Quantum-coupled single-electron thermal to electric conversion scheme

Thermal to electric energy conversion with thermophotovoltaics relies on radiation emitted by a hot body, which limits the power per unit area to that of a blackbody. Microgap thermophotovoltaics take advantage of evanescent waves to obtain higher throughput, with the power per unit area limited by...

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Bibliographic Details
Main Authors: Wu, D. M. (Contributor), Hagelstein, Peter L. (Contributor)
Other Authors: Massachusetts Institute of Technology. Department of Electrical Engineering and Computer Science (Contributor), Massachusetts Institute of Technology. Research Laboratory of Electronics (Contributor)
Format: Article
Language:English
Published: American Institute of Physics (AIP), 2012-07-16T20:04:30Z.
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Online Access:Get fulltext
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100 1 0 |a Wu, D. M.  |e author 
100 1 0 |a Massachusetts Institute of Technology. Department of Electrical Engineering and Computer Science  |e contributor 
100 1 0 |a Massachusetts Institute of Technology. Research Laboratory of Electronics  |e contributor 
100 1 0 |a Hagelstein, Peter L.  |e contributor 
100 1 0 |a Wu, D. M.  |e contributor 
100 1 0 |a Hagelstein, Peter L.  |e contributor 
700 1 0 |a Hagelstein, Peter L.  |e author 
245 0 0 |a Quantum-coupled single-electron thermal to electric conversion scheme 
260 |b American Institute of Physics (AIP),   |c 2012-07-16T20:04:30Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/71634 
520 |a Thermal to electric energy conversion with thermophotovoltaics relies on radiation emitted by a hot body, which limits the power per unit area to that of a blackbody. Microgap thermophotovoltaics take advantage of evanescent waves to obtain higher throughput, with the power per unit area limited by the internal blackbody, which is n2 higher. We propose that even higher power per unit area can be achieved by taking advantage of thermal fluctuations in the near-surface electric fields. For this, we require a converter that couples to dipoles on the hot side, transferring excitation to promote carriers on the cold side which can be used to drive an electrical load. We analyze the simplest implementation of the scheme, in which excitation transfer occurs between matched quantum dots. Next, we examine thermal to electric conversion with a lossy dielectric (aluminum oxide) hot-side surface layer. We show that the throughput power per unit active area can exceed the n2 blackbody limit with this kind of converter. With the use of small quantum dots, the scheme becomes very efficient theoretically, but will require advances in technology to fabricate. 
546 |a en_US 
655 7 |a Article 
773 |t Journal of Applied Physics