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Search for GUT Monopoles at Super-Kamiokande | Super-Kamiokande Collaboration
; K. Ueno
; K. Abe
; Y. Hayato
; T. Iida
; K. Iyogi
; J. Kameda
; Y. Koshio
; Y. Kozuma
; M. Miura
; S. Moriyama
; M. Nakahata
; S. Nakayama
; Y. Obayashi
; H. Sekiya
; M. Shiozawa
; Y.Suzuki
; A. Takeda
; Y. Takenaga
; K. Ueshima
; S. Yamada
; T. Yokozawa
; K. Martens
; J. Schuemann
; M. Vagins
; C. Ishihara
; H. Kaji
; T. Kajita
; K. Kaneyuki
; T. McLachlan
; K. Okumura
; Y. Shimizu
; N. Tanimoto
; E. Kearns
; M. Litos
; J. L. Raaf
; J. L. Stone
; L. R. Sulak
; K. Bays
; W. R. Kropp
; S. Mine
; C. Regis
; A.Renshaw
; M. B. Smy
; H. W. Sobel
; K. S. Ganezer
; J. Hill
; W. E. Keig
; J. S. Jang
; J. Y. Kim
; I. T. Lim
; J. B. Albert
; K. Scholberg
; C. W. Walter
; R. Wendell
; T. Wongjirad
; T. Ishizuka
; S. Tasaka
; J. G. Learned
; S. Matsuno
; T. Hasegawa
; T. Ishida
; T. Ishii
; T. Kobayashi
; T. Nakadaira
; K. Nakamura
; K. Nishikawa
; Y. Oyama
; K. Sakashita
; T. Sekiguchi
; T. Tsukamoto
; A. T. Suzuki
; Y. Takeuchi
; M. Ikeda
; A. Minamino
; T. Nakaya
; L. Labarga
; Ll. Marti
; Y. Fukuda
; Y. Itow
; G. Mitsuka
; T. Tanaka
; C. K. Jung
; G. Lopez
; I. Taylor
; C. Yanagisawa
; H. Ishino
; A. Kibayashi
; S. Mino
; T. Mori
; M. Sakuda
; H. Toyota
; Y. Kuno
; M. Yoshida
; S. B. Kim
; B. S. Yang
; H. Okazawa
; Y. Choi
; K. Nishijima
; M. Koshiba
; Y. Totsuka
; M. Yokoyama
; S. Chen
; Y. Heng
; Z. Yang
; H. Zhang
; D. Kielczewska
; P. Mijakowski
; K. Connolly
; M. Dziomba
; E. Thrane
; R. J. Wilkes
; | Date: |
5 Mar 2012 | Abstract: | GUT monopoles captured by the Sun’s gravitation are expected to catalyze
proton decays via the Callan-Rubakov process. In this scenario, protons, which
initially decay into pions, will ultimately produce
u_{e},
u_{mu} and
ar{
u}_{mu}. After undergoing neutrino oscillation, all neutrino species
appear when they arrive at the Earth, and can be detected by a 50,000 metric
ton water Cherenkov detector, Super-Kamiokande (SK). A search for low energy
neutrinos in the electron total energy range from 19 to 55 MeV was carried out
with SK and gives a monopole flux limit of F_M(sigma_0/1 mb) < 6.3 imes
10^{-24} (eta_M/10^{-3})^2 cm^{-2} s^{-1} sr^{-1} at 90% C.L., where eta_M
is the monopole velocity in units of the speed of light and sigma_0 is the
catalysis cross section at eta_M=1. The obtained limit is more than eight
orders of magnitude more stringent than the current best cosmic-ray
supermassive monopole flux limit, F_M < 1 imes 10^{-15} cm^{-2} s^{-1}
sr^{-1} for eta_M < 10^{-3} and also two orders of magnitude lower than the
result of the Kamiokande experiment, which used a similar detection method. | Source: | arXiv, 1203.0940 | Services: | Forum | Review | PDF | Favorites |
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