1995
DOI: 10.1016/s1567-2719(05)80008-3
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Chapter 4 Field induced phase transitions in ferrimagnets

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Cited by 39 publications
(36 citation statements)
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“…For TbIG, T comp is equal to (243.5 ± 0.5 K) and (249.0 ± 0.5 K) for the single crystal and powder samples respectively (Lahoubi et al, 1985;Lahoubi, 1986). In the vicinity of T comp, the magnetic behavior is equivalent to that observed in the antiferromagnet compounds with the existence of the so-called field induced phase transitions which have been studied previously theoretically and experimentally (Zvezdin, 1995). In the Néel model, the RE 3+ magnetic behavior is described by the pure free ion Brillouin function assuming that the superexchange interactions are represented by the isotropic Weiss molecular field coefficients.…”
Section: Introductionmentioning
confidence: 84%
“…For TbIG, T comp is equal to (243.5 ± 0.5 K) and (249.0 ± 0.5 K) for the single crystal and powder samples respectively (Lahoubi et al, 1985;Lahoubi, 1986). In the vicinity of T comp, the magnetic behavior is equivalent to that observed in the antiferromagnet compounds with the existence of the so-called field induced phase transitions which have been studied previously theoretically and experimentally (Zvezdin, 1995). In the Néel model, the RE 3+ magnetic behavior is described by the pure free ion Brillouin function assuming that the superexchange interactions are represented by the isotropic Weiss molecular field coefficients.…”
Section: Introductionmentioning
confidence: 84%
“…Field induced phase transitions are valuable means for studying various aspects of solid state physics such as the exchange interactions in a broad range of bulk and mesoscopic materials [3].…”
Section: The First Order Fipt In the Rco Itinerant Metamagnetsmentioning
confidence: 99%
“…The antiferromagnetic indirect interaction between the magnetic ions embedded within the molecules results in ferrimagnetic ground state of the molecules. However, there is a significant difference between the magnetization process of bulk and mesoscopic ferrimagnetic materials that can be seen from the slide 18: the former has a monotonous increase of magnetization with the external magnetic field and a plateau on its magnetic susceptibility curve while the latter has specific quantum steps on magnetization and oscillations of susceptibility with the field [3].…”
Section: The Full Magnetization Process In Ferrimagnets Difference Bmentioning
confidence: 99%
“…The many interesting magnetic properties at low temperature which is often taken in account including strong magnetocrystalline anisotropy, spontaneous non-collinear magnetic structures (double umbrella-type), SR and FI magnetic phase transitions and their complicated experimental MPD in the vicinity of the compensation temperature, have been thoroughly reviewed by Guillot [2] and Zvezdin [3]. The occurrence of the so-called <uuw> and <uv0> angular LT phases where the iron sublattices magnetisation M Fe l i e s on a low symmetry direction are studied experimentally [4,5,6] and theoretically [7,8] by using different phenomenological models based on the generalized spin effective Hamiltonian broadly applicable to such magnetic transitions.…”
Section: Introductionmentioning
confidence: 99%