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Light Absorption and Carrier Generation

Light absorption and charge carrier generation in solids... [Pg.354]

The number of charge carriers generated in the SCR depends on the absorbed flux of incident photons per unit area P, the width W of the SCR and the wave-length-dependent absorption coefficient a of bulk Si. The latter parameter is shown in Fig. 7.6, while the resulting penetration depth for light of different wavelengths is shown in Fig. 10.4a. [Pg.212]

In organic cells, however, the steps involved in the generation of photo-current are (1) light absorption, (2) exciton creation, (3) exciton diffusion, (4) exciton dissociation in the bulk or at the surface, (5) field-assisted carrier separation, (6) carrier transport, and (7) carrier delivery to external circuit. Assuming that only the excitons which reach the junction interface produce free carriers, if the blocking contact is illuminated [65],... [Pg.813]

See other pages where Light Absorption and Carrier Generation is mentioned: [Pg.2679] [Pg.25] [Pg.3135] [Pg.3159] [Pg.2679] [Pg.25] [Pg.3135] [Pg.3159] [Pg.345] [Pg.238] [Pg.152] [Pg.3] [Pg.350] [Pg.30] [Pg.121] [Pg.360] [Pg.388] [Pg.521] [Pg.307] [Pg.261] [Pg.368] [Pg.379] [Pg.129] [Pg.290] [Pg.251] [Pg.173] [Pg.242] [Pg.346] [Pg.191] [Pg.212] [Pg.149] [Pg.379] [Pg.532] [Pg.68] [Pg.114] [Pg.273] [Pg.214] [Pg.9] [Pg.16] [Pg.1] [Pg.129] [Pg.87] [Pg.276] [Pg.370] [Pg.205] [Pg.251] [Pg.67] [Pg.285] [Pg.811]

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Absorption light

Carrier Generators

Carrier generation