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SOME where and 1041 MAGNETIC FIRST-ORDER TRANSITIONS To*=To coscp(1-P*K{3), 'YJ*='YJ coscp/(1-P*K{3), (4) O·~--~--~---r-'ITt~1 P*=P-aIT/K. AFM Evaluating the free energy for j=! and various 'YJ's, Tequil as a function of 'YJ is determined (recalling that Tequil is the temperature at which the magnetic and nonmagnetic states have the same free energy). In Fig. 4 the results of these evaluations are given as a plot of Tequil'YJ/TO vs 1/'YJ. As no restrictions have been put upon 'YJ and since To'YJ= To*'YJ*, we may proceed with Eq.

Rev. Letters 6, 452 (1961). 21 J. O. , R. W. Boom, G. D. Kneip, R. E. Worsham, and C. E. Roos, Phys. Rev. Letters 6, 532 (1961). 22 H. R. , I. S. Jacobs, C. L. Kolbe, and P. E. Lawrence, Bull. Am. Phys. Soc. 6 (1961) (post-deadline paper); 1961 International Conference on High Magnetic Fields, Massachusetts Institute of Technology, November 1-4, 1961. 23 R. W. Boom (private communication). 24 P. R. Aron and H. C. Hitchcock (to be published). 25 J. K. Hulm, Phys. Rev. 98, 1539 (1955). 26 B. T. Matthias, T.

Tanenbaum for stimulating discussions and several valuable comments. 43 L. J. Donadieu, 1961 Conference on Fundamental Research in Superconductivity, IBM, Yorktown Heights, New York, June 15-17,1961. 44 B. T. Matthias, E. A. Wood, E. Corenzwit, and V. B. Bala, J. Phys. Chern. Solids 1, 188 (1956). 45 G. F. Hardy and J. K. Hulm, Phys. Rev. 93, 1004 (1954). JOURNAL OF APPLIED PHYSICS SUPPLEMENT TO VOL. 33. 3 MARCH, 1962 Magnetic Devices W. L. , Chairman Threshold Properties of Partially Switched Ferrite Cores V.

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