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Clear evidence of a spin glass transition was found in dilute metallic alloys [e.g., Cu-Mn, R. Omari, J. Prejean, and J. Souletie, J. Phys. (Paris) 44, 1069 (1983)]
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0041974253
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as well as in concentrated insulators where the frustration may be due either to a competition between ferromagnetic and antiferromagnetic interactions [e.g., (Formula presented) N. Bontemps, J. Rajchenbach, R. V. Chamberlin, and R. Orbach, J. Magn. Magn. Mater. 1, 54 (1986).
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0031550483
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or a topological frustration in presence of antiferromagnetic interactions only [e.g., (Formula presented) M. J. Gingras, C. V. Stager, N. P. Raju, B. D. Gaulin, and J. E. Gredan, Phys. Rev. Lett. 78, 947 (1997)].
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0031206673
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This effect is well known in ferrite nanoparticles and oxides. See, for instance, R. H. Kodama, Salah A. Makhlouf, and A. E. Berkowitz, Phys. Rev. Lett. 79, 1393 (1997).
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R. H. Kodama, A. E. Berkowitz, E. J. McNiff, Jr., and S. Foner, J. Appl. Phys. 81, 5552 (1997).
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30244560850
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See also Conference Digest of the 15th International Colloquium on Magnetic Films and Surfaces, Institute for Chemical Research, Kyoto University, 1997
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B. Dieny, V. S. Speriosu, S. S. P. Parkin, B. A. Gurney, D. R. Wilhoit, and D. Mauri, Phys. Rev. B 43, 1297 (1991); See also Conference Digest of the 15th International Colloquium on Magnetic Films and Surfaces, Institute for Chemical Research, Kyoto University, 1997.
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0000058858
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It is interesting to note that in Ref. 14 the surface spin disorder of ferrites is explained by the sensitivity of superexchange to broken bonds. In our case the sample is metallic, but the high deformation of the boundary, also with broken bonds and a distribution of interatomic distances, should explain the coexistence of competitive interactions. A similar case has recently been analyzed in the boundary of nanocrystalline pure Fe. See, for instance, L. Del Bianco, A. Hernando, E. Bonetti, and E. Navarro, Phys. Rev. B 56, 8894 (1997).
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Del Bianco, L.1
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