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optoelectronic materials

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Quantum-Confined Optoelectronics

1964 - 1993

The period 1964–1993 witnesses the maturation of quantum-confined nanostructures and impurity-engineered infrared photonics, yielding size-tunable absorption and emission in quantum dots and quantum wells, along with ultrafast nonlinear optical responses and room-temperature excitonic effects in semiconductor-doped glasses and MQWs. Purposive defect control and processing techniques reconfigure optical band gaps across a broad materials set, including amorphous silicon and oxide films, while Er3+-activated and impurity-enabled infrared sources underscore silicon compatibility as a route toward integrated photonics. Infrared detectors, intersubband transitions in quantum wells, and superlattice architectures illustrate enhanced spectral response, foreshadowing later infrared and silicon-photonic developments.

Ultrafast nonlinear optical responses and transient gratings are studied across semiconductor-doped glasses and quantum-confined structures, revealing femtosecond bleaching, picosecond relaxation, and room-temperature excitonic nonlinearities in CdSSe glasses, CdS nanocrystals, CdSe QDs, and GaAs/GaAlAs MQWs [1], [4], [15], [6], [17], [18], [11].

Telecom-band (1.54 μm) luminescence and electroluminescence arise from Er3+ implanted/doped semiconductors, with oxygen impurities enabling optical activation in silicon, highlighting impurity engineering as a route to infrared light sources [2], [3], [8].

Infrared photodetectors and IR-active architectures use quantum wells, superlattices, and intersubband transitions to achieve enhanced detection and spectral response, as demonstrated in GaAs QWIPs, GaAs/AlGaAs superlattices, and SiGe/Si MQWs [9], [14], [13].

Quantum confinement in CdS/CdSe nanostructures and nanoporous silicon yields size-tunable absorption and emission, with ultrafast phenomena and nonlinearities [7], [16], [17], [6].

Processing, impurities, and defect engineering modulate optical/electronic properties across diverse materials—from amorphous Si and ITO to oxide films—reconfiguring conductivity, band gaps, and luminescence via light or heat treatments [20], [19], [10].

Interface-Engineered Nanoscale Emitters

1994 - 2000

Phosphorescent Triplet Harvesting OLEDs

2001 - 2007

Confinement-Driven Optoelectronics

2008 - 2010

Hybrid Perovskite-2D Optoelectronics

2011 - 2017

Convergent 2D-Perovskite Optoelectronics

2018 - 2024