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Beilstein J. Nanotechnol. 2025, 16, 1557–1566, doi:10.3762/bjnano.16.110
Figure 1: Appearance of a cobalt fcc crystallite (500 atoms) together with the orientation of atomic spins at...
Figure 2: Variation of magnetic energy (a) and magnetization modulus (b) of a cobalt fcc crystallite (500 ato...
Figure 3: Dependences of the deviation of the relative normalized magnetic energy (a) and magnetization modul...
Figure 4: Variation of the magnetic energy of cobalt (fcc) normalized by the number of atoms in the system fo...
Figure 5: Variation of the magnetization modulus of cobalt (fcc) normalized by the number of atoms in the sys...
Figure 6: Variation of magnetization vector components (in absolute values) Mα,α = {x,y,z} as a function of c...
Figure 7: Formation of Neel domain walls in a cobalt nanofilm after the relaxation stage.
Figure 8: Variation of cobalt magnetic energy as a function of nanofilm thickness measured in crystalline lay...
Beilstein J. Nanotechnol. 2023, 14, 23–33, doi:10.3762/bjnano.14.3
Figure 1: Problem statement for the complex study of cobalt and niobium heterostructures. The sketch of the N...
Figure 2: Variation of the average value of the crystal lattice ideality parameter in horizontal layers of a ...
Figure 3: Multilayer nanocomposite of niobium and cobalt (a) formed in a numerical experiment during depositi...
Figure 4: Spatial distribution of cobalt atom spins for ideal crystal hexagonal close-packed lattice (a), (b)...
Figure 5: Changes in spin temperature under a constant external magnetic field of 1.0 T for ideal hexagonally...
Figure 6: Changes in the magnetization vector modulus under a constant external magnetic field with an induct...