Transition from near-field thermal radiation to phonon heat conduction at sub-nanometre gaps

When the separation of two surfaces approaches sub-nanometre scale, the boundary between the two most fundamental heat transfer modes, heat conduction by phonons and radiation by photons, is blurred. Here we develop an atomistic framework based on microscopic Maxwell's equations and lattice dyn...

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Bibliographic Details
Main Authors: Chiloyan, Vazrik (Contributor), Garg, Jivtesh (Author), Esfarjani, Keivan (Author), Chen, Gang (Contributor)
Other Authors: Massachusetts Institute of Technology. Department of Mechanical Engineering (Contributor)
Format: Article
Language:English
Published: Nature Publishing Group, 2015-11-10T19:28:45Z.
Subjects:
Online Access:Get fulltext
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100 1 0 |a Chiloyan, Vazrik  |e author 
100 1 0 |a Massachusetts Institute of Technology. Department of Mechanical Engineering  |e contributor 
100 1 0 |a Chen, Gang  |e contributor 
100 1 0 |a Chiloyan, Vazrik  |e contributor 
100 1 0 |a Chen, Gang  |e contributor 
700 1 0 |a Garg, Jivtesh  |e author 
700 1 0 |a Esfarjani, Keivan  |e author 
700 1 0 |a Chen, Gang  |e author 
245 0 0 |a Transition from near-field thermal radiation to phonon heat conduction at sub-nanometre gaps 
260 |b Nature Publishing Group,   |c 2015-11-10T19:28:45Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/99896 
520 |a When the separation of two surfaces approaches sub-nanometre scale, the boundary between the two most fundamental heat transfer modes, heat conduction by phonons and radiation by photons, is blurred. Here we develop an atomistic framework based on microscopic Maxwell's equations and lattice dynamics to describe the convergence of these heat transfer modes and the transition from one to the other. For gaps >1 nm, the predicted conductance values are in excellent agreement with the continuum theory of fluctuating electrodynamics. However, for sub-nanometre gaps we find the conductance is enhanced up to four times compared with the continuum approach, while avoiding its prediction of divergent conductance at contact. Furthermore, low-frequency acoustic phonons tunnel through the vacuum gap by coupling to evanescent electric fields, providing additional channels for energy transfer and leading to the observed enhancement. When the two surfaces are in or near contact, acoustic phonons become dominant heat carriers. 
520 |a United States. Dept. of Energy. Office of Basic Energy Sciences (DE-FG02-02ER45977) 
546 |a en_US 
655 7 |a Article 
773 |t Nature Communications