We measured the ac susceptibility of sintered Y₁{Ba}₂Cu₃{O}_{7{{-}}{{δ}}}$ pellets as a function of temperature and ac magnetic field amplitude and frequency. The imaginary part of the susceptibility {χ}'' exhibits two peaks. A narrow peak is located at the critical temperature of the grains. A broad peak at lower temperature is attributed to hysteresis losses at the grain boundaries. There is a small shift in this coupling peak to higher temperature as the frequency increases from 10 to 1000 Hz. We explain the shift in terms of Anderson flux creep on a time scale of milliseconds. The shift depends on the amplitude of the measuring field. The activation energy for flux creep ranges from 11.9±{}1.0 eV in the zero-field limit [0.8 A mʳ-r1(0.01 Oe)] to 1.2±{}0.3 eV at 800 A m^-1(10 Oe). We extrapolate our data to find the value for an intergrain decoupling field of 1--2 kA m-1 (13--25 Oe), above which flux creep presumably becomes flux flow at the grain boundaries.
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Nikolo et al. (1989) studied this question.
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