Search for a Light Higgs Boson in Single-Photon Decays of Upsilon(1S) Using (SIC)(2S) -> pi(+) pi(-) Upsilon(1S) Tagging Method

Belle Collaboration, S. Jia,C. P. Shen,I. Adachi, H. Aihara,S. Al Said,D. M. Asner, H. Atmacan,T. Aushev, R. Ayad, V. Babu,P. Behera, K. Belous,J. Bennett, M. Bessner,V. Bhardwaj,B. Bhuyan, T. Bilka,A. Bobrov,D. Bodrov, G. Bonvicini, J. Borah, M. Bračko, P. Branchini,T. E. Browder, A. Budano,M. Campajola, D. Červenkov,M. -C. Chang,P. Chang, V. Chekelian,A. Chen,B. G. Cheon,K. Chilikin,H. E. Cho,K. Cho,S. -J. Cho,S. -K. Choi,Y. Choi,S. Choudhury,D. Cinabro,S. Cunliffe,S. Das,N. Dash,G. De Nardo,G. De Pietro,R. Dhamija,F. Di Capua,Z. Doležal, T. V. Dong,D. Epifanov, T. Ferber, D. Ferlewicz,B. G. Fulsom,R. Garg,V. Gaur, N. Gabyshev,A. Giri, P. Goldenzweig, B. Golob, E. Graziani, Y. Guan, K. Gudkova, C. Hadjivasiliou, T. Hara, K. Hayasaka,H. Hayashii,M. T. Hedges,W. -S. Hou, K. Inami, G. Inguglia,A. Ishikawa, R. Itoh,M. Iwasaki, Y. Iwasaki,W. W. Jacobs,E. -J. Jang, Y. Jin, K. K. Joo,J. Kahn,A. B. Kaliyar,K. H. Kang, T. Kawasaki, C. Kiesling,C. H. Kim,D. Y. Kim,K. -H. Kim,Y. -K. Kim,K. Kinoshita, P. Kodyš,S. Kohani,T. Konno, A. Korobov, S. Korpar, E. Kovalenko, P. Križan,R. Kroeger,P. Krokovny,M. Kumar,R. Kumar,K. Kumara,Y. -J. Kwon,T. Lam, M. Laurenza,S. C. Lee, J. Li,L. K. Li,Y. Li,Y. B. Li,L. Li Gioi, J. Libby, K. Lieret, D. Liventsev,A. Martini,M. Masuda,T. Matsuda, D. Matvienko,S. K. Maurya, F. Meier,M. Merola, F. Metzner, K. Miyabayashi, R. Mizuk,G. B. Mohanty, M. Nakao, D. Narwal, Z. Natkaniec,A. Natochii,L. Nayak,N. K. Nisar, S. Nishida,K. Nishimura,K. Ogawa,S. Ogawa,H. Ono, P. Oskin,P. Pakhlov, G. Pakhlova,T. Pang, S. Pardi,S. -H. Park,S. Patra,S. Paul,T. K. Pedlar, R. Pestotnik,L. E. Piilonen, T. Podobnik, E. Prencipe,M. T. Prim,M. Röhrken, A. Rostomyan,N. Rout,G. Russo,D. Sahoo, S. Sandilya,A. Sangal, L. Santelj, T. Sanuki, V. Savinov, G. Schnell, J. Schueler, C. Schwanda, Y. Seino, K. Senyo,M. E. Sevior, M. Shapkin,C. Sharma, V. Shebalin,J. -G. Shiu, B. Shwartz,J. B. Singh,A. Sokolov, E. Solovieva, S. Stanič, M. Starič,Z. S. Stottler, M. Sumihama, K. Sumisawa, T. Sumiyoshi, W. Sutcliffe,M. Takizawa,U. Tamponi, K. Tanida, F. Tenchini, K. Trabelsi,M. Uchida, S. Uehara,T. Uglov, Y. Unno,K. Uno,S. Uno, P. Urquijo, S. E. Vahsen,R. Van Tonder, G. Varner, A. Vinokurova,E. Waheed,D. Wang,E. Wang, M. -Z. Wang,S. Watanuki, E. Won,B. D. Yabsley,W. Yan, S. B. Yang,H. Ye, J. Yelton, J. H. Yin, Y. Yusa, Y. Zhai, Z. P. Zhang,V. Zhilich,V. Zhukova

PHYSICAL REVIEW LETTERS(2022)

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摘要
We search for a light Higgs boson (A(0)) decaying into a tau(+)tau(-) or mu(+)mu(-) pair in the radiative decays of Upsilon(1S). The production of Upsilon(1S) mesons is tagged by Upsilon(2S) -> pi(+)pi(-)Upsilon(1S) transitions, using 158 x 10(6) Upsilon(2S) events accumulated with the Belle detector at the KEKB asymmetric energy electron-positron collider. No significant A(0) signals in the mass range from the tau(+)tau(-) or mu(+)mu(-) threshold to 9.2 GeV/c(2) are observed. We set the upper limits at 90% credibility level (C.L.) on the product branching fractions for Upsilon(1S) -> gamma A(0) and A(0) -> tau(+)tau(-) varying from 3.8 x 10(-6) to 1.5 x 10(-4). Our results represent an approximately twofold improvement on the current world best upper limits for the Upsilon(1S) -> gamma A(0) (tau(+)tau(-)) production. For A(0) -> mu(+) mu(-), the upper limits on the product branching fractions for Upsilon(1S) -> gamma A(0) and A(0) -> mu(+)mu(-) are at the same level as the world average limits, and vary from 3.1 x 10(-7) to 1.6 x 10(-5). The upper limits at 90% credibility level on the Yukawa coupling f((SIC)(1S)) and mixing angle sin theta(A0) are also given.
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