2014
DOI: 10.1016/j.physe.2014.06.028
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The effects of next nearest-neighbor exchange interaction on the magnetic properties in the one-dimensional Ising system

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Cited by 31 publications
(7 citation statements)
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“…However, when h is larger than h c , the coefficient of friction becomes negative [53]. The theoretical results obtained by Zhong and Zhang using a multiple-scattering method showed that the energy spectra for multilayer photonic structures analogous to multilayer graphene structures with AAA, ABA, and ABC stacking are highly dependent on the distances between the layers, the stacking number in the layers, and the type of stacking, which are closely analogous to the electronic effects in multilayer graphene structures [54] and the next nearest-neighbor effects on the magnetic properties of a one-dimensional Ising system [55]. Similarly, we found that the magnetic properties (magnetization and hysteresis) of the ferromagnetic spin-1/2 TLINS were highly dependent on the distance (d) between the layers.…”
Section: Theoretical Results and Discussionmentioning
confidence: 91%
“…However, when h is larger than h c , the coefficient of friction becomes negative [53]. The theoretical results obtained by Zhong and Zhang using a multiple-scattering method showed that the energy spectra for multilayer photonic structures analogous to multilayer graphene structures with AAA, ABA, and ABC stacking are highly dependent on the distances between the layers, the stacking number in the layers, and the type of stacking, which are closely analogous to the electronic effects in multilayer graphene structures [54] and the next nearest-neighbor effects on the magnetic properties of a one-dimensional Ising system [55]. Similarly, we found that the magnetic properties (magnetization and hysteresis) of the ferromagnetic spin-1/2 TLINS were highly dependent on the distance (d) between the layers.…”
Section: Theoretical Results and Discussionmentioning
confidence: 91%
“…We search for the magnetic features of the ferromagnetic (J1>0) S1-1DIS shown in Figure 1 [41] in which each site is occupied by the spin-1 Ising particle. By using Kaneyoshi approach [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17][18][19][20], the Hamiltonian of the S1-1DIS is given by,…”
Section: Theoretical Methodsmentioning
confidence: 99%
“…Recently, the EFTdeveloped by Kaneyoshi has been used in the theoretical investigation of the magnetic features of the nanostructures [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17][18][19][20], due to the description of the lowdimensional systems is very easily applied by using EFT and the theoretical results of that system obtained by EFT are in good consistent with the other theoretical and experimental findings of low-dimensional systems. Such as, magnetic features of the Ising nanowire [21][22][23][24][25][26][27][28][29][30][31][32], core/shell Ising nanostructures [33][34][35], Ising nanotube [36,37], Ising thin film [38], Ising nanolattices [39], Ising nanographene [40] and onedimensional Ising system (1DIS) [41] were worked by using effective field theory. Although the EFT is commonly widely used for the examinations of the magnetic features of the low-dimensional system and its theoretical findings are in good consistent with the experimental results of that system, there is only one work reported by Şarlı [41]…”
Section: Introductionmentioning
confidence: 99%
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“…In this work, the magnetic properties of Ni50Mn36Sn14 HA are investigated by using Kaneyoshi approach (KA) [37][38][39][40] within the effective field theory. There are many researches by using Kaneyoshi approach within EFT: the binary Nickel/Bizmuth alloy [41], the honeycomb structured thin film [42], single-, two-and three-layer [43][44][45], Ising nanographene systems, and carbon diamond nanolattice [46], composite Ising nanoparticles consisting of core and shell [47], cubic nanowire [48], the sc, bcc and fcc nanolattices [49], hexagonal Ising nanowire [50], the nanowire system consisting of composite core and shell [51], transverse Ising nanowire [52], cubic nanowire with core and shell [53], cylindrical Ising nanowires [54][55], the cylindrical core and shell spin-1 ising nanowire [56], spin-1 Ising nanotube [57], the kinetic cylindrical Ising nanotube [58], cylindrical transverse spin-1 Ising nanowire [59], Ising-type segmented nanowire (ISN) [15], the antiferromagnetic YBCO-7 superconductor [60], one-dimensional Ising system (1DIS) [61], a Isingtype endohedral fullerene (EF) with a doped magnetic spin-1/2 particle confined within a spherical cage (by diluted magnetic spin-1 particles) [62], etc.…”
Section: Introductionmentioning
confidence: 99%