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Solid State Communications

Polarization-dependent coherent nonlinear optical response in GaAs quantum wells: Dominant effects of two-photon coherence between ground and biexciton states

Hailin Wang, Jagdeep Shah, Theo C. Damen, Loren N. Pfeiffer

Published Sep 1, 1994• 114 citations
Publisher
DOI
10.1016/0038-1098(94)90004-3

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We present in this paper polarization dependent four-wave-mixing (FWM) measurements in homogeneously broadened GaAs quantum wells (QW). We have unambiguously demonstrated the important contribution of the two-photon coherence (TPC) between the ground and biexciton states to the nonlinear response. We show for the first time the dominant effects of the TPC on the polarization dependence of FWM. In particular, by including the TPC-induced contribution, we are able to account for the anomalous polarization dependence, a subject of considerable current interest [1].
The coherent response of excitons in semiconductor nanostructures measured in four-wave mixing (FWM) depends strongly on the inhomogeneous broadening of the exciton transition. We investigate GaAs/Al0.3Ga0.7As single quantum wells (SQW) and AlxGa1-xAs mixed crystals. Additional to the usual phase-space filling nonlinearity, excitation-induced dephasing (EID) and biexciton formation (BIF) are important. EID leads to a strong dependence of the signal on the angle between the linear input polarizations. We find that EID persists in inhomogeneous systems, showing that the mutual density-dependent dephasing rate difference between two subsystems within the inhomogeneous distribution is strongly dependent on their energy difference. BIF is strongly affecting the cross-linear polarized FWM response. The signal for positive delay is dominated by the transitions from the one-exciton state X to the two-exciton states. Here, the third-order polarization at X-XX is not at the same resonance as the first-order polarization at 0-X. Consequently, the rephasing of the microscopic third-order polarization to the macroscopic FWM photon echo is blurred by the non-perfect correlation of X and XX energies, leading to a fast and non-exponential signal decay in delay time. For inhomogeneous broadenings larger than the biexciton binding energy, we find an enhanced biexciton binding energy, and a quenching of the oscillator strength of the unbound biexciton.