Download Anomalous Rare Earths and Actinides. Valence Fluctuation and by J.X. Boucherle, J. Flouquet and C. Lacroix (Eds.) PDF

By J.X. Boucherle, J. Flouquet and C. Lacroix (Eds.)

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Fulde for a critical reading of the manuscript and D. Wohlleben for stimulating discussions. L. Lin, J. E. Crow, T. Mihalisin, J. I. R. Stewart, Phys. Rev. Lett. 54 (1985) 2541. [2] C. Vettier, P. Morin and J. Flouquet, Phys. Rev. Lett. 56 (1986) 1980. [3] P. Lethuillier and J. Chaussy, J. de Phys. 37 (1976) 123. [4] D. Duerkop, E. Braun, B. Politt, H. Schmidt and D. Wohlleben, Z. Physik B63 (1986) 55. J. Birgeneau, J. Phys. Chem. Solids 33 (1972) 59. [6] D. Niki, W. Assmus, I. Konrondir, M. Yoshizawa and B.

CePb3: Magnetization, magnetoresistance, Hall effect Fig. 4. Variation of the Hall resistance (rH = Hall voltage divided by the current) vs. H at different temperatures. Inset shows the variation of the Hall coefficient RH vs. T around T N at ambient and 10 kbar pressure. agreement with the general experience, that T K increases with pressure. 3 K. 5 x 10 1 0 Pa [7]. This value of flm is rather large compared with for instance the value for CeAl 2 at P = 0 which is about - 5 . Assuming a linear pressure dependence, CePb 3 will enter a nonmagnetic state at about 22 kbar.

Squires, Thermal Neutron Scattering, (Cambridge University Press, Cambridge, 1978). [12] Y. Kuramoto and H. Kojima, J. Magn. Magn. Mat. 47&48 (1985) 329. [13] P. Schlottmann, in: Valence Instabilities, eds. P. W├Ąchter and H. Boppart (North-Holland, Amsterdam, 1982) p. 471. [14] H. Rietschel, Phys. Rev. B33 (1986) 2027. X. Boucherie and J. Schweizer, Physica 130B (1985) 337. X. Boucherie, J. Flouquet, Y. Lassailly, J. Palleau and J. Schweizer, J. Magn. Magn. Mat. 31 (1983) 409. M. S. D. Parks, Rep.

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