2017
DOI: 10.1103/physrevb.96.125404
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Near-field thermal radiative transfer between two coated spheres

Abstract: In this work, we present an expression for the near-field thermal radiative transfer between two spheres with arbitrary numbers of coatings. We numerically demonstrate that the spectrum of heat transfer between layered spheres exhibits novel features due to the newly introduced interfaces between coatings and cores. These features include broad super-Planckian peaks at non-resonant frequencies and near-field selective emission between metallic spheres with polar material coatings. Spheres with cores and coatin… Show more

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Cited by 14 publications
(10 citation statements)
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“…The effect provides the possibility to strengthen the SPPs near the interface of the substrate, in other words, as surface modes, the SPPs can spread further from the interface. Considering the lack of the channel between metal particles and the substrate, the core/shell configuration of nanoparticles can be utilized to realize the modifying of the particles [20,21]. Inspired by the above, we introduce a concept of a thermal repeater by modifying the particles with shell and embedding the substrate with multilayered graphene sheets, to form strongly coupled modes.…”
mentioning
confidence: 99%
“…The effect provides the possibility to strengthen the SPPs near the interface of the substrate, in other words, as surface modes, the SPPs can spread further from the interface. Considering the lack of the channel between metal particles and the substrate, the core/shell configuration of nanoparticles can be utilized to realize the modifying of the particles [20,21]. Inspired by the above, we introduce a concept of a thermal repeater by modifying the particles with shell and embedding the substrate with multilayered graphene sheets, to form strongly coupled modes.…”
mentioning
confidence: 99%
“…R (M) l (ρ i ) and R (N) l (ρ i ) are the effective Mie reflection coefficients at the interface between region f and sphere i for M (1) lm (k f r i ) and N (1) lm (k f r i ) waves, respectively. See Czapla and Narayanaswamy [12] for the definitions of VSWs and Mie reflection coefficients, which are exactly identical to those used in this work. V X,Y,i, j l,ν,m are scattered field coefficients.…”
Section: Theorymentioning
confidence: 99%
“…To that end, a great deal of research has been directed towards determining explicit formulas for heat transfer in experimentally important thermal systems. Certain problems are best attacked using DGF and spectral density methods, such as NFRHT in plane-plane [9], sphere-sphere [6,[10][11][12], and sphere-plane [6,13] configurations, where the electromagnetic fields are easily described by vector wave eigenfunction expansions. Thermal systems which do not yield to those methods often require methods that involve surface or volume meshing, such as BEM and T-DDA.…”
Section: Introductionmentioning
confidence: 99%
“…Narayanaswamy et al [19] studied the NFRHT between two spherical particles of arbitrary radius based on rigorous solution of the fluctuational electrodynamics theory with an quasi-analytical approach using vector spherical harmonics expansion. Czapla et al [20] extended the method developed by Narayanaswamy et al [19] to investigate NFRHT between two coated spheres with an arbitrary numbers of coatings. Messina et al [21][22][23] proposed a scattering operator method to investigate NFRHT between two particles of arbitrary shape.…”
Section: Introductionmentioning
confidence: 99%