Photovoltaic Solar Energy Conversion pp 167-200 | Cite as
Advanced Concepts: Beyond the Shockley–Queisser Limit
Chapter
Abstract
The main difference between the theoretical limit of solar energy conversion, like that of a Mueser engine at maximum concentration (see Sect. 4.1.4, where we found η Mues = 0. 86) and the Shockley–Queisser efficiency , representing the radiative limit of a single-gap absorber illuminated by sunlight without concentration (η SQ = 0. 29, [1]) results from
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the excess energy of photons \(\hslash \omega >\epsilon _{\mathrm{g}}\) which is converted into heat,
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the amount of photons \(\hslash \omega <\epsilon _{\mathrm{g}}\) not absorbed,
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the low photon solid angle \(\varOmega _{\mathrm{in}} =\varOmega _{\mathrm{Sun}} = 5.3 \times 10^{-6}\) of non-concentrated sunlight1 compared to the solid angle for emission Ω out (e.g., for flat absorbers with highly reflecting rear contacts Ω out = 2π)
Keywords
Photonic Crystal Fluorescence Photon Intermediate Band Tandem Cell Solar Photon
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