1970
DOI: 10.1088/0022-3719/3/1/012
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On the spontaneous magnetization of the classical Heisenberg ferromagnet

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1973
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Cited by 29 publications
(10 citation statements)
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“…At smaller values of t, the theory readily reaches the asymptotic spherical regime. Moreover, while in the Ising-model SCOZA the coexistence curve displays a non-classical exponent β = 7/20 [1,14], the Heisenberg coexistence curve predicted by the SCOZA instead is associated with β = 1/2, and is overall considerably narrower than the expected one as given by MC simulations [4] and Padè approximant techniques [8]. (We find however that it displays the correct behavior in the low-temperature limit).…”
Section: Introductionmentioning
confidence: 64%
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“…At smaller values of t, the theory readily reaches the asymptotic spherical regime. Moreover, while in the Ising-model SCOZA the coexistence curve displays a non-classical exponent β = 7/20 [1,14], the Heisenberg coexistence curve predicted by the SCOZA instead is associated with β = 1/2, and is overall considerably narrower than the expected one as given by MC simulations [4] and Padè approximant techniques [8]. (We find however that it displays the correct behavior in the low-temperature limit).…”
Section: Introductionmentioning
confidence: 64%
“…In particular, the theory has already been formulated also for the D-vector model [3], i.e., a system of classical D-dimensional spins with nearest-neighbor interaction. In the present paper the D-vector model SCOZA is further investigated and the simplest version of the SCOZA that we have developed is solved numerically in the case of three-dimensional spins (classical Heisenberg model) on a threedimensional lattice, and the results are compared with Monte Carlo simulations [4,5,6] and Padè approximants based on high-temperature expansions [7,8,9,10,11]. An analysis of what is lacking in this simple application to the D-vector model then guides us in formulating a more sophisticated version of the theory that takes into account the influence of transverse correlations on the longitudinal susceptibility and as a result, yields a more complete and accurate description of the spin-wave properties of the model.…”
Section: Introductionmentioning
confidence: 99%
“…[1][2][3][4][5][6][7] This class of materials contains some of the very few ferromagnetic (FM) insulators with a simple rock salt lattice structure. In particular, EuO has an accessible Curie temperature 7 (T c ) of 69 K that is seen to be sensitive to lattice strain.…”
mentioning
confidence: 99%
“…16 Metal-toinsulator transition and colossal magneto-resistance have been reported in EuO systems with electron doping. 14,[17][18][19][20] Much effort has been put into investigating the influence of the substrate on the magnetic properties of EuO [2][3][4][5][6]11,12,21,22 including changes to the Curie temperature (T c ) and critical exponents. Ferroelectric (FE) substrates are unique due to the potential for electric modulation, coming from the ferroelectric polarization reversal, which can be considered as a form of extrinsic electrostatic doping at the FM-FE interfaces.…”
mentioning
confidence: 99%
“…where the kinetic weighting factors ji are given by (7) ji=n;/nex = exp( -E;/kT) /(Qvib-l): (8) ni is the equilibrium number of excited molecules in state i, nex is the total number of equilibrium excited molec:;ules, Ei is the energy of state i, and Qvib is the vibrational partition function. A derivation of Eq.…”
Section: Resultsmentioning
confidence: 99%