S. Enomoto
University of Washington
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Featured researches published by S. Enomoto.
Physical Review C | 2012
A. Gando; Y. Gando; H. Hanakago; H. Ikeda; Katsuya Inoue; R. Kato; M. Koga; S. Matsuda; T. Mitsui; T. Nakada; Ko Nakamura; A. Obata; A. Oki; Y. Ono; I. Shimizu; J. Shirai; A. Suzuki; Y. Takemoto; K. Tamae; K. Ueshima; H. Watanabe; B. D. Xu; S. Yamada; H. Yoshida; A. Kozlov; S. Yoshida; T. I. Banks; J. A. Detwiler; Stuart J. Freedman; B. K. Fujikawa
We present limits on Majoron-emitting neutrinoless double-β decay modes based on an exposure of 112.3 days with 125 kg of 136Xe. In particular, a lower limit on the ordinary (spectral index n=1) Majoron-emitting decay half-life of 136Xe is obtained as T1/20νχ0>2.6×1024 yr at 90% C.L., a factor of five more stringent than previous limits. The corresponding upper limit on the effective Majoron-neutrino coupling, using a range of available nuclear matrix calculations, is 〈gee〉<(0.8-1.6)×10−5. This excludes a previously unconstrained region of parameter space and strongly limits the possible contribution of ordinary Majoron emission modes to 0νββ decay for neutrino masses in the inverted hierarchy scheme.
The Astrophysical Journal | 2012
A. Gando; Y. Gando; K. Ichimura; H. Ikeda; K. Inoue; Y. Kibe; Y. Kishimoto; M. Koga; Y. Minekawa; T. Mitsui; T. Morikawa; N. Nagai; Kazuo Nakajima; K. Nakamura; K. Narita; I. Shimizu; Y. Shimizu; J. Shirai; F. Suekane; A. Suzuki; H. Takahashi; N. Takahashi; Y. Takemoto; K. Tamae; H. Watanabe; B. D. Xu; H. Yabumoto; H. Yoshida; Shijun Yoshida; S. Enomoto
We present the results of a search for extraterrestrial electron antineutrinos (ν_e’s)in the energy range 8.3MeV < E_(νe) < 31.8MeV using the KamLAND detector. In an exposure of 4.53 kton-year, we identify 25 candidate events. All of the candidate events can be attributed to background, most importantly neutral current atmospheric neutrino interactions, setting an upper limit on the probability of ^8B solar ν_es converting into ν_e’s at 5.3 × 10^(–5) (90% CL), if we assume an undistorted v_e shape. This limit corresponds to a solar v_e flux of 93 cm^(–2) s^(–1) or an event rate of 1.6 events (kton–year)^(–1) above the energy threshold (E_(ve) ≥ 8.3MeV). The present data also allows us to set more stringent limits on the diffuse supernova neutrino flux and on the annihilation rates for light dark matter particles.
Nuclear Physics | 2016
K. Asakura; A. Gando; Y. Gando; T. Hachiya; S. Hayashida; H. Ikeda; Katsuya Inoue; K. Ishidoshiro; T. Ishikawa; S. Ishio; M. Koga; S. Matsuda; T. Mitsui; D. Motoki; K. Nakamura; S. Obara; M. Otani; T. Oura; I. Shimizu; Y. Shirahata; J. Shirai; Akira Suzuki; H. Tachibana; K. Tamae; K. Ueshima; H. Watanabe; B. D. Xu; Hiroshi Yoshida; A. Kozlov; Y. Takemoto
Abstract 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 ν β β decay were evaluated in an exposure of 89.5 kg ⋅ yr of 136Xe, while the same transitions of 2 ν β β decay were evaluated in an exposure of 61.8 kg ⋅ yr . No excess over background was found for all decay modes. The lower half-life limits of the 2 1 + state transitions of 0 ν β β and 2 ν β β decay were improved to T 1 / 2 0 ν ( 0 + → 2 1 + ) > 2.6 × 10 25 yr and T 1 / 2 2 ν ( 0 + → 2 1 + ) > 4.6 × 10 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 ν β β and 2 ν β β decay. They are T 1 / 2 0 ν ( 0 + → 0 1 + ) > 2.4 × 10 25 yr and T 1 / 2 2 ν ( 0 + → 0 1 + ) > 8.3 × 10 23 yr (90% C.L.). The transitions to the 2 2 + states are also evaluated for the first time to be T 1 / 2 0 ν ( 0 + → 2 2 + ) > 2.6 × 10 25 yr and T 1 / 2 2 ν ( 0 + → 2 2 + ) > 9.0 × 10 23 yr (90% C.L.). These results are compared to recent theoretical predictions.
