1988
DOI: 10.1103/physrevd.38.2102
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Cited by 66 publications
(36 citation statements)
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“…As a result, stringent constraints can be placed on the models from the experimental limits on µ → eγ, τ → µγ, [145] µ-e conversion in nuclei [515,516], muoniumantimuonium oscillation [517,518], etc. For instance, the MEGA limit on µ → eγ leads to the constraint [511] ε e ε µ ≈ 0 .…”
Section: Nutev Physicsmentioning
confidence: 99%
“…As a result, stringent constraints can be placed on the models from the experimental limits on µ → eγ, τ → µγ, [145] µ-e conversion in nuclei [515,516], muoniumantimuonium oscillation [517,518], etc. For instance, the MEGA limit on µ → eγ leads to the constraint [511] ε e ε µ ≈ 0 .…”
Section: Nutev Physicsmentioning
confidence: 99%
“…Historic overview of constraints on µ [194] SREL (1972) < 1.6 × 10 [196] TRIUMF (1985) < 1.6 × 10 [197] TRIUMF (1988) < 4.6 × 10 [199] PSI (1998) < 6.1 × 10 [197] TRIUMF (1988) < 4.9 × 10 [200] PSI (1996) < 4.6 × 10…”
Section: µ − E Conversionmentioning
confidence: 99%
“…In the aspect of experimental study, the current upper limits for muon-electron conversion in the nuclear field are given by the experiments at TRIUMF and PSI. The upper limit for gold is 7 × 10 −13 from the results of SINDRUM-II experiment at PSI [7], and upper limits for titanium are 4.3 × 10 −12 and 4.6 × 10 −12 from the results of SINDRUM-II [8] and an experiment at TRIUMF [9], respectively. The experimental results are getting closer to the level of thoeretical predictions and it is possible to reach the predicted level by improving the experimental sensitivity by only a few orders of magnitude.…”
Section: Introductionmentioning
confidence: 93%