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The goal of the experiment is a 1% measurement of \( \Lambda _{s} \) ( \( \approx 1.5\: 10^{-3} \) \( \lambda _{0} \)). The capture rate will be measured as \( \Lambda _{s}= \) \( \lambda _{\mu -}-\lambda _{\mu +} \), thus \( \delta \Lambda _{s}\sim \) \( \sqrt{2}\delta \lambda _{\mu } \). As a result the lifetime of the positive and negative muon have to be measured with at least 10 ppm precision, if both have to be determined. At present, even the positive muon lifetime is only known to 20 ppm, though recent experiments propose to reduce this error to 1 ppm [17,18]. Then, in principle, only a 14 ppm measurement of the negative muon lifetime in hydrogen is required for the present experiment. Nevertheless, as regards systematics, it is much preferable to measure both \( \mu ^{+} \)and \( \mu ^{-} \)simultaneously in a single experiment.



Peter Kammel 2001-02-04