The Astrophysical Journal | 2016
K. Asakura; A. Gando; Y. Gando; T. Hachiya; S. Hayashida; H. Ikeda; Katsuya Inoue; K. Ishidoshiro; T. Ishikawa; S. Ishio; M. Koga; S. Matsuda; T. Mitsui; D. Motoki; K. Nakamura; S. Obara; T. Oura; I. Shimizu; Y. Shirahata; J. Shirai; Akira Suzuki; H. Tachibana; K. Tamae; K. Ueshima; H. Watanabe; B. D. Xu; A. Kozlov; Y. Takemoto; S. Yoshida; K. Fushimi
In the late stages of nuclear burning for massive stars (
The Astrophysical Journal | 2016
A. Gando; Y. Gando; T. Hachiya; A Hayashi; S. Hayashida; H. Ikeda; Katsuya Inoue; K. Ishidoshiro; Y Karino; M. Koga; S. Matsuda; T. Mitsui; K. Nakamura; S. Obara; T. Oura; H Ozaki; I. Shimizu; Y. Shirahata; J. Shirai; Akira Suzuki; T Takai; K. Tamae; Y Teraoka; K. Ueshima; H. Watanabe; A. Kozlov; Y Takemoto; S. Yoshida; K. Fushimi; A. Piepke
M>8~M_{sun}
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2015
T. I. Banks; S. J. Freedman; J. Wallig; N. Ybarrolaza; A. Gando; Y. Gando; H. Ikeda; Katsuya Inoue; Y. Kishimoto; M. Koga; T. Mitsui; K. Nakamura; I. Shimizu; J. Shirai; Akira Suzuki; Y. Takemoto; K. Tamae; K. Ueshima; H. Watanabe; B. D. Xu; H. Yoshida; S. Yoshida; A. Kozlov; C. Grant; G. Keefer; A. Piepke; T. Bloxham; B. K. Fujikawa; K. Han; K. Ichimura
), the production of neutrino-antineutrino pairs through various processes becomes the dominant stellar cooling mechanism. As the star evolves, the energy of these neutrinos increases and in the days preceding the supernova a significant fraction of emitted electron anti-neutrinos exceeds the energy threshold for inverse beta decay on free hydrogen. This is the golden channel for liquid scintillator detectors because the coincidence signature allows for significant reductions in background signals. We find that the kiloton-scale liquid scintillator detector KamLAND can detect these pre-supernova neutrinos from a star with a mass of
The Astrophysical Journal | 2015
A. Asakura; A. Gando; Y. Gando; T. Hachiya; S. Hayashida; H. Ikeda; Katsuya Inoue; K. Ishidoshiro; T. Ishikawa; S. Ishio; M. Koga; S. Matsuda; T. Mitsui; D. Motoki; K. Nakamura; S. Obara; Y. Oki; T. Oura; I. Shimizu; Y. Shirahata; J. Shirai; Akira Suzuki; H. Tachibana; K. Tamae; K. Ueshima; H. Watanabe; B. D. Xu; H. Yoshida; A. Kozlov; Y. Takemoto
25~M_{sun}
Physical Review D | 2015
K. Asakura; A. Gando; Y. Gando; T. Hachiya; S. Hayashida; H. Ikeda; Koji Inoue; K. Ishidoshiro; T. Ishikawa; S. Ishio; M. Koga; R. Matsuda; S. Matsuda; T. Mitsui; D. Motoki; K. Nakamura; S. Obara; Y. Oki; T. Oura; I. Shimizu; Y. Shirahata; J. Shirai; Akira Suzuki; H. Tachibana; K. Tamae; K. Ueshima; H. Watanabe; B. D. Xu; Y. Yamauchi; H. Yoshida
at a distance less than 690~pc with 3
The Astrophysical Journal | 2017
A. Gando; Y. Gando; T. Hachiya; A Hayashi; S. Hayashida; H. Ikeda; Katsuya Inoue; K. Ishidoshiro; Y Karino; M. Koga; S. Matsuda; T. Mitsui; K. Nakamura; S. Obara; T. Oura; H Ozaki; I. Shimizu; Y. Shirahata; J. Shirai; Akira Suzuki; T Takai; K. Tamae; Y Teraoka; K. Ueshima; H. Watanabe; A. Kozlov; Y. Takemoto; S. Yoshida; K. Fushimi; A. Piepke
sigma
Physical Review Letters | 2013
A. Gando; Y. Gando; H. Hanakago; H. Ikeda; Koji Inoue; K. Ishidoshiro; R. Kato; M. Koga; S. Matsuda; T. Mitsui; D. Motoki; T. Nakada; K. Nakamura; A. Obata; A. Oki; Y. Ono; M. Otani; I. Shimizu; J. Shirai; Akira Suzuki; Y. Takemoto; K. Tamae; K. Ueshima; H. Watanabe; B. D. Xu; S. Yamada; H. Yoshida; A. Kozlov; S. Yoshida; T. I. Banks
significance before the supernova. This limit is dependent on the neutrino mass ordering and background levels. KamLAND takes data continuously and can provide a supernova alert to the community.