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By L. Marton

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Extra resources for Advances Electronics and Electron Physics. Vol. XI

Example text

Atomic Energy Commission. 31 32 R. M. 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.

4, where the negative sign indicates that more @-particlesare emitted in the direction opposite to the nuclear spin than along the spin direction. From the values of a and (J,)/J, one finds for the parameter 0 [Eq. 7. According to the theory of Lee, Oehme, and Yang (10) this large value of the asymmetry indicates not only parity (P ) nonconservation, but also violation of the invariance under charge conjugation (C) in the 0-decay. There exists a third related operation, called time reversal (7').

The formation of this atom could be an important source of depolarization, both because of its internal hyperfine splitting and on account of the precession of its total magnetic moment (= electron magnetic moment) around the (smal1)external magnetic field. I n a second paper, Friedman and Telegdi (14)have presented their results for the asymmetry for a somewhat larger sample consisting of 2,000 complete r+-p+-e+ decays. The ratio E [Eq. 038) cos e (13) Thus, the asymmetry in this more accurate determination is somewhat higher than the value reported in their first paper.

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

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