The nonlinear optical properties of MQW structures with binary (ZnSe/ZnMnSe) and ternary (ZnCdSe/ZnSe) wells grown by MBE are compared. Pump-probe experiments and high-excitation PL measurements are carried out to study the excitonic nonlinearity as well as gain processes. It is found that the nonlinear optical response is qualitatively different in these two structures as a result of the different kinds of disorder present in the QWs.
General Sample PropertiesZnSe-based quantum structures are promising candidates for photonic devices operating in the blue-green spectral range. However, a debate is currently running about the physical processes giving rise to lasing and optical nonlinearity. This paper compares the nonlinear optical properties of multiple quantum well (MQW) structures with binary (ZnSe/ZnMnSe) and ternary (ZnCdSe/ZnSe) wells. The MQW structures, grown on (001) GaAs by MBE, are of excellent quality and exhibit distinct and sharp excitonic features. They are of type I and both electrons and holes are well confined to the QWs. For transmission experiments the GaAs substrate and the ZnSe buffer layer were removed using a selective wet etching technique. The etched samples are fixed on a glass plate by adhesion.The binary ZnSe-QW of the Mn structures is under tensile in-plane strain so that the band edge is shifted to lower energies and the light-hole exciton (&h) is the ground state. Conversely, compressive strain arises in the ternary wells of the Cd structures and the heavy-hole exciton (Xhh) is the lowest electronic excitation. Furthermore, alloy fluctuations occur here in the QW and are thus expected to have a larger influence on the linear as well as nonlinear optical response than for the Mn structures. The samples of the present study were designed to contain five wells of a width that is close to the ZnSe bulk exciton radius of 4.5 nm.
Pump-Probe ExperimentsThe excitonic nonlinearities are studied by pump-probe experiments using amplified tunable sub-ps-pulses. The third harmonic of a mode-locked Nd-YLF laser is used as the pump source for a synchronously pumped dye laser containing a saturable absorber for pulse shortening. Output pulses with a typical width of 0.8 ps and a repetition rate of 76 MHz are generated. Pulse selection and amplification is achieved by a four-stage excimer pumped dye amplifier. The amplifier output is used to excite the sample as well as to generate a ')