Compensation and critical behavior of Ising mixed spin (1-1/2-1) three layers system of cubic structure

Magnetic properties and phase diagrams of mixed spin-1 and spin-1/2 Ising model on a checkerboard square structure: A Monte Carlo study

“…6 (b and c). We can remark that a similar double-peak phenomenon in χtot and C curves has been observed for the mixed spin-5/2 and spin-2 Ising model on a decorated square lattice [27], triple layer spin (1-1/2-1) cubic system [34], mixed-spin (1/2, 1) Ising double layer superlattice [35] and cylindrical core/shell spin-1 Ising nanowire [38]. The figure also shows that MA changes more rapidly than MB because of the weaker exchange coupling J1.…”

“…Therefore, it is not just the magnetic interaction that influenced the Tcomp and Tc, but the crystal field D has significant on both temperatures. In our earlier work on different structures, we ignored the crystal field because of its weak significance [14,34]. The same behavior has also been observed in nanoparticles with hexagonal core-shell structure [36].…”

Compensation and transition order temperature behavior of mixed spin-1 and spin-1/2 ising model on a centered honeycomb-hexagonal structure: two points of compensation

“…A similar system to this structure can be found in the nano-graphene system [39] and be applicable for bimetallic layered compounds [40,41]. Similar works were done by us using different crystal structures [18,42,43].…”

“…The two-dimensional structure is the most widely studied because of its wide range of high-density recording media applications. Various studies emphasize the effect of temperature, magnetic field, exchange coupling, and crystal field on the magnetic properties of the system [16][17][18]. Many shaped structures have been studied such as hexagonal core-shell [19][20][21], ladderlike boronene nanoribbon [22], square-octagon lattice [23], Blume-Capel system for square and simple cubic lattices [24][25][26], borophene core-shell structure [27], ladder-like graphene nanoribbon [28][29][30][31], triangular lattice [31,32], diamond-like decorated square [33], rectangle Ising nanoribbon [34].…”

Magnetic properties of the ferrimagnetic triangular nanotube with core–shell structure: A Monte Carlo study

“…Among the different mixed spin structures studied within the Ising model, the twodimensional structure remains the most widely studied structure in the literature. Various shapes of the two-dimensional structures such as the triangular [39], cubic [40], honeycomb [41] have been studied thoroughly within this model. In recent years, a growing interest has been observed in simulating the magnetic properties of various shapes of the two-dimensional nanotube structure [42][43][44] within the framework of the Ising model because of its wide range of applications in high-density recording media.…”