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Stars as Laboratories for Fundamental Physics - MPP Theory Group

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256 Chapter 7<br />

ever effect causes the “wrong” de<strong>for</strong>mation of the end-point spectrum.<br />

In spite of apparent systematic problems, the Troitsk group (Belesev<br />

et al. 1994) claims a limit of m νe < 4.5 eV at 95% CL; see also Otten<br />

(1995).<br />

One h<strong>as</strong> attempted to determine m νµ by me<strong>as</strong>uring the muon momentum<br />

from the decay of stopped pions, π + → µ + ν µ , leading to m 2 ν µ<br />

=<br />

m 2 π<br />

+ m 2 + µ − 2m π +(m 2 µ + p 2 µ) 1/2 . A recent p µ me<strong>as</strong>urement (Daum et al.<br />

1991) implied a negative squared m<strong>as</strong>s of m 2 ν µ<br />

= −(0.154±0.045) MeV 2 ,<br />

probably due to large systematic uncertainties in the determination of<br />

m π +. Hence, it seemed that the often-quoted bound of m νµ < 0.27 MeV<br />

did not apply. An older experiment studied the in-flight decay of pions<br />

with a result m 2 ν µ<br />

= −(0.14 ± 0.20) MeV 2 , largely independent of<br />

the pion m<strong>as</strong>s (Anderhub et al. 1982). This implies a 90% CL upper<br />

limit of m νµ < 0.50 MeV. Most recently, the m<strong>as</strong>s of the negative<br />

pion w<strong>as</strong> reconsidered by Jeckelmann, Goudsmit, and Leisi (1994).<br />

Their previous experiment allows <strong>for</strong> two m<strong>as</strong>s <strong>as</strong>signments, m π =<br />

139.56782±0.00037 MeV or 139.56995±0.00035 MeV. The larger value<br />

had previously been rejected on the b<strong>as</strong>is of evidence which now appears<br />

questionable. Together with a new p µ me<strong>as</strong>urement (Assamagan et al.<br />

1994) one finds m 2 ν µ<br />

= −0.148 ± 0.024 MeV 2 or −0.022 ± 0.023 MeV 2 .<br />

The first value is negative by 6.2 standard deviations and thus may<br />

be rejected <strong>as</strong> unphysical. The second solution is compatible with zero<br />

and gives a 90% CL upper limit of m νµ < 0.16 MeV.<br />

For ν τ the best bounds also come from limits on missing energy<br />

in certain reactions, the only <strong>for</strong>m in which ν τ h<strong>as</strong> ever been “observed.”<br />

The ARGUS Collaboration (1988, 1992) studied the decay<br />

τ − → 3π − 2π + ν τ with a total of 20 events with good energy determinations<br />

<strong>for</strong> all five pions, leading to m ντ < 31 MeV at 95% CL.<br />

A similar experiment by the CLEO Collaboration (1993) b<strong>as</strong>ed on a<br />

much larger data sample gave m ντ < 32.6 MeV at 95% CL. Most recently,<br />

the ALEPH Collaboration (1995) at CERN h<strong>as</strong> reported a new<br />

Table 7.2. Experimental neutrino m<strong>as</strong>s limits.<br />

Flavor Limit CL Reference<br />

ν e (5 eV) — See Tab. 7.1<br />

ν µ 0.16 MeV 90% Assamagan et al. (1994)<br />

ν τ 23.8 MeV 95% ALEPH Collaboration (1995)

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