1993
DOI: 10.1117/12.161947
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<title>Converging TIR lens for nonimaging concentration of light from compact incoherent sources</title>

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Cited by 6 publications
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“…The aim of this design is to avoid the metalized surfaces, which cause reflection losses and are difficult to manufacture, and to optimize the position of the emitter/receiver for the encapsulation, electrical connection, and heat sink. A concentrator with a magnification of 1256 × has a theoretical efficiency of 100% (without optical losses) with an acceptance angle of ± 1.7° and aspect ratio of 0.34 [37,39]. Figure 10 shows another 3D freeform device designed by SMS for CPV applications.…”
Section: Simultaneous Multiple Surface Methodsmentioning
confidence: 99%
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“…The aim of this design is to avoid the metalized surfaces, which cause reflection losses and are difficult to manufacture, and to optimize the position of the emitter/receiver for the encapsulation, electrical connection, and heat sink. A concentrator with a magnification of 1256 × has a theoretical efficiency of 100% (without optical losses) with an acceptance angle of ± 1.7° and aspect ratio of 0.34 [37,39]. Figure 10 shows another 3D freeform device designed by SMS for CPV applications.…”
Section: Simultaneous Multiple Surface Methodsmentioning
confidence: 99%
“…Since 1990, Light Prescriptions Innovators Europe (LPI, Altadena, USA) has designed a variety of concentrators used in CPV, including R(refractive)R [37], X(reflective)R [37], RX [38], RXI [total internal reflection (TIR)] concentrator [38], TIR-R concentrator [37,39], and so on. Taking the TIR-R concentrator, for example, as shown in Figure 9, it has two parts: the primary surface is TIR surface as a microstructure with infinitesimal flat facets, and the secondary surface is refractive surface.…”
Section: Simultaneous Multiple Surface Methodsmentioning
confidence: 99%