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Search for Majorana Neutrinos Near the Inverted Mass Hierarchy Region with KamLAND-Zen.
Gando, A; Gando, Y; Hachiya, T; Hayashi, A; Hayashida, S; Ikeda, H; Inoue, K; Ishidoshiro, K; Karino, Y; Koga, M; Matsuda, S; Mitsui, T; Nakamura, K; Obara, S; Oura, T; Ozaki, H; Shimizu, I; Shirahata, Y; Shirai, J; Suzuki, A; Takai, T; Tamae, K; Teraoka, Y; Ueshima, K; Watanabe, H; Kozlov, A; Takemoto, Y; Yoshida, S; Fushimi, K; Banks, T I; Berger, B E; Fujikawa, B K; O'Donnell, T; Winslow, L A; Efremenko, Y; Karwowski, H J; Markoff, D M; Tornow, W; Detwiler, J A; Enomoto, S; Decowski, M P.
Afiliação
  • Gando A; Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan.
  • Gando Y; Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan.
  • Hachiya T; Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan.
  • Hayashi A; Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan.
  • Hayashida S; Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan.
  • Ikeda H; Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan.
  • Inoue K; Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan.
  • Ishidoshiro K; Kavli Institute for the Physics and Mathematics of the Universe (WPI), The University of Tokyo Institutes for Advanced Study, The University of Tokyo, Kashiwa, Chiba 277-8583, Japan.
  • Karino Y; Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan.
  • Koga M; Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan.
  • Matsuda S; Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan.
  • Mitsui T; Kavli Institute for the Physics and Mathematics of the Universe (WPI), The University of Tokyo Institutes for Advanced Study, The University of Tokyo, Kashiwa, Chiba 277-8583, Japan.
  • Nakamura K; Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan.
  • Obara S; Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan.
  • Oura T; Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan.
  • Ozaki H; Kavli Institute for the Physics and Mathematics of the Universe (WPI), The University of Tokyo Institutes for Advanced Study, The University of Tokyo, Kashiwa, Chiba 277-8583, Japan.
  • Shimizu I; Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan.
  • Shirahata Y; Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan.
  • Shirai J; Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan.
  • Suzuki A; Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan.
  • Takai T; Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan.
  • Tamae K; Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan.
  • Teraoka Y; Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan.
  • Ueshima K; Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan.
  • Watanabe H; Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan.
  • Kozlov A; Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan.
  • Takemoto Y; Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan.
  • Yoshida S; Research Center for Neutrino Science, Tohoku University, Sendai 980-8578, Japan.
  • Fushimi K; Kavli Institute for the Physics and Mathematics of the Universe (WPI), The University of Tokyo Institutes for Advanced Study, The University of Tokyo, Kashiwa, Chiba 277-8583, Japan.
  • Banks TI; Kavli Institute for the Physics and Mathematics of the Universe (WPI), The University of Tokyo Institutes for Advanced Study, The University of Tokyo, Kashiwa, Chiba 277-8583, Japan.
  • Berger BE; Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan.
  • Fujikawa BK; Faculty of Integrated Arts and Science, University of Tokushima, Tokushima 770-8502, Japan.
  • O'Donnell T; Physics Department, University of California, Berkeley, and Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA.
  • Winslow LA; Kavli Institute for the Physics and Mathematics of the Universe (WPI), The University of Tokyo Institutes for Advanced Study, The University of Tokyo, Kashiwa, Chiba 277-8583, Japan.
  • Efremenko Y; Physics Department, University of California, Berkeley, and Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA.
  • Karwowski HJ; Kavli Institute for the Physics and Mathematics of the Universe (WPI), The University of Tokyo Institutes for Advanced Study, The University of Tokyo, Kashiwa, Chiba 277-8583, Japan.
  • Markoff DM; Physics Department, University of California, Berkeley, and Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA.
  • Tornow W; Physics Department, University of California, Berkeley, and Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA.
  • Detwiler JA; Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA.
  • Enomoto S; Kavli Institute for the Physics and Mathematics of the Universe (WPI), The University of Tokyo Institutes for Advanced Study, The University of Tokyo, Kashiwa, Chiba 277-8583, Japan.
  • Decowski MP; Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, USA.
Phys Rev Lett ; 117(8): 082503, 2016 Aug 19.
Article em En | MEDLINE | ID: mdl-27588852
ABSTRACT
We present an improved search for neutrinoless double-beta (0νßß) decay of ^{136}Xe in the KamLAND-Zen experiment. Owing to purification of the xenon-loaded liquid scintillator, we achieved a significant reduction of the ^{110m}Ag contaminant identified in previous searches. Combining the results from the first and second phase, we obtain a lower limit for the 0νßß decay half-life of T_{1/2}^{0ν}>1.07×10^{26} yr at 90% C.L., an almost sixfold improvement over previous limits. Using commonly adopted nuclear matrix element calculations, the corresponding upper limits on the effective Majorana neutrino mass are in the range 61-165 meV. For the most optimistic nuclear matrix elements, this limit reaches the bottom of the quasidegenerate neutrino mass region.

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2016 Tipo de documento: Article

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2016 Tipo de documento: Article