Theory of coherent optical nonlinearities of intersubband transitions in semiconductor quantum wells

We theoretically study the coherent nonlinear response of electrons confined in semiconductor quantum wells under the effect of an electromagnetic radiation close to resonance with an intersubband transition. Our approach is based on the time-dependent Schrodinger-Poisson equation stemming from a Hartree description of Coulomb-interacting electrons. This equation is solved by standard numerical tools and the results are interpreted in terms of approximated analytical formulas. For growing intensity, we observe a redshift of the effective resonance frequency due to the reduction of the electric dipole moment and the corresponding suppression of the depolarization shift. The competition between coherent nonlinearities and incoherent saturation effects is discussed. The strength of the resulting optical nonlinearity is estimated across different frequency ranges from mid-IR to THz with an eye to ongoing experiments on Bose-Einstein condensation of intersubband polaritons and to the speculative exploration of quantum optical phenomena such as single-photon emission in the mid-IR and THz windows.

Automated summary

The coherent nonlinear response of electrons in semiconductor quantum wells to resonant electromagnetic radiation is theoretically studied. The study is based on the time-dependent Schrodinger-Poisson equation and the results are interpreted with approximated analytical formulas. The redshift of the resonance frequency and the competition between coherent nonlinearities and incoherent saturation effects are observed and discussed. The optical nonlinearity is estimated across different frequency ranges, which is important for ongoing experiments and the exploration of quantum optical phenomena.