By L. Marton
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Additional resources for Advances Electronics and Electron Physics. Vol. XI
58. L. Marton and L. B. Leder, Phys. Rev. * S9. S. W. Wonssowski, A. W. Sokolow, and A. S. Wexler, Progr. Phys. ) 4, 115 (1956). 40. M. J. Buckingham, Phys. Rev. B. Makinson and M. J. Buckingham, Proc. Phys. A64, 135 (1951); H. B. Huntington, Phys. Rev. 89,357 (1953). 41. G. E. Pikus, J . Exptl. Theoret. Phys. ) 27, 369 (1954); J. M. Dykman, J . Tech. Phys. ) 26, 1026 (1955). 48. P. Gorlich, H. Hora, and W. Macke, Jenaer Jahrb. p. 91 (1957); Exptl. Tech. d. Physik 6, 217 (1957); P. Gorlich and H.
33 38 42 43 49 52 57 67 76 83 83 I. INTRODUCTION In 1956, Lee and Yang (1) showed in a very important paper that the concept of parity conservation, which had been tacitly assumed for over thirty years, had not been either proved or refuted for the weak interactions by the then existing experiments. Here the term weak interactions refers to the decay of the strange particles ( K particles and hyperons), the T- and p-meson decays, as well as the pdecay of nuclei.
The anthracene crystal is connected by a long (4 ft) Lucite pipe to a photomultiplier which is placed at the top of the cryostat. Upon demagnetization of the sample, a vertical solenoid is raised around the lower part of the cryostat. The counting is then started. The results obtained are shown in Fig. 3. The upper part of this figure shows the y-ray anisotropy, as given by the difference between the counting rates in the polar and the equatorial y-counters. The time for complete warm-up is -6 min.