Abstract

We investigate thermal transport in square ice, a two-dimensional analogue of spin ice, exploring the role played by emergent magnetic monopoles in transporting energy. Using kinetic Monte Carlo simulations based on energy preserving extensions of single-spin-flip dynamics, we explicitly compute the (longitudinal) thermal conductivity, κκ, over a broad range of temperatures. We use two methods to determine κκ: a measurement of the energy current between thermal baths at the boundaries, and the Green-Kubo formula, yielding quantitatively consistent values for the thermal conductivity. We interpret these results in terms of transport of energy by diffusion of magnetic monopoles. We relate the thermal diffusivity, κ/Cκ/C where CC is the heat capacity, to the diffusion constant of an isolated monopole, showing that the subdiffusive monopole implies κ/Cκ/C vanishes at zero temperature. Finally, we discuss the implications of these results for thermal transport in three-dimensional spin ice, in spin ice materials such as Dy2_2Ti2_2O7_7 and Ho2_2Ti2_2O7_7, and outline some open questions for thermal transport in highly frustrated magnets.

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