A Search for Charged Excitation of Dark Matter with the KamLAND-Zen Detector

S. Abe,S. Asami, A. Gando, Y. Gando, T. Gima, Atsushi Goto,Takahiko Hachiya, Keiko Hata, S. Hayashida, K. Hosokawa, Kunihiro Ichimura, S. Ieki, H. Ikeda,K. Inoue,K. Ishidoshiro, Y. Kamei, N. Kawada, T. Kinoshita, M. Koga,N. Maemura, T. Mitsui, H. Miyake, Kenzo Nakamura, R. Nakamura, Akira Ono,Naomi Ota, S. Otsuka, Hironori Ozaki, T. Sakai, H. Sambonsugi, I. Shimizu, Y. Shirahata, J. Shirai,Kiyoshi Shiraishi, A. Suzuki, Y. Suzuki, A. Takeuchi, K. Tamae, K. Ueshima,Yoshiki Wada, H. Watanabe,Yuki Yoshida,Shigeru Obara,D. Chernyak,Alexandre Kozlov,S. Yoshida,S. Umehara, Y. Takemoto,K. Fushimi, S. Hirata, A. K. Ichikawa,Kiseki Nakamura,Masato Yoshida,B. E. Berger,B. K. Fujikawa,C. Grant,A. Li, J. G. Learned,J. Maricic,Spencer Axani,L. A. Winslow, Z. Fu,Y. V. Efremenko,H. J. Karwowski,D. M. Markoff, W. Tornow, Tommy O'Donnell, S. Dell’Oro,J. A. Detwiler,S. Enomoto,M. P. Decowski

arXiv (Cornell University)(2021)

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摘要
Author(s): Abe, S; Asami, S; Gando, A; Gando, Y; Gima, T; Goto, A; Hachiya, T; Hata, K; Hayashida, S; Hosokawa, K; Ichimura, K; Ieki, S; Ikeda, H; Inoue, K; Ishidoshiro, K; Kamei, Y; Kawada, N; Kinoshita, T; Koga, M; Maemura, N; Mitsui, T; Miyake, H; Nakamura, K; Nakamura, K; Nakamura, R; Ono, A; Ota, N; Otsuka, S; Ozaki, H; Sakai, T; Sambonsugi, H; Shimizu, I; Shirahata, Y; Shirai, J; Shiraishi, K; Suzuki, A; Suzuki, Y; Takeuchi, A; Tamae, K; Ueshima, K; Wada, Y; Watanabe, H; Yoshida, Y; Obara, S; Chernyak, D; Kozlov, A; Yoshida, S; Umehara, S; Takemoto, Y; Fushimi, K; Hirata, S; Ichikawa, A; Nakamura, KZ; Yoshida, M; Berger, BE; Fujikawa, BK; Grant, C; Li, A; Learned, JG; Maricic, J; Axani, S; Winslow, LA; Fu, Z; Efremenko, Y; Karwowski, HJ; Markoff, DM; Tornow, W; ODonnell, T; DellOro, S; Detwiler, JA; Enomoto, S; Decowski, MP | Abstract: There are many theories where a dark matter particle is part of a multiplet with an electrically charged state. If WIMP dark matter ($\chi^{0}$) is accompanied by a charged excited state ($\chi^{-}$) separated by a small mass difference, it can form a stable bound state with a nucleus. In supersymmetric models, the $\chi^{0}$ and the $\chi^{-}$ could be the neutralino and a charged slepton, such as the neutralino-stau degenerate model. The formation binding process is expected to result in an energy deposition of {\it O}(1--10 MeV), making it suitable for detection in large liquid scintillator detectors. We describe new constraints on the bound state formation with a xenon nucleus using the KamLAND-Zen 400 Phase-II dataset. In order to enlarge the searchable parameter space, all xenon isotopes in the detector were used. For a benchmark parameter set of $m_{\chi^{0}} = 100$ GeV and $\Delta m = 10$ MeV, this study sets the most stringent upper limits on the recombination cross section $\langle\sigma v\rangle$ and the decay-width of $\chi^{-}$ of $2.0 \times 10^{-31}$ ${\rm cm^3/s}$ and $1.1 \times 10^{-18}$ GeV, respectively (90\% confidence level).
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dark matter,charged excitation,kamland-zen
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