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Gamma‐Ray Scintillation Spectrometer with Logarithmic Pulse‐Height Response
1.D. Maeder and V. Wintersteiger, Physica 18, 1147 (1952);
1.J. G. Campbell and A. J. F. Boyle, Austral. J. Phys. 6, 171 (1953);
1.Maeder, Mueller, and Wintersteiger, Helv. Phys. Acta 27, 3 (1954).
2.C. J. Borkowski and R. L. Clark, Rev. Sci. Instr. 24, 1046 (1953);
2.P. R. Bell, Nucleonics 12, No. 3, 54 (1954);
2.R. S. Foote and H. W. Koch, Rev. Sci. Instr. 25, 746 (1954);
2.G. Hine (Mass. Inst. Technology), private communication;
2.W. E. Kreger and L. McIsaac, Phys. Rev. 93, 943 (1954), and private communication.
3.C. G. Kelley, Nucleonics 10, No. 4, 34 (1952).
4.Equivalent pulse shaping has been obtained previously by the use of two short‐circuited delay lines with a conventional amplifier inserted between them. Separate limiter circuits are required in that case—see Francis, Bell, and Kelley, Nucleonics 12, No. 3, 55 (1954).
5.D. Maeder, Helv. Phys. Acta 20, 139 (1947);
5.Bernstein, Chase, and Schardt, Rev. Sci. Instr. 24, 437 (1953).
6.D. Maeder and H. Medicus, Helv. Phys. Acta 23 (Suppl. III), 175 (1950).
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