4.6 Article

Coherent phonon transport in short-period two-dimensional superlattices of graphene and boron nitride

Journal

PHYSICAL REVIEW B
Volume 93, Issue 12, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevB.93.125427

Keywords

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Funding

  1. Natural Sciences and Engineering Research Council of Canada (NSERC) through the Discovery grant program
  2. Natural Sciences and Engineering Research Council of Canada (NSERC) through the Collaborative Research and Development (CRD) grant program
  3. Canada Foundation for Innovation under the of Compute Canada
  4. Government of Ontario
  5. Ontario Research Fund-Research Excellence
  6. University of Toronto
  7. Canada Foundation for Innovation (CFI)
  8. NanoQuebec
  9. RMGA
  10. Fonds de Recherche du Quebec-Nature et technologies (FRQ-NT)

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Promoting coherent transport of phonons at material interfaces is a promising strategy for controlling thermal transport in nanostructures and an alternative to traditional methods based on structural defects. Coherent transport is particularly relevant in short-period heterostructures with smooth interfaces and long-wavelength heat-carrying phonons, such as two-dimensional superlattices of graphene and boron nitride. In this work, we predict phonon properties and thermal conductivities in these superlattices using a normal mode decomposition approach. We study the variation of the frequency dependence of these properties with the periodicity and interface configuration (zigzag and armchair) for superlattices with period lengths within the coherent regime. Our results showed that the thermal conductivity decreases significantly from the first period length (0.44 nm) to the second period length (0.87 nm), 13% across the interfaces and 16% along the interfaces. For greater periods, the conductivity across the interfaces continues decreasing at a smaller rate of 11 W/mK per period length increase (0.43 nm), driven by changes in the phonon group velocities (coherent effects). In contrast, the conductivity along the interfaces slightly recovers at a rate of 2 W/mK per period, driven by changes in the phonon relaxation times (diffusive effects). By changing the interface configuration from armchair to zigzag, the conductivities for all period lengths increase by approximately 7% across the interfaces and 19% along the interfaces.

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