Fig. 2 | Nature Communications

Fig. 2

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

Fig. 2

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/ 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

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