Near-Field Radiative Heat Transfer Across Nanometer Vacuum Gaps 2016
DOI: 10.1016/b978-0-323-42994-8.00007-6
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Applications of Near-Field Thermal Radiation

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Cited by 1 publication
(2 citation statements)
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“…To elucidate such an observation, the photocurrent generation is measured as a function of the vacuum gap distance and compared with theoretical predictions based on the fluctuational electrodynamics and quantum efficiency of the PV cell (see the Methods section). Figure b clearly reveals the oscillatory nature of the photocurrent with respect to the vacuum gap distance, unlike the monotonic increase in the heat transfer in the near field. , This oscillation occurs because the PV cell utilizes photons whose energy is greater than the band-gap energy; that is, the PV cell acts as an optical short-wavelength-pass filter. Due to the coherence of thermal radiation in the far-to-near-field transition regime, our experiments demonstrate that the performance of the NF-TPV device is not always improved as the emitter closely approaches the PV cell.…”
Section: Resultsmentioning
confidence: 98%
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“…To elucidate such an observation, the photocurrent generation is measured as a function of the vacuum gap distance and compared with theoretical predictions based on the fluctuational electrodynamics and quantum efficiency of the PV cell (see the Methods section). Figure b clearly reveals the oscillatory nature of the photocurrent with respect to the vacuum gap distance, unlike the monotonic increase in the heat transfer in the near field. , This oscillation occurs because the PV cell utilizes photons whose energy is greater than the band-gap energy; that is, the PV cell acts as an optical short-wavelength-pass filter. Due to the coherence of thermal radiation in the far-to-near-field transition regime, our experiments demonstrate that the performance of the NF-TPV device is not always improved as the emitter closely approaches the PV cell.…”
Section: Resultsmentioning
confidence: 98%
“…The near-field radiation between the emitter and the PV cell is calculated by adding contributions of propagating and evanescent modes, as ,, where Θ­(ω, T i ) = ℏω/{exp­[ℏω/( k B T i )] – 1} is the mean energy of the Planck oscillator, ω is the angular frequency, ℏ is the reduced Planck constant, k B is the Boltzmann constant, and T 1 and T 2 are the temperature of the emitter and the PV cell, respectively. The exchange functions for propagating and evanescent waves are expressed by where r 01 p,s and r 02 p,s are the modified reflection coefficients for the vacuum/doped-Si/SiO 2 (or vacuum/SiO 2 ) and vacuum/Au/ n -GaSb multilayers, respectively.…”
Section: Methodsmentioning
confidence: 99%