Abstract
The conserved-vector-current theory of the strangeness-conserving weak decays predicts that , the vector coupling constant in nuclear beta decay, should be equal to , the coupling constant in the muon decay. To make possible a more precise comparison of and , the value of has been remeasured. The endpoint energy of the positron decay has been determined by measuring the values of the reactions and (2.311-MeV state), using the same techniques and equipment where possible in order to minimize the uncertainty in the difference of the values. The results of these measurements are keV and keV, which yield keV, all energies relative to the threshold assumed as 1880.7±0.4 keV. The half-life of has also been remeasured as 71.00±0.13 sec, which implies a partial half-life of 71.43±0.15 sec for the transition to the 2.311-MeV state of . Averaged with the recent half-life measurement of Hendrie and Gerhart, we obtain an value of 3075±10 sec for the decay, after correcting for nuclear form factors, electron screening, and -capture competition. With the radiative corrections of Kinoshita and Sirlin, the value obtained for is (1.4025±0.0022)× erg-, where the quoted error is experimental in origin. This is to be compared with the value computed from recent muon decay measurements, erg-, which is (2.0±0.2)% larger. As there appear to be several possible theoretical explanations for this small discrepancy, the present results are consistent with the conserved-vector-current hypothesis.
- Received 13 March 1962
DOI:https://doi.org/10.1103/PhysRev.127.583
©1962 American Physical Society