1985
DOI: 10.1016/0378-4363(85)90378-x
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Recombination of carriers confined at In0.53Ga0.47As/InP and In0.75Ga0.25As0.5P0.5/InP interfaces

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Cited by 6 publications
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“…As illustrated in Figure 4c, due to the different electron affinity energy and bandgap of InGaAs and InP, the band bending occurs near the heterointerface, forming the triangular potential well and barrier. [33][34][35] When laser pumping is applied, the photogenerated electrons are directly bound in the triangular potential well at the InGaAs/n-InP interface, forming 2D electron gas (2DEG). Holes also approach the strongly negatively charged interface and can be bound close to it via Coulomb interaction.…”
Section: Pl Mechanismmentioning
confidence: 99%
“…As illustrated in Figure 4c, due to the different electron affinity energy and bandgap of InGaAs and InP, the band bending occurs near the heterointerface, forming the triangular potential well and barrier. [33][34][35] When laser pumping is applied, the photogenerated electrons are directly bound in the triangular potential well at the InGaAs/n-InP interface, forming 2D electron gas (2DEG). Holes also approach the strongly negatively charged interface and can be bound close to it via Coulomb interaction.…”
Section: Pl Mechanismmentioning
confidence: 99%