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Beilstein J. Nanotechnol. 2023, 14, 485–493, doi:10.3762/bjnano.14.39
Figure 1: (a) Dependence of the SAR of randomly oriented assemblies of nanoparticles of various diameters dis...
Figure 2: (a) Dependence of the SAR on the dc magnetic field applied perpendicular to the ac magnetic field f...
Figure 3: (a) Dynamics of αx and αz components of the unit magnetization vector of a nanoparticle with D = 30...
Figure 4: Evolution of the normalized energy density of a particle, W(θ,φ)/K1V, as a function of dc magnetic ...
Figure 5: (a) Schematic representation of the crossed uniform ac and non-uniform dc magnetic field geometry w...
Beilstein J. Nanotechnol. 2019, 10, 2294–2303, doi:10.3762/bjnano.10.221
Figure 1: Dynamics of the unit magnetization vector in RMFs in the magneto-dynamics approximation for various...
Figure 2: The domains of various magneto-dynamic modes of motion of a superparamagnetic nanoparticle in a vis...
Figure 3: The domains I–III of the different magneto-dynamic modes of nanoparticle motion in a viscous liquid...
Figure 4: Comparison of the SAR of a dilute assembly of superparamagnetic nanoparticles in AMFs and RMFs depe...
Figure 5: a) SAR in RMFs for dilute assemblies of superparamagnetic nanoparticles with various magnetic aniso...
Figure 6: Comparison of the experimentally measured SAR values [41] at frequencies f = 130 and 160 kHz and amplit...
Figure 7: a) SAR of a dilute assembly of iron oxide nanoparticles of different diameters at a fixed frequency...