Nuclear spin assisted quantum tunnelling of magnetic monopoles in spin ice

The data of Fig 3 a-c are stored as column 1 (magnetisation) column 2 (time) for the different wait times for each experiment (isotope of spine ice ) below the freezing temperature. Clearly the magnetisation changes depending on the wait time showing non-equilibrium behaviour The data of Fig 4 a-c are stored as column 1 (field) column 2 (magnetisation) for the different wait times in each sheet for the different isotopes of spin ice. Clearly the thermal avalanches changes depending on the wait time showing non-equilibrium behaviour.