. Li, S. X. Li, W. Z. Li, Y Li, Y. B. Li, J Libby, H Bae, J. Lin, Z. Liptak, V. Lisovskyi, C Liu, G. Liu, M. H. Liu, Q Liu, D. Liventsev, S. Longo, A Lozar, N. K. Baghel, T. Lueck, C. Lyu, J. L., Y. Ma, M Maggiora, S. P. Maharana, R Maiti, G Mancinelli, R Manfredi, E Manoni, S. Bahinipati, M Mantovano, D Marcantonio, S Marcello, M Marfoli, C. Marinas, C. Martellini, A Martens, T Martinov, L Massaccesi, M. Masuda, P. Bambade, T Matsuda, D Matvienko, S. K. Maurya, M Maushart, J. A. McKenna, Z. Mediankin Gruberová, R Mehta, F Meier, D Meleshko, M Merola, P. Banerjee, C Miller, M Mirra, K Miyabayashi, H Miyake, R Mizuk, G. B. Mohanty, S Moneta, A. L. Moreira de Carvalho, H.-G. Moser, N. Mudgal, M. Barrett, Th. Muller, H Murakami, R Mussa, K. R. Nakamura, M Nakao, Y. Nakazawa, Z Natkaniec, A Natochii, M. Nayak, M Neu, M Bartl, S Nishida, R Nomaru, S Ogawa, R. Okubo, H. Ono, Y Onuki, G Pakhlova, S Pardi, H. Park, K Park, J Baudot, S T Park, A. Passeri, S Patra, T. K. Pedlar, L. E. Piilonen, P. L. M. Podesta-Lerma, T Podobnik, L. Polat, A Prakash, R. pramanik, A Beaubien, V. Prasad, C Praz, S Prell, E Prencipe, M. T. Prim, I. Prudiiev, H Purwar, P Rados, S Raiz, K Ravindran, H. Ahmed, F Becherer, J. U. Rehman, M Reif, S Reiter, M. Remnev, L Reuter, D. Ricalde Herrmann, I Ripp-Baudot, S Robertson, J. M. Roney, A. Rostomyan, J Becker, N Rout, G. Russo, S Saha, D. A. Sanders, S. Sandilya, L Santelj, C Santos, V Savinov, B. Scavino, J. Schmitz, G.F. Benfratello, S. Schneider, G Schnell, K. Schoenning, C Schwanda, Y Seino, K Senyo, J Serrano, C Sfienti, W. Shan, C. P. Shen, J. V. Bennett, X. D. Shi, T Shillington, T Shimasaki, J.-G. Shiu, D Shtol, B Shwartz, A Sibidanov, F. Simon, J. B. Singh, J Skorupa, F. U. Bernlochner, A Soffer, A Sokolov, E Solovieva, S. Spataro, K Špenko, B Spruck, M Starič, P Stavroulakis, S Stefkova, R. Stroili, V Bertacchi, M Sumihama, M. Takahashi, M. Takizawa, U Tamponi, S. S. Tang, K Tanida, F Testa, A Thaller, D. V. Thanh, T. Tien Manh, M Bertemes, O Tittel, R Tiwary, E. Torassa, F. F. Trantou, I Tsaklidis, M Uchida, I Ueda, T. Uglov, K. Unger, Y Unno, E Bertholet, K Uno, S Uno, Y Ushiroda, R van Tonder, K. E. Varvell, M Veronesi, A. Vinokurova, V Vismaya, L Vitale, V Vobbilisetti, M Bessner, R Volpe, M Wakai, S Wallner, M.-Z. Wang, A Warburton, M. Watanabe, S Watanuki, C. Wessel, X Xu, B. D. Yabsley, S Bettarini, S Yamada, W L Yan, J Yelton, K Yi, J. H. Yin, K Yoshihara, C. Z. Yuan, J Yuan, L Yuan, Y Ahn, V Bhardwaj, Y Yusa, L Zani, F. Zeng, M. Zeyrek, B Zhang, X Zhao, V Zhilich, Jin Zhou, Q. D. Zhou, X.J. Zhou, B. Bhuyan, L Zhu, R Žlebčík, Belle-II Collaboration, Belle Collaboration, F Bianchi, T Bilka, D. Biswas, D Bodrov, G Bonvicini, A Boschetti, A. Bozek, M Bračko, H Aihara, P Branchini, R. A. Briere, T. E. Browder, A. Budano, S Bussino, F Callet, Q Campagna, M Campajola, M. Carminati, G Casarosa, M. Akdag, C. Cecchi, P Cheema, C. Chen, L Chen, B. G. Cheon, C Cheshta, H Chetri, K Chilikin, K. Chirapatpimol, H.-E. Cho, N. Akopov, K Cho, S.-J. Cho, S.-K. Choi, S Choudhury, S Chutia, J Cochran, J.A. Colorado-Caicedo, I Consigny, L. Corona, S Cuccuini, S Alghamdi, J. X. Cui, E de la Cruz-Burelo, S Motte, G de Nardo, G de Pietro, R de Sangro, M Destefanis, S. Dey, R Dhayal, A Di Canto, M Alhakami, J Dingfelder, Z Doležal, X Dong, M Dorigo, G Dujany, P Ecker, J Eppelt, R Farkas, P Feichtinger, T Ferber
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Le résumé fourni par la source
We search for the pionic transitions $X(3872)\toπ^0χ_{cJ}(1P)$$(J = 0,~1,~2)$ and $X(3915)\toπ^0χ_{c1}$ in $B^+\to π^0χ_{cJ}K^+$ decays using the Belle and Belle~II data samples collected at the $Υ(4S)$ resonance, corresponding to integrated luminosities of $711~\mathrm{fb}^{-1}$ and $492~\mathrm{fb}^{-1}$, respectively. We report the first evidence for the decay $X(3872)\toπ^0χ_{c0}$ with a significance of $3.4σ$, including systematic uncertainties. We measure the product of branching fractions ${\cal B}(B^+\to X(3872)K^+)\times{\cal B}(X(3872)\toπ^0χ_{c0})=(20.0\pm6.8\pm2.3)\times10^{-6}$ and the branching fraction ratio ${\cal B}(X(3872)\toπ^0χ_{c0})/{\cal B}(X(3872)\toπ^+π^-J/ψ)=2.3\pm0.8\pm0.4$, where the first and second uncertainties are statistical and systematic, respectively. The upper limits at 90% credibility on the products of branching fractions for the $π^0χ_{c1}$ and $π^0χ_{c2}$ modes are $7.5\times10^{-6}$ and $15.3\times10^{-6}$, respectively. The corresponding upper limits on the branching fraction ratios relative to the $π^+π^-J/ψ$ decay are $0.9$ and $1.8$. The measured branching fractions for $X(3872)\toπ^0χ_{cJ}$ are consistent with several theoretical predictions based on the hadronic molecular interpretation of the $X(3872)$. No significant signal is seen for the $X(3915)\toπ^0χ_{c1}$ decay, and we set the 90% credibility upper limit of ${\cal B}(B^+\to X(3915)K^+)\times{\cal B}(X(3915)\toπ^0χ_{c1})<6.6\times10^{-6}$, while the decays for $J=0$ and 2 are forbidden by parity conservation.
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Les sujets associés
Quantum Chromodynamics and Particle InteractionsParticle physics theoretical and experimental studiesHigh-Energy Particle Collisions Research