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Summary and future works

A periodic AlGaInAs QW/barrier structure grown on a Fe-doped substrate was used to not only be a saturable absorber for the 1064nm and 1342nm passively Q-switched and mode-locked lasers but also to be a gain medium for the 1360nm and 1570nm optically-pumped semiconductor lasers.

In passively Q-switched lasers, we have demonstrated that the AlGaInAs QWs based SESA is promising candidate to develop high-performance Nd-doped passively Q-switched laser. Compared with InGaAsP, AlGaInAs have larger conduction band offset which can reduce carrier leakage and get higher temperature stability. And the barrier layers play a role not only to confine the carriers but also to locate the QW groups in the region of the nodes of the lasing standing wave to avoid damage.

Therefore, in 1.06µm PQS laser , stable Q-switched pulses of 0.9 ns duration with an average output power of 3.5 W and a repetition rate of 110 kHz were obtained at an incident pump power of 13.5 W. The remarkable performance confirms the prospect of using AlGaInAs QWs as saturable absorbers in solid-state lasers.

In passively mode-locked lasers, we have designed AlGaInAs QWs grown on the Fe-doped InP substrate to be a saturable absorber for self-starting continuous-mode-locked Nd:YVO4 laser at 1342 nm. Stable mode-locked pulses of 26.4 ps duration with a repetition rate of 152 MHz were generated within the range of incident pump power from 4.5 W to 12.3 W. The average output power for the cw mode-locked operation was 1.05 W at an incident pump power of 12.3 W.

In optically-pumped semiconductor lasers, we have demonstrated the periodic AlGaInAs QW/barrier structure grown on an Fe-doped InP transparent substrate was

developed to be a gain medium in a room-temperature high-peak-power nanosecond laser at 1.36µm and 1.57µm. The quantum wells are separated by half-wavelength thick AlGaInAs barriers and designed to be located at the antinodes of the intra-cavity standing wave field to enhance the interaction between a standing wave optical field and an active medium. The maximum peak power was achieved 1.2kW and 290 W at 1.36µm and 1.57µm, respectively. For power scaling up, we also have demonstrated an optically pumped high-peak-power AlGaInAs/InP eye-safe laser by in-well pumping scheme. The conversion efficiency is enhanced over three times compared with barrier pumping scheme. Double gain chips were used to increase the absorption efficiency of pump laser and maximum output power and peak power was up to 300mW and 0.52kW. For optically-pumped semiconductor lasers, the performance of AlGaInAs quantum wells grown on InP substrate without DBR has been studied through many ways. We tried to analysis the effect of temperature, pumping spot size, different actively Q-switched frequency (or different duty cycle), different cavity setup (cavity length, output coupler) and improved the performance of AlGaInAs quantum well laser in the room-temperature.

In the future, we will try to deal with the thermal problems of optically-pumped semiconductor laser such that the OPSLs can be operated in the cw-mode. The ways to deal with the heat of OPSLs are substrate removal and bonding a heat-spreader to the semiconductor gain chip. Furthermore, we will also try to develop the 1.2µm and 660 nm (red) optically-pumped semiconductor laser.

In addition to be the saturable absorber and gain medium, many physical phenomena can be observed in semiconductor. Some topics like Rabi oscillation, slow light, PL spectrum, and exciton-polariton in semiconductor microcavity are interesting and important to understand the dynamic of the carrier in the semiconductor.

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