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The exchange bias field becomes lower when the number of spins frozen along the cooling field direction is reduced.
b ZFC FC hysteresis loop of nanoparticles measured at 60 K Fig. 3 Plot of calculated values of effective magnetic moment versus cooling field.
f Two-dimensional plot of cooling field against the mean size < d>, while different colors are used to differentiate the values of n.
The dipolar interaction between the FM nanoparticles was investigated by further measuring the cooling field H FC dependent remanent magnetization, using the same experimental protocol; see Fig. 9f.
f Two-dimensional plot of cooling field against the mean size < d>, while different colors are used to differentiate the β values, with β ~ 0 (blue color), β ~ 0.5 (green color), and β = 1 (red color).
It is difficult to describe the difference along the H FC-axis, which could tempt us to conclude that the remanent magnetization behaves as having a cooling field dependence.
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In order to relate the cooling field to the exchange bias phenomena, we have to measure the exchange bias at various cooling fields.
To gain further insight into the influence of cooling fields, we measure a series of cooling field-dependent magnetization as a function of time, as shown in Fig. 8f.
Ferroelectric oxides are used widely in the microelectronic, ferroelectric, optoelectronic, and refrigerated cooling fields on account of their high dielectric constant, and large spontaneous polarization [1,2].
Measurements of the magnetization as a function of temperature after Zero field cooling and field cooling were carried out by using a MPMS Quantum Design SQUID magnetometer.
Magnetic measurements as a function of temperature and magnetic field at field cooling and zero-field cooling modes, provided a Curie temperature around 230 K, saturation magnetization of about 81 emu/g, and coercive field of 390 Oe at 10 K.
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