4.7 Article

Super-Planckian thermal radiation between 2D phononic hBN monolayers

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出版社

ELSEVIER FRANCE-EDITIONS SCIENTIFIQUES MEDICALES ELSEVIER
DOI: 10.1016/j.ijthermalsci.2021.107315

关键词

LO phonons; Tunneling; NFRHT; Hybridization coupling; LDOS

资金

  1. NSFC [61775195, 62075196]
  2. NSFC of Zhejiang Province [LR15F050001, LZ17A040001]
  3. National Key Research and Development Program of China [2017YFA0205700]

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The study investigated near-field radiation heat transfer in 2D hexagonal boron nitride monolayer and composite structures, finding that phononic modes split into LO and TO modes disappear in 2D materials at the Gamma-point. The conductivity of atomic thin hBN monolayer is dependent on the LO phonon frequency. By tuning Fermi energy, the flux density between monolayer hBN can be enhanced by 2.8 times, showing great potential for designing thermally controlled devices.
Near-field radiation heat transfer (NFRHT) in two-dimensional (2D) hexagonal boron nitride (hBN) monolayer and its composite symmetric-based structure was investigated. Contrary to three-dimensional (3D) materials, the splitting of modes (in 2D materials) into the longitudinal optical (LO) and transverse optical (TO) phononic modes disappears at the Gamma-point even in some polar materials. The conductivity of atomic thin hBN monolayer depends on the LO phonon frequency under the long wavelength limit. Exploiting such concept, the electromagnetic local density of states (EM-LDOS) accounting for the near-field radiation spectrum was evaluated in free-space close to an interface with the hBN monolayer as well as composite structures. An intense narrow peak of LDOS was found in the case of hBN monolayer caused by the surface phonon polariton (SPhP) resonance. This peak was modified in the case of hBN-graphene composite due to hybridization, which strongly depends on two factors - the distance of observer (in vacuum) from interface and graphene Fermi energy. It was found that the flux density between monolayer hBN gets 2.8-fold enhanced as compared to the monolayer graphene configuration under 0.11 eV Fermi energy applied at a vacuum gap of 15 nm. The possibility of tuning Fermi energy has great potentials in designing thermally controlled devices.

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