Download PDF by L. Marton: Advances Electronics and Electron Physics. Vol. XI

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5 (9) arises from the relation which holds for J 4 J transitions with emission of positrons; P+ is the analog of the coefficient p for electron emitters. It can be shown generally that P+ = -P, where is given by Eq. (7). 5 can be immediately obtained by comparing (10) with (6). I n agreement with the prediction of Eq. (lo), the measured value of a for Co68had roughly one-third the magnitude of a(Co60)and was positive. 4 for electrons from Co60 with the same velocity. The asymmetry CY was measured as a function of velocity in this experiment.

M. STERNHEIMER by the two-component neutrino theory (with V A interaction): /3 = +v,/c [see Eq. (17)]. Their results are thus also in agreement with the observations of Ambler et al. 2) on the decay. OF FRIEDMAN AND TELEGDI IV. THEEXPERIMENT POSITRON ASYMMETRY IN THE a+-p+-e+ DECAY ON THE At about the same time as the experiment of Wu et al. (9)(in late 1956), Friedman and Telegdi (4) carried out an experiment on the asymmetry of the angular distribution of positrons from p+ decays in nuclear emulsion, which was also suggested in the paper of Lee and Yang (1).

STERRHEIMER the weak interactions. The first of these experiments was carried out by Wu et al. ( 2 ) on the /%decay asymmetry from oriented Co60 nuclei. By showing that the counting rate of the electrons is different along the directions parallel and antiparallel to the nuclear spin, it was clearly demonstrated for the first time that parity is not conserved for the (weak)p-decay interaction. The degree of violation of parity conservation in the weak interactions is actually equal to its maximum possible value.

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Advances Electronics and Electron Physics. Vol. XI by L. Marton

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