Numéro |
J. Phys. Colloques
Volume 49, Numéro C8, Décembre 1988
Proceedings of the International Conference on Magnetism
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Page(s) | C8-363 - C8-364 | |
DOI | https://doi.org/10.1051/jphyscol:19888163 |
J. Phys. Colloques 49 (1988) C8-363-C8-364
DOI: 10.1051/jphyscol:19888163
MAGNETIC ORDER IN VERY DILUTED Y-Er ALLOYS
R. Caudron1, 2, H. Bouchiat3, P. J. Brown4, P. Monod3 et J. L. Tholence51 ONERA, B.P. 72, 92322 Chatillon Cedex, France
2 Laboratoire Léon Brillouin, C.E.N. Saclay, 91191 Gif sur Yvette Cedex, France
3 Laboratoire de Physique des Solides, Bât. 510, 91405, Orsay, France
4 Institut Laue-Langevin 39042 Grenoble, France
5 Centre de recherches sur les très basses températures, CNRS, B.P. 166X, 38042 Grenoble Cedex, France
Abstract
Neutron scattering and non-linear susceptibility measurements were performed on Y single crystals doped with 3, 2, 1 and 0.5 at. % Er. All the samples exhibit long range order satellites. Though Er in Y is Ising-like, no harmonics were detected. Down to T / TN ~ 0.02, the intensities are consistent with a model where the mean magnetization of each hexagonal layer is sinusoïdally modulated in the c direction. Just above TN, the divergence of the non linear susceptibility along the c axis behave as in a spin glass and the critical exponents γSG = 1 and δSG=2 were found. Because of the dilution, they are related to an antiferromagnetic long range order, with βAF = 0.5 (consistent with the behaviour of the staggered magnetization), and γAF = 1.9.