Fig. 2
From: Nuclear spin assisted quantum tunnelling of magnetic monopoles in spin ice

Controlled cooling of spin ice below its freezing temperature. How the temperature of the samples varies during and after the AQP: a The applied field (black) during an AQP, and the temperatures measured by a small thermometer glued directly on top of the samples (schematically shown in (b)) vs. log time for Ho2Ti2O7 (HTO, red) and natDy2Ti2O7 (DTO, blue). The inset shows a zoom of the first 6 s vs. time. b Comparison of the sample cooling rates dT/dt as a function of temperature after the AQP for Ho2Ti2O7 and natDy2Ti2O7 from the data in (a) to the equilibrium cooling rate dT/dτ extracted from ac susceptibility data for the two samples (see Supplementary Fig. 6). The cooling rate for Ho2Ti2O7 crosses the equilibrium rate at ~0.9 K, and natDy2Ti2O7 at 0.72 K