1987
DOI: 10.1088/0022-3719/20/12/011
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Antiferromagnetic Ising spin glass

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Cited by 34 publications
(36 citation statements)
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“…In this section we present the results of several numerical studies and show that they are in good agreement. First, we numerically solved for the critical point of the RSB-1 free energy 13 We have glossed over one important point, which is that although the expressions for the free energies Eq. 3.5 and Eq.…”
Section: Numerical Resultsmentioning
confidence: 99%
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“…In this section we present the results of several numerical studies and show that they are in good agreement. First, we numerically solved for the critical point of the RSB-1 free energy 13 We have glossed over one important point, which is that although the expressions for the free energies Eq. 3.5 and Eq.…”
Section: Numerical Resultsmentioning
confidence: 99%
“…2.42). 13 We numerically tested the replica prediction Eq. 3.7 by simulating many instances of random bipartite graphs and using a simple variant of the well-known Kernighan-Lin (KL) [41] algorithm.…”
Section: )mentioning
confidence: 99%
“…Most studies have concentrated on situations where the exchange distributions are either symmetric or with an additional ferromagnetic interaction. More recently a twosublattice version of the SK model was introduced [10][11][12][13] to allow for antiferromagnetic interactions between different sublattices. Such extension is quite natural in view of the existence of many experimental systems such as Fe x Mg 1−x Cl 2 [14][15][16] and Fe x Mn 1−x TiO 3 [17,18], which exhibit a transition from an Ising antiferromagnetic into an Ising spin glass state for a certain range of x values.…”
Section: Introductionmentioning
confidence: 99%
“…Such extension is quite natural in view of the existence of many experimental systems such as Fe x Mg 1−x Cl 2 [14][15][16] and Fe x Mn 1−x TiO 3 [17,18], which exhibit a transition from an Ising antiferromagnetic into an Ising spin glass state for a certain range of x values. In contrast to the standard SK model, in the two-sublattice SK model with antiferromagnetic intersublattice interactions, the ordered (antiferromagnetic) phase extends to finite fields and the de Almeida-Thouless instability line [5] has distinct branches in the paramagnetic and antiferromagnetic phases, which do not meet at a first-order transition [10][11][12][13]. Experimental determination of the field-temperature phase diagram in Fe x Mn 1−x TiO 3 , as well as the de AlmeidaThouless instability line [19], are in qualitative agreement with mean-field results [13].…”
Section: Introductionmentioning
confidence: 99%
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