1973
DOI: 10.1103/physrevb.7.370
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Scaling with Respect to a Parameter for the Gibbs Potential and Pair Correlation Function of theS=12Ising Model with Lattice Anisotropy

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Cited by 37 publications
(3 citation statements)
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“…For 2D magnetic materials with weak interlayer coupling such as CrBr 3 , the critical temperature is primarily determined by the intralayer interaction and weakly depends on the interlayer interaction. Further correction to the critical temperature is in agreement with our density functional theory (DFT) calculations that the FM phase with higher interlayer coupling would possess a slightly higher critical temperature . Second, apart from the pure AFM samples, the S2-class samples show obvious residual magnetic moment near zero fields (indicating the presence of an FM component) and then undergo another spin-flip ( H 2 ) transition to a forced FM state under high fields (Figure c).…”
Section: Resultssupporting
confidence: 84%
See 1 more Smart Citation
“…For 2D magnetic materials with weak interlayer coupling such as CrBr 3 , the critical temperature is primarily determined by the intralayer interaction and weakly depends on the interlayer interaction. Further correction to the critical temperature is in agreement with our density functional theory (DFT) calculations that the FM phase with higher interlayer coupling would possess a slightly higher critical temperature . Second, apart from the pure AFM samples, the S2-class samples show obvious residual magnetic moment near zero fields (indicating the presence of an FM component) and then undergo another spin-flip ( H 2 ) transition to a forced FM state under high fields (Figure c).…”
Section: Resultssupporting
confidence: 84%
“…Further correction to the critical temperature is in agreement with our density functional theory (DFT) calculations that the FM phase with higher interlayer coupling would possess a slightly higher critical temperature. 35 Second, apart from the pure AFM samples, the S2-class samples show obvious residual magnetic moment near zero fields (indicating the presence of an FM component) and then undergo another spin-flip (H 2 ) transition to a forced FM state under high fields (Figure 2c). The magnetic configuration of the S2 sample is different from that of the uncompensated odd-layer A-type AFM sample but exhibits the coexistence of FM and AFM components because 4) the H 2 seems to disappear at a lower temperature than the H c with increasing temperature (Figure 2e), consistent with the fact that T N is slightly lower than T c for pure AFM and FM samples.…”
Section: Antiferromagntic and Mixed-phase Crbrmentioning
confidence: 99%
“…The theoretical studies of the dimensional crossover have been carried out by using perturbation theory [2]- [5], high temperature series expansion [6]- [13], generalized homogeneous functions [14], and rigorous approach [15]- [17]. The results are that the critical and the crossover temperature are singular with respect to λ.…”
Section: Introductionmentioning
confidence: 99%