Abstract
We use a Bi gaussmeter of micron dimensions to explore the magnetic field dependence of the magnetization relaxation rate and the critical current down to millikelvin temperatures in untwinned single crystals of $\mathrm{Y}{\mathrm{Ba}}_{2}{\mathrm{Cu}}_{3}{\mathrm{O}}_{7\ensuremath{-}\ensuremath{\delta}}$ with columnar defects. The response separates into three regimes as a function of the ratio of vortex density to columnar defect density $\frac{B}{{B}_{\ensuremath{\varphi}}}$: enhancements in both critical current and quantum creep in the dilute limit, vanishing magnetization relaxation at the matching density (the proposed "Mott insulator" phase line), and the emergence of temperature-dependent vortex motion for $B\ensuremath{\gg}{B}_{\ensuremath{\varphi}}$.
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