The Franz-Keldysh effect is a change in optical absorption by a semiconductor when an electric field is applied. The effect is named after the German physicist Walter Franz and Russian physicist Leonid Keldysh (nephew of Mstislav Keldysh). As originally conceived, the Franz-Keldysh effect is the result of wavefunctions "leaking" into the band gap. When an electric field is applied, the electron and hole wavefunctions become Airy functions rather than plane waves. The Airy function includes a "tail" which extends into the classically-forbidden band gap. According to Fermi's Golden Rule, the more overlap there is between the wavefunctions of a free electron and a hole, the stronger the optical absorption will be. The Airy tails slightly overlap even if the electron and hole are at slightly different potentials (slightly different physical locations along the field). The absorption spectrum now includes a tail at energies below the band gap and some oscillations above it. This explanation does, however, omit the effects of excitons, which may dominate optical properties near the band gap. The Franz-Keldysh effect occurs in uniform, bulk semiconductors, unlike the quantum confined Stark effect, which requires a quantum well. Both are used for Electro-absorption modulators. The Franz-Keldysh effect usually requires hundreds of volts, limiting its usefulness with conventional electronics - although this is not the case for commercially available Franz-Keldysh-effect electro-absorption modulators that utilize a waveguide geometry to guide the optical carrier. See also Franz-Keldysh effect and modulation spectroscopy
W. Franz, Einfluß eines elektrischen Feldes auf eine optische Absorptionskante, Z. Naturforschung 13a (1958) 484-489. Retrieved from "http://en.wikipedia.org/" |
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