2017
DOI: 10.1007/s10948-017-4018-4
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Critical Properties of Two-dimensional Anisotropic Ising Model on a Square Lattice

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Cited by 7 publications
(5 citation statements)
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“…We approximated the magnetic behavior of Hf 2 MnC 2 O 2 by a classical spin-half Ising model on a triangular lattice, with strain-induced anisotropy. The Hamiltonian is where σ i = ±1 are Ising spins, ⟨ ij ⟩ x indicates that the sum is over nearest neighbors in the horizontal x direction, ⟨ ij ⟩ diag indicates nearest neighbors in other directions, J 1 and J 2 are couplings along the horizontal and diagonal directions, respectively, as shown in Figure , and E 0 represents the nonmagnetic part of the energy. According to eq , the energies of the spin configurations in Figure a,b,e are Solving for the couplings yields which allows us to infer J 1 and J 2 from the results of DFT energy calculations.…”
Section: Resultsmentioning
confidence: 99%
“…We approximated the magnetic behavior of Hf 2 MnC 2 O 2 by a classical spin-half Ising model on a triangular lattice, with strain-induced anisotropy. The Hamiltonian is where σ i = ±1 are Ising spins, ⟨ ij ⟩ x indicates that the sum is over nearest neighbors in the horizontal x direction, ⟨ ij ⟩ diag indicates nearest neighbors in other directions, J 1 and J 2 are couplings along the horizontal and diagonal directions, respectively, as shown in Figure , and E 0 represents the nonmagnetic part of the energy. According to eq , the energies of the spin configurations in Figure a,b,e are Solving for the couplings yields which allows us to infer J 1 and J 2 from the results of DFT energy calculations.…”
Section: Resultsmentioning
confidence: 99%
“…7 % σ 8 7 & … is always positive. When summed for all possible configurations a factor of 2 ( will be formed, therefore the partition function from equation ( 8) can be written using the expression from equation (9),…”
Section: Graphical Correspondence For the High-temperature Limitmentioning
confidence: 99%
“…Hence, a specific value of 𝛼 corresponds to a single critical temperature 𝑘 % 𝑇 & /𝐽. [9], in which they simulate a square lattice of size 𝑁 = 𝑆 × 𝑆 for 𝑆 = {8,16,32,64} and rely on finite-size scaling analysis using a Binder cumulant. This is done by comparing the Binder parameter for each finite size of 𝑁 to obtain a critical temperature close to the exact solution where the size of 𝑁 is infinite (see Table 1).…”
Section: Anisotropy Between 𝑱 and 𝑱′mentioning
confidence: 99%
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“…Количество таких исследований велико, отметим только некоторые из них. Модель Изинга в дальнейшем изучалась с анизотропией (модель Изинга, в которой спины имеют большие значения) [26][27][28][29], с биквадратичным взаимодействием [30], в случайных полях [31,32], в магнитных полях [33][34][35], в поперечном поле [36], с трехспиновым взаимодействием [37], с четырехспиновым взаимодействием [38], в антиферромагнитных системах [39][40][41][42][43][44], с фрустрацией [45][46][47][48][49][50][51][52][53][54][55][56], со смешанным значением спина [57][58][59][60], с конкуренцией обменных взаимодействий [61][62][63][64][65][66][67][68][69], на декорированных решетках [59,60,70,…”
Section: модель изингаunclassified