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The FS6 nanoparticles were superparamagnetic as evidenced by the zero coercivity [23].
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The zero coercivity FePt nanoparticle transforms to nonzero after post-treatment at 200 °C, which proves once again that the Fe3O4 nanoparticle are generated by using the post-treatment method.
From hysteresis measurements, the zero coercivity fields of IOSi-NPs can be considered equal to 0 Oe at 300 K.
The nanocomposite samples exhibited superparamagnetic behaviour as evidenced by zero remanence, zero coercivity and the absence of hysteresis loops.
The synthesized MNPs also show a superparamagnetic behavior, as evidenced by zero coercivity and remanance on the magnetization loops.
For the films annealed at 500°C, the FePt/Ru shows nearly zero coercivity, and the FePt single layer shows a very low perpendicular coercivity, while the FePt/Ag film shows hard magnetic properties with a dramatically high coercivity of 4 kOe, which is obviously larger than that of the FePt/Ru and FePt single layer.
The PNCs do not show hysteresis loop with zero coercivity, indicating the superparamagnetic behavior at room temperature.
This is further supported by the magnetization hysteresis (M H) curve taken at 300 K, for the as-deposited thin film, which shows zero coercivity and remanence.
The experimental activation volume agreed with the result calculated by the dynamic coercivity method.
If the boundedness of is replaced by the uniform coercivity of in Theorem 2.5, then we have the following result.
Taking (v_{h}=w_{h}), by the coercivity results stated in Theorem 4.2, we have |w_{h}|_{varepsilon}=0.
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