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Hysteresis loops were obtained by using maximum applied field up to 50 kOe at 5 and 300 K.
The results indicate that the bead's remnant magnetization is half of the value at maximum applied field in all cases.
The maximum applied field, 8 kOe, does not saturate the magnetizations which should be attributed to weak ferromagnetic ordering of the spins in the nanoparticles.
The GMI ratio was defined with respect to the magnetically saturated sample in the maximum applied field of Hsat = 12 kA/m.
Hysteresis loops with a maximum applied field of 1 T were measured at room temperature with a Princeton Vibrating Sample Magnetometer (VSM) (noise level ~10−7 Am2).
Figure 11 shows the magnetization versus magnetic field (M H) hysteresis loops for the BNTF nanoparticles at room temperature for the maximum applied field (H) of 20 kOe.
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The magnetic field dependence of MR was measured using a conventional four-probe method in the maximum applied magnetic field of 20 kOe with current in the plane at RT.
The hysteresis loop did not reach magnetization saturation, even at the maximum applied magnetic field (to 10 kOe).
The hysteresis loops were obtained at the maximum applied electric field of 20 kV/cm and a frequency of 50 Hz.
Magnetic M(H) measurements were performed at 2 and 300 K with a maximum applied magnetic field of 6 T using a superconducting quantum interference device (SQUID) equipment from Quantum Design (SQUID, San Diego, California, USA).
The magnetization versus magnetic field (M H) curves for samples S1 to S4 are displayed in Figure 5a which were measured at 300 K under the maximum applied magnetic field of 5,000 Oe using a sample holder of high-purity capsules free from any metallic impurity.
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