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Figure 6 Peak of third-order susceptibility as a function of relaxation constant.
Figure 3 Second-order susceptibility as a function of sample thickness for a doped sample Figure 4 Second-order susceptibility as a function of sample thickness for the undoped sample.
Figure 5 Second-order susceptibility as a function of Cu-doping density for a sample with thickness 2.5 nm Figure 6 Second-order susceptibility as a function of Cu-doping density for a thin sample.
Figure 5 shows the second-order susceptibility as a function of Cu-doping density for a sample with crystal thickness 2.5 nm.
Inset: inverse susceptibility as a function of temperature: a 0.05 M cobalt concentration, b 0.18 M cobalt concentration Figure 8 Variation of χT with temperature.
A quantum design physical property measurement system magnetometer was used to measure AC susceptibility as a function of magnetic field, frequency, temperature and field history.
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Measurements of magnetization and AC-susceptibility as a function of temperature were performed with a quantum design SQUID magnetometer.
(b) Magnetic susceptibilities as a function of Co doping.
Using a one-pass UVC exposure chamber, however, we have shown that vaccinia virus (a surrogate for variola major) is susceptible to UVC and that the susceptibility varies as a function of dose and relative humidity (RH).[8] In these dose-response experiments the fluence rate and exposure time, and therefore, dose were carefully controlled.
Inset in Fig. 7a and 7b displayed the inverse susceptibility (χ−1) as a function of temperature with cobalt concentrations of 0.05 and 0.18 M, respectively.
The hollandite oxides were characterized by X-ray diffraction analysis and magnetic susceptibility measurements as a function of temperature in the range 298 550 K which in turn allows postulation of each cationic distribution.
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