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首页> 外文期刊>Advances in OptoElectronics >Room Temperature Direct Band Gