1999
DOI: 10.1016/s0370-2693(99)01188-0
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Neutrino-induced upward stopping muons in Super-Kamiokande

Abstract: A total of 137 upward stopping muons of minimum energy 1.6 GeV are observed by Super-Kamiokande during 516 detector live days. The measured muon flux is 0.39+/-0.04(stat.)+/-0.02(syst.)x10^{-13}cm^{-2}s^{-1}sr^{-1} compared to an expected flux of 0.73+/-0.16(theo.)x10^{-13}cm^{-2}s^{-1}sr^{-1}. Using our previously-published measurement of the upward through-going muon flux, we calculate the stopping/through-going flux ratio R}, which has less theoretical uncertainty. The measured value of R=0.22+/-0.02(stat.)… Show more

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Cited by 168 publications
(68 citation statements)
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“…[6,7] A consistent pattern of energy and pathlength dependence emerges that clearly points to neutrino oscillations as the explanation. Because atmospheric ν e behave normally to the precision measured so far, the main effect must lie in the ν µ ↔ ν τ sector (or involve sterile neutrinos, which are now disfavored).…”
Section: Department Of Energy Under Grant No De-fg02-91er40626mentioning
confidence: 67%
“…[6,7] A consistent pattern of energy and pathlength dependence emerges that clearly points to neutrino oscillations as the explanation. Because atmospheric ν e behave normally to the precision measured so far, the main effect must lie in the ν µ ↔ ν τ sector (or involve sterile neutrinos, which are now disfavored).…”
Section: Department Of Energy Under Grant No De-fg02-91er40626mentioning
confidence: 67%
“…Rapidly growing interest in neutrino physics has recently been stimulated by new data from facilities at Kamiokande [1], Super-Kamiokande [2], LSND [3], CHOOZ [4], and some others [5,6]. These data are indicative, directly or indirectly, of the Pontecorvo (vacuum) oscillations [7] of neutrinos of three types, ν e , ν µ , and ν τ .…”
mentioning
confidence: 99%
“…These data are indicative, directly or indirectly, of the Pontecorvo (vacuum) oscillations [7] of neutrinos of three types, ν e , ν µ , and ν τ . The frequency of these oscillations, i.e., of the ν i ν k transitions in oscillations, is proportional to sin 2 , where p ν is the ultrarelativistic neutrino momentum and t = L / c is the time it takes for a neutrino to run from source to detector (the distance L is called the "base length"). In what follows, we set c = 1 for convenience.…”
mentioning
confidence: 99%
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