4.3 Article

Interfacial thermal transport in spin caloritronic material systems

Journal

PHYSICAL REVIEW MATERIALS
Volume 5, Issue 11, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevMaterials.5.114403

Keywords

-

Funding

  1. U.S. Army Research Laboratory
  2. U.S. Army Research Office [W911NF-18-1-0364]
  3. National Science Foundation [1750786]
  4. DOE BES Award [DE-FG02-07ER46351]
  5. U.S. Department of Energy (DOE) [DE-FG02-07ER46351] Funding Source: U.S. Department of Energy (DOE)
  6. Directorate For Engineering [1750786] Funding Source: National Science Foundation
  7. Div Of Chem, Bioeng, Env, & Transp Sys [1750786] Funding Source: National Science Foundation

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Interfaces play a crucial role in governing the thermal performance of nanoscale devices and nanostructured materials. Research has shown that the thermal boundary conductance between different materials ranges from 50 to 300 MW m(-2) K-1, with variations at different temperatures. This knowledge is essential for accurately modeling the temperature response of nanoscale devices and materials.
Interfaces often govern the thermal performance of nanoscale devices and nanostructured materials. As a result, accurate knowledge of thermal interface conductance is necessary to model the temperature response of nanoscale devices or nanostructured materials to heating. Here, we report the thermal boundary conductance between metals and insulators that are commonly used in spin-caloritronic experiments. We use time-domain thermoreflectance to measure the interface conductance between metals such as Au, Pt, Ta, Cu, and Al with garnet and oxide substrates, e.g., NiO, yttrium iron garnet (YIG), thulium iron garnet (TmIG), Cr2O3, and sapphire. We find that, at room temperature, the interface conductance in these types of material systems range from 50 to 300 MW m(-2) K-1. We also measure the interface conductance between Pt and YIG at temperatures between 80 and 350 K. At room temperature, the interface conductance of Pt/YIG is 170 MW m(-2) K-1 and the Kapitza length is similar to 40 nm. A Kapitza length of 40 nm means that, in the presence of a steady-state heat current, the temperature drop at the Pt/YIG interface is equal to the temperature drop across a 40-nm-thick layer of YIG. At 80 K, the interface conductance of Pt/YIG is 60 MW m(-2) K-1, corresponding to a Kapitza length of similar to 300 nm.

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