2004
DOI: 10.1016/j.physb.2004.08.026
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Magnetic properties of amorphous Gd0.67Y0.33

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Cited by 7 publications
(2 citation statements)
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“…The curvature in such isotherms becomes more pronounced as the temperature at which a given isotherm is taken deviates more and more from T C . However, in our case the isotherms just below and above T C exhibit the same curvature, as previously observed for semi-disordered systems [27], indicating that nature of the phase transition is slightly different form a classical ferromagnet. Because we do not measure exactly the isotherm for T = T C we obtain the value of δ by interpolating the slopes of the approximately straight parts of the near-critical isotherms for large Ln(H ) [28].…”
Section: Modified Arrott Plot and Critical Isothermsupporting
confidence: 88%
“…The curvature in such isotherms becomes more pronounced as the temperature at which a given isotherm is taken deviates more and more from T C . However, in our case the isotherms just below and above T C exhibit the same curvature, as previously observed for semi-disordered systems [27], indicating that nature of the phase transition is slightly different form a classical ferromagnet. Because we do not measure exactly the isotherm for T = T C we obtain the value of δ by interpolating the slopes of the approximately straight parts of the near-critical isotherms for large Ln(H ) [28].…”
Section: Modified Arrott Plot and Critical Isothermsupporting
confidence: 88%
“…CdCr 2 Se 4 is a ferromagnetic semiconductor with a Curie temperatures T C ≈ 130K [2]. In CdCr 2 Se 4 the magnetic order results from the competition of nearest neighbors positive Cr-Se-Cr interaction and more distant negative Cr-Se-Cd-Se-Cr exchange interaction [3]. Substitution of the manganese and tin for the divalent cadmium ion therefore causes fundamental changes of magnetic properties.…”
Section: Introductionmentioning
confidence: 99%