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-3 Hz at which the thermal wavelength is still shorter than the sample size (we are still in the thermally thick limit). However, the dc impedance does see the outer boundary, as it has "infinite" time to reach steady state. To compensate for this we add a small frequency, temperature, and amplitude-independent correction term to the limiting value of Z2 when estimating Z0. This correction term value was chosen, so that measurements with different amplitudes give the same values for A (T).
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- 3 Hz at which the thermal wavelength is still shorter than the sample size (we are still in the thermally thick limit). However, the dc impedance does see the outer boundary, as it has "infinite" time to reach steady state. To compensate for this we add a small frequency, temperature, and amplitude-independent correction term to the limiting value of Z 2 when estimating Z 0. This correction term value was chosen, so that measurements with different amplitudes give the same values for A (T).
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