In this paper we study the propagation of light through an asymmetric array of dielectric multilayers built by joining two porous silicon substructures in a Fibonacci sequence. Each Fibonacci substructure follows the well-known recursive rule but in the second substructure dielectric layers A and B are exchanged. Even without mirror symmetry, this array gives rise to multiple transparent states, which follow the scaling properties and self-similar spectra of a single Fibonacci multilayer. We apply the transfer matrix formalism to calculate the transmittance. By setting the transfer matrix of the array equal to ± I, the identity matrix, frequencies of perfect light transmission are reproduced in our theoretical calculations. Although the light absorption of porous silicon in the optical range limits our experimental study to low Fibonacci generations, the positions of the transparent states are well predicted by the above-mentioned condition. We conclude that mirror symmetry in arrays of Fibonacci multilayers is sufficient but not necessary to generate multiple transparent states, opening broader applications of quasiperiodic systems as filters and microcavities of multiple frequencies.
We calculate the optical constants of porous silicon ͑por-Si͒ from the electronic band structure obtained by means of an sp 3 s* tight-binding Hamiltonian and a supercell model, in which the pores are columns dug in crystalline Si. The position of the absorption edge of the material is defined by two competing effects: ͑i͒ transitions assisted by the scattering of carriers on the lattice of pores, which effectively decrease the ''indirectness'' of por-Si and result in a redshift of the absorption edge, and ͑ii͒ quantum confinement, which increases the band gap. The interplay between these effects is illustrated by calculating the imaginary part of the dielectric function for 8-, 32-, and 128-atom supercells with different porosities. We also show how the supercell model can be extended to take into account weak disorder, which produces nonvertical optical transitions in k space and smoothens the absorption spectra. Our results, obtained without any adjustable parameters, are compared with experimental data. ͓S0163-1829͑99͒05023-7͔
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