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Applied Physics Letters

Microscopic carrier dynamics of quantum-well-based light storage cells

S. K. Zhang, Paulo Ventura Santos, R. Hey, Alberto García-Cristóbal, A. Cantarero

Published Dec 25, 2000• 9 citations
Publisher

Abstract

The dynamics of storage and recombination of electron–hole pairs in quantum-well-based light memory cells driven by high-frequency electric fields is investigated by spatially and time-resolved photoluminescence spectroscopy. In these cells, a laterally modulated potential is used to ionize and spatially separate photogenerated electron–hole pairs. The temporal and spatial dependence of the carrier dynamics depends not only on the modulated potential, but also on the transport properties of electrons and holes.

DOI
10.1063/1.1336160

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The dynamics of storage and recombination of electron–hole pairs in quantum-well-based light memory cells driven by high-frequency electric fields is investigated by spatially and time-resolved photoluminescence spectroscopy. In these cells, a laterally modulated potential is used to ionize and spatially separate photogenerated electron–hole pairs. The temporal and spatial dependence of the carrier dynamics depends not only on the modulated potential, but also on the transport properties of electrons and holes.
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Photonic signals were efficiently stored in a semiconductor-based memory cell. The incident photons were converted to electron-hole pairs that were locally stored in a quantum well that was laterally modulated by a field-effect tunable electrostatic superlattice. At large superlattice potential amplitudes, these pairs were stored for a time that was at least five orders of magnitude longer than their natural lifetime. At an arbitrarily chosen time, they were released in a short and intense flash of incoherent light, which was triggered by flattening the superlattice amplitude.
Indirect excitons in GaAs coupled quantum well nanostructures are a versatile system for fundamental study of cold neutral bosonic gases and demonstration of novel optoelectronic devices based on excitons -- a bound electron-hole pair -- rather than electrons. Indirect exciton lifetimes range from nanoseconds to microseconds and cool rapidly after photoexcitation to the lattice temperature. Lithographically-patterned electrodes enable design of potential energy landscapes, and both energy and lifetime can be controlled in situ, rapidly, on timescales much shorter than the exciton lifetime. Such intrinsically optoelectronic devices can operate at speeds relevant to optical networks, and later be fabricated in other semiconductors for higher-temperature operation. Two different kinds of devices are demonstrated Photon storage -- an optical memory -- with 250 ps rise time of the readout optical signal and storage time reaching microseconds was implemented with indirect excitons in CQW. The storage and release of photons was controlled by the gate voltage pulse, and the transient processes in the CQW studied by measuring the kinetics of the exciton emission spectra. This control of excitons on timescales much shorter than the exciton lifetime demonstrates the feasibility of studying excitons in in situ controlled electrostatic traps. The Exciton Conveyer is a laterally moving electrostatic lattice potential for actively transporting excitons. Generated by laterally modulated electrodes, the potential velocity and depth are controlled in situ by frequency and voltage. We observed exciton transport characterized by average exciton cloud spatial extension over several tens of microns, and observed dynamical localization-delocalization transitions for the excitons in the conveyer : In the localization regime of deeper potentials and moderate exciton density, excitons are moved by the conveyer; in the delocalized regime of shallower lattice potential or high exciton density, excitons do not follow the conveyer motion. We explore conveyer velocities both slower and faster than phonon velocities. Realizing subnanosecond manipulations of exciton energy and lifetime required versatile control of pulsed and multiple AC RF electrical signals in optical, liquid helium cryogenic systems. Considerable detail is presented of design, construction, and test of flexible experimental apparatus
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