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The analysis reveals stray field at the tip position induced by the sample magnetization.
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The chapter presents quantitative observation modes, which produce direct maps of the sample magnetization configuration.
The chord magnetic susceptibility (χ = M/H) can be obtained by measuring the sample's magnetization (M) induced by a weak external dc/ac field (H).
For these purposes, the experimental data of α-Fe2O3 nanoparticles have been utilized such that their magnetization results were measured by vibrating sample magnetization (VSM).
This is consistent with the direction of sample magnetization.
Magnetization per unit mass is not directly related to the microstructure of the sample; therefore, magnetization per unit volume has been calculated by multiplying the magnetization per unit mass with the experimental density, ρexp.
Obtained results are shown in Table 1 together with results of measurements by other methods: XRD, TEM, as well as with results of approximation of sample magnetization dependence measured by VSM in the field range 0.8 T [14].
DC magnetization curves were acquired by equilibrating the sample at the measurement temperature in zero field, incrementally increasing the field, and pausing 100 seconds at each field before measurement.
Heat release in a macroscopic sample of magnetic material is due only to magnetic hysteresis (the loop described by the magnetization of a sample as a function of the applied magnetic field).
With a sample-to-SQUID separation of 400 500 μm, this procedure yielded a two-dimensional magnetic field image produced by the local remanent magnetization of the sample.
The result is that the sample has no net magnetization.
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