Proceedings of 1994 IEEE 1st World Conference on Photovoltaic Energy Conversion - WCPEC (A Joint Conference of PVSC, PVSEC and
DOI: 10.1109/wcpec.1994.520557
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Design and fabrication of thermophotovoltaic cells

Abstract: Recent advances in PV cell technology and in thermal emitters has led t o renewed interest in TPV electric power generation. We review thermal sources, theoretical analysis t o select materials with optimum bandgap, and fabrication of efficient TPV cells. Some experimental data are included. BACKGROUND

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Cited by 5 publications
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“…Broadband radiator establishes the emission across a wide range of wavelength for temperature range between 1000 to 2000 K [32,37]. Examples of broadband radiators are alumina, zirconia, magnesia, silica, yttria, and more, which possess a major challenge in low thermal shock resistance and low emissivity [38].…”
Section: Tpv System Overviewmentioning
confidence: 99%
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“…Broadband radiator establishes the emission across a wide range of wavelength for temperature range between 1000 to 2000 K [32,37]. Examples of broadband radiators are alumina, zirconia, magnesia, silica, yttria, and more, which possess a major challenge in low thermal shock resistance and low emissivity [38].…”
Section: Tpv System Overviewmentioning
confidence: 99%
“…A radiator emits electromagnetic energy by translating heat from generators into an emission spectrum to provide appropriate receiver cell sensitivity [ 22 ]. Selective radiators such as silicon carbide (SiC), tungsten (W), W-SiO 2 rare-earth oxide, and photonics crystal (PhC) provide narrow spectral range emission by enhancing in-band radiation and suppressing out-of-band radiation [ 28 , 29 , 30 , 31 , 32 , 33 , 34 ]. There are two significant types of selective radiators, namely the rare-earth oxide radiator and the broadband radiator [ 35 ].…”
Section: Tpv System Overviewmentioning
confidence: 99%
“…The selective emitters were generated with several techniques; grating structures using micro/nano-scale fabrication technique [36], magnetic polaritons [37], and metamaterials such as (i) epsilon-near zero [38], (ii) passivated platinum and alumina [17], and (iii) alternate tungsten and alumina [39]. There are several types of selective emitters that have been discussed in the literature, which are silicon carbide (SiC) [7], tungsten (W) [40], rareearth oxide [41], and photonics crystal (PhC) [42] [43]. Among the selective emitters, rare-earth oxide is an isolated ion, serves as the most popular candidate for selective emitter.…”
Section: B Tpv Emittermentioning
confidence: 99%
“…Another reason for this development is connected with thermophotovoltaic power converters. It was shown that materials with bandgap energy lower than 0.7 eV are very promising for thermophotovoltaic applications [7,8]. Over the emitter temperature range 1000-2000K the optimum bandgap for maximum electrical power density output is around 0.5-0.6 eV [7, 81, decreasing slightly for lower temperatures.…”
Section: Ingasbas/gasb Cellsmentioning
confidence: 99%