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By FAY AJZENBERG-SELOVE (Eds.)

ISBN-10: 1483230635

ISBN-13: 9781483230634

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The property of a particle-localization detector of this type lends itself quite readily for use along the focal line of a magnetic spectrometer. The display of the ratio pulse in a multichannel analyzer can be used to pick out a particular group of particles separated in energy from other groups by the magnetic analyzer and corresponding to the particular state to be studied. This would be an intermediate modification of Buechner's (35) wide-range spectrometer which might be particularly 42 Ν.

Wu, Theory of multiple scattering: second Born approximation and correc­ tions to Moliere's work (in print). 10. E . J. Williams, Proc. Roy. Soc. (London) A169, 531 (1939); Phys. Rev. 68, 292 (1940). 11. Η. H. Seliger, Phys. Rev. 78, 491 (1950). 12. H. A. Bethe and W. Heitler, Proc. Roy. Soc. (London) A146, 83 (1934). IS. P. A. Cerenkov, Compt. rend. Acad. Sei. R. 8, 451 (1934); 14, 105 (1937); Phys. Rev. 52, 378 (1937). / 4 . I. Frank and I. Tamm, Compt. rend. Acad. Sei. R. 14, 109 (1937). 15.

S. WALL rather than an ion chamber tends to decrease E/AE because of the additional statistical fluctuations in the multiplication process. In the case of ion chambers, it is necessary to have a high transparency grid at a potential intermediate to that of the collector and the cathode to ensure that the size of the induced current pulse is independent of the location of the ionizing event. This enables one to use just electron rather than FIG. 7. A gaseous ionization chamber constructed by D. A.

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Nuclear Spectroscopy by FAY AJZENBERG-SELOVE (Eds.)


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