Beilstein J. Nanotechnol.2019,10, 1348–1359, doi:10.3762/bjnano.10.133
doping on structure, morphology and magnetic properties of CoxFe3−xO4 samples was investigated. In particular, we examined the interparticle interactions in the samples by δm graphs and Henkelplots that have not been reported before in literature. Finally, we studied the hyperthermia properties and
observed that the heat efficiency of soft Fe3O4 is about 4 times larger than that of hard CoFe2O4 ferrite, which was attributed to the high coercive field of samples compared with the external field amplitude.
Keywords: anisotropy; cobalt; ferrite; Henkelplots; hyperthermia therapy; nanoparticles
and Henkelplots are shown in Figure. 12. The interaction field increases with increasing cobalt content, which can be related to the particle size and the larger magnetic moment of bigger nanoparticles [13][47]. The particle aggregation visible in FE-SEM images shows that the particles are
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Figure 1:
(a) XRD patterns of the CoxFe3−xO4 (0 ≤ x ≤1) nanoparticles. (b) Shift of the (440) reflection.
Beilstein J. Nanotechnol.2011,2, 473–485, doi:10.3762/bjnano.2.51
boundaries facing a Pt-rich environment. Moreover, magnetic coupling of NPs can be excluded as shown by Henkelplots.
On the Pt(100) epitaxial films a completely different behavior has been observed up to intermediate annealing temperature TA = 380 °C. In this regime, both µL/µSeff and the coercive field
: 30 min). The lines are given as guides to the eye.
(a) In-plane hysteresis loops measured by SQUID magnetometry at T = 29 K, i.e., close to the compensation temperature of the diamagnetic MgO substrate and the paramagnetic Pt(111) film on top. In (b), the Henkelplots for three annealing steps are
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Figure 1:
(a) XRD of Pt films on STO(100) and MgO(100) in Bragg–Brentano geometry. The diffractograms clearly...