Advances in the calculation of optical properties in superlattices; novel insights derived from the theory of finite periodic systems

摘要

Using the genuine superlattice eigenvalues and eigenfunctions, and their parity symmetries, new transition selection rules are derived, and a novel approach for the explicit calculation of the optical spectra of periodic structures presented. The optical response and infrared spectra published in the last 40 years for (In, Ga)N and (Al, Ga)As superlattices, with different number of unit cells n (varying from similar to 10 to similar to 400) and barrier and valley widths in the range of 2.5 nm to 40 nm, and different properties have been revisited. Among the various examples discussed here, we study the narrow peaks clustered in groups reported in high resolution spectra of blue-emitting devices, that could not be explained until now. These properties are faithfully reproduced and fully understood. We show that these effects are related to and depend on the surface energy levels and their tuneable detachment. We shown also that the optical transitions experimentally observed, but forbidden by the current optical physics, are really allowed transitions. Since the number of energy eigenvalues E-mu,v(r,v), and eigenfunctions Psi(r,v)(mu',v')(z ) is now much greater, the number of allowed matrix-elements can be extremely large (of the order of n(2) n(c)n(v)/2, with n, and n, the number of subbands in the conduction and valence bands). We show that this number can be reduced by using the eigenfunctions' symmetries, which are behind the parity symmetry selection rules and the leading order selection rules. These rules reduce the number of matrix-elements evaluations from similar to n(2) n(c)n(v)/2 to similar to nn(c)n(v)/2, i.e., depending on the superlattice, from about 1000 to 100. We discuss also a third rule, that collects the contributions of the surface and edge states, reducing the number of transitions even more to N-s = n(c)n(v). With these rules, the main peaks are conserved and their number practically matches that of the real spectrum. Excellent agreements