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The quantum well self-electrooptic effect device: Optoelectronic bistability and oscillation, and self-linearized modulation
548
Citations
17
References
1985
Year
Quantum PhotonicsEngineeringOptoelectronic DevicesSelf-electrooptic Effect DeviceElectronic DevicesSelf-linearized ModulationOptical SwitchingPhotonicsQuantum ScienceElectrical EngineeringPhysicsQuantum DeviceOptoelectronic BistabilityElectro-optics DeviceApplied PhysicsNegative Resistance Self-oscillationQuantum DevicesElectrical BistabilityElectronic Self-oscillationQuantum Photonic DeviceOptoelectronicsOptical Devices
We report extended experimental and theoretical results for the quantum well self-electrooptic effect devices. Four modes of operation are demonstrated: 1) optical bistability, 2) electrical bistability, 3) simultaneous optical and electronic self-oscillation, and 4) self-linearized modulation and optical level shifting. All of these can be observed at room-temperature with a CW laser diode as the light source. Bistability can be observed with 18 nW of incident power, or with 30 ns switching time at 1.6 mW with a reciprocal relation between switching power and speed. We also now report bistability with low electrical bias voltages (e.g., 2 V) using a constant current load. Negative resistance self-oscillation is observed with an inductive load; this imposes a self-modulation on the transmitted optical beam. With current bias, self-linearized modulation is obtained, with absorbed optical power linearly proportional to current. This is extended to demonstrate light-by-light modulation and incoherent-to-incoherent conversion using a separate photodiode. The nature of the optoelectronic feedback underlying the operation of the devices is discussed, and the physical mechanisms which give rise to the very low optical switching energy (∼4 fJ/ μm <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sup> ) are discussed.
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