Abstract
For a proper understanding of nonlinear optical experiments in semiconductors even the low-density limit Coulomb-induced manybody correlations beyond the Hartree-Eock decoupling scheme need to be considered. In the coherent χ(3) limit these correlations manifest themselves in the contributions of bound and unbound two-exciton states to the optical response.1–4 The understanding of nonlinear excitonic effects in the Stark effect of semiconductors including carrier-correlations is still of fundamental interest.
© 1999 Optical Society of America
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