1977
DOI: 10.1002/pssb.2220800137
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Reaction field and dipolar interaction in quasi‐onedimensional heisenberg systems. Application to CsNiF3

Abstract: An improved mean field theory, the reaction field approximation, which was previously used for a Heisenberg paramagnet, is extended to include the magnetic dipolar interaction. It is shown that in spin chains, when the intra-chain interaction is ferromagnetic, the dipolar inter-chain interaction plays an important role in explaining the phase transition to an antiferromagnetic three-dimensional order a t low temperature. A study of the magnetic susceptibility of CsNiF3 is presented as an explicit example. Valu… Show more

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Cited by 15 publications
(8 citation statements)
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“…RFA was originally proposed by Onsager [67] and was extended to the Ising system by Brout et al [68] and to an arbitrary spin system S in the entire phase space (both below and above T c ) by Scherer et al [69][70][71][72][73].…”
Section: Reaction Field Approximation (Rfa)mentioning
confidence: 99%
“…RFA was originally proposed by Onsager [67] and was extended to the Ising system by Brout et al [68] and to an arbitrary spin system S in the entire phase space (both below and above T c ) by Scherer et al [69][70][71][72][73].…”
Section: Reaction Field Approximation (Rfa)mentioning
confidence: 99%
“…This requires either analytical approximations, such as field theories, or numerical simulations, such as Monte Carlo simulations. Spinteract uses a self-consistent extension of mean-field theory called Onsager reaction-field theory [48][49][50][51][52][53]. This approach takes account of thermal fluctuations in an approximate way, but has been shown to give results in excellent agreement with Monte Carlo simulations [24,54].…”
Section: B Magnetic Neutron Scattering Intensitymentioning
confidence: 99%
“…1) which is different from the 120 • structure of CsMnBr 3 , an XY system having strong AF coupling along the chains. This difference is due to the relatively strong dipolar field originating from the neighboring ferromagnetic chains 11 . This dipolar field depends strongly on the angle between the magnetic sub-lattices and it can be shown quite easily that there is no interchain dipolar field present on a given site at H c , where the magnetization of all the sub-lattices are parallel to the field.…”
Section: Mean-field Coupling Of Quasi-1d Chainsmentioning
confidence: 99%
“…It is important to note that dipolar field is almost nonexistant if the ordering along the chains is antiferromagnetic (AF), as it is in many other ABX 3 compouds such as CsMnBr 3 and CsNiCl 3 . 10 This strong dipolar field is responsible for the particular planar AF arrangement 11 of CsNiF 3 which is different from the expected 120 • structure of a system with only AF interactions on a triangular lattice. This magnetic phase occurs for temperatures smaller than T N ≃ 2.77 K. 12 .…”
Section: Introductionmentioning
confidence: 95%