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

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 Added by Keishi Hosokawa
 Publication date 2021
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and research's language is English




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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 $langlesigma vrangle$ 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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A search for double-beta decays of 136Xe to excited states of 136Ba has been performed with the first phase data set of the KamLAND-Zen experiment. The 0+1, 2+1 and 2+2 transitions of 0{ u}{beta}{beta} decay were evaluated in an exposure of 89.5kg-yr of 136Xe, while the same transitions of 2{ u}{beta}{beta} decay were evaluated in an exposure of 61.8kg-yr. No excess over background was found for all decay modes. The lower half-life limits of the 2+1 state transitions of 0{ u}{beta}{beta} and 2{ u}{beta}{beta} decay were improved to T(0{ u}, 0+ rightarrow 2+) > 2.6times10^25 yr and T(2{ u}, 0+ rightarrow 2+) > 4.6times10^23 yr (90% C.L.), respectively. We report on the first experimental lower half-life limits for the transitions to the 0+1 state of 136Xe for 0{ u}{beta}{beta} and 2{ u}{beta}{beta} decay. They are T (0{ u}, 0+ rightarrow 0+) > 2.4times10^25 yr and T(2{ u}, 0+ rightarrow 0+) > 8.3times10^23 yr (90% C.L.). The transitions to the 2+2 states are also evaluated for the first time to be T(0{ u}, 0+ rightarrow 2+) > 2.6times10^25 yr and T(2{ u}, 0+ rightarrow 2+) > 9.0times10^23 yr (90% C.L.). These results are compared to recent theoretical predictions.
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