2008
DOI: 10.1103/physrevb.77.014105
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Realization of the mean-field universality class in spin-crossover materials

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Cited by 123 publications
(130 citation statements)
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“…However, it was shown that in an elastic model applied with periodic boundary conditions the domain growth is hindered. 24 Therefore, the use of open boundary conditions is a necessary requirement for obtaining macroscopic clusters. Recent works showed that in the elastic model with open boundary conditions the nucleation always starts from corners (very rarely from non-corner edge sites), either in rectangular or triangular lattices.…”
Section: Introductionmentioning
confidence: 99%
“…However, it was shown that in an elastic model applied with periodic boundary conditions the domain growth is hindered. 24 Therefore, the use of open boundary conditions is a necessary requirement for obtaining macroscopic clusters. Recent works showed that in the elastic model with open boundary conditions the nucleation always starts from corners (very rarely from non-corner edge sites), either in rectangular or triangular lattices.…”
Section: Introductionmentioning
confidence: 99%
“…At variance from these electronic models, the continuous medium model developed by Spiering [7] showed that an elastic interaction could as well give rise to the observed first-order transitions. More recently, discrete models based on deformable lattices [8][9][10][11][12][13][14][15][16] were introduced so as to mimic the spatio-temporal features revealed by optical microscopy investigations [17][18][19] for the nucleation and growth of the spin state phases at the thermal transition of SCO single crystals. They conciliate the continuous medium and discrete lattice approaches, with purely elastic interactions, so as to reproduce both lattice and spin transformations of the system.…”
Section: The Modelmentioning
confidence: 99%
“…When Δ and P are the values of the same order as occurs for Δ at the point of intersection Δ c , spin transitions from one state to another can be controlled by external influences such as temperature, pressure and light irradiation. Thus, the spin transition results from an interaction-induced interplay between the valence electrons on the ligands and d-electrons in the lower energy shells located near the Fe 2+ (3d 6 ) core [3]. These states are determinate numerical: S = 0 for diamagnetic LS state and S = 2 for paramagnetic HS state.…”
Section: Introductionmentioning
confidence: 99%
“…For the first time, the Ising-like model for treating nearest-neighbour interactions in spincrossover compounds was proposed Bouseksou et al [5]. This model was successful in simulating a transition of the steady state of the Fe(II) metal compounds [6][7][8][9][10][11]. Also, for these materials many efforts have been devoted to understand theoretically spin transition in phenomenological models [12][13][14].…”
Section: Introductionmentioning
confidence: 99%
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