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. 2022 Apr 20;16(5):6960–7079. doi: 10.1021/acsnano.1c09150

Figure 42.

Figure 42

Spin Seebeck effect and magnon transport with 2D magnets. (a) Crystal structure of CGT and CST.467 (b) Schematic of the longitudinal SSE measurements in CST/Pt or CGT/Pt bilayers. H denotes the external magnetic field and ΔT (∇T) the temperature difference (gradient).467 (c, d) Normalized SSE voltage S = (V/∇T) (Lz/Ly) as a function of H in the (c) CST/Pt and (d) CGT/Pt bilayers at selected temperatures.467 Panels (a–d) are adapted with permission from ref (467). Copyright 2019 American Physical Society. (e) Schematic of the magnon generation, transport, and detection in MnPS3.468 (f) Optical image of the device with the MnPS3 flake and Pt electrodes, including the measurement configuration of the nonlocal SSE.468 (g) Normalized nonlocal signal Inline graphic as a function of distance (d) for selected temperatures in a 16 nm-thick MnPS3 flake. The solid lines represent the best-fitting results based on a diffusion equation.468 (h) Magnon diffusion length as a function of MnPS3 thickness (t) for selected temperatures.468 Panels (e–h) are adapted with permission under a Creative Commons CC BY 4.0 license from ref (468). Copyright 2019 American Physical Society.