INTERMAG Asia 2005. Digests of the IEEE International Magnetics Conference, 2005. 2005
DOI: 10.1109/intmag.2005.1464485
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Magnetic anisotropy and magnetization variation with temperature

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“…The value of R in the dense system is about eight times larger than that in the noninteracting case, implying that the magnitude of the FC magnetization memory effect does depend on the interparticle dipolar interaction. This is in quite good agreement with the experimental results of Telem-Shafir et al 16 In the noninteracting case, no memory effect is seen during a ZFC process ͑see Fig. 8͒ below ͑T b ͒, since the occupation probabilities of up and down particles are both equal to 0.5 ͑two-state model͒.…”
Section: Superparamagnetism Versus Spin-glasssupporting
confidence: 91%
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“…The value of R in the dense system is about eight times larger than that in the noninteracting case, implying that the magnitude of the FC magnetization memory effect does depend on the interparticle dipolar interaction. This is in quite good agreement with the experimental results of Telem-Shafir et al 16 In the noninteracting case, no memory effect is seen during a ZFC process ͑see Fig. 8͒ below ͑T b ͒, since the occupation probabilities of up and down particles are both equal to 0.5 ͑two-state model͒.…”
Section: Superparamagnetism Versus Spin-glasssupporting
confidence: 91%
“…Time-dependent magnetization measurements suggest that dense nanoparticle samples may exhibit glassy dynamics due to dipolar interparticle interaction; 16,[26][27][28] disorder and frustration are induced by the randomness in the particle positions and anisotropy axis distributions. As discussed within a simple mean field theory picture, adapted to the two-state model of Chakraverty et al, 9 the random dipolar interaction can be accounted for in terms of a local, self-consistent field that has the form…”
Section: Spin-glass-like Slow Dynamicsmentioning
confidence: 99%
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