1997
DOI: 10.1364/josaa.14.003001
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Thermodynamic limit to light trapping in thin planar structures

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Cited by 111 publications
(112 citation statements)
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“…7 However, Stuart and Hall wrote r m ¼ C m av m g u m (their Equation (15)); v m g is the group velocity of mode m, not the group velocity for a radiative mode. 3 As a consequence, their expression (18b) for f m (the fractional absorption) contains v m g =v 0 g , which is the ratio of the group velocity of the waveguide mode to the ordinary speed of light in a material of index n. With our interpretation, the ratio is v 0 g =v 0 g , which of course simplifies their expression to the one we've used (Eq. (4) above).…”
Section: Appendix A: Dielectric Absorption For Wave-guide Modes and Smentioning
confidence: 91%
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“…7 However, Stuart and Hall wrote r m ¼ C m av m g u m (their Equation (15)); v m g is the group velocity of mode m, not the group velocity for a radiative mode. 3 As a consequence, their expression (18b) for f m (the fractional absorption) contains v m g =v 0 g , which is the ratio of the group velocity of the waveguide mode to the ordinary speed of light in a material of index n. With our interpretation, the ratio is v 0 g =v 0 g , which of course simplifies their expression to the one we've used (Eq. (4) above).…”
Section: Appendix A: Dielectric Absorption For Wave-guide Modes and Smentioning
confidence: 91%
“…In this paper we shall use the basic formalism developed by Stuart and Hall for their calculations of the thermodynamic limit for the absorptance of a thin semiconductor film 3 ; they note that their approach is an application of the extended radiance theorem proven by Bassett. 14 In this section we briefly reprise some of their results that we use subsequently when surface plasmon polaritons are incorporated.…”
Section: Thermodynamic Absorptance In a Thin Semiconductor Filmmentioning
confidence: 99%
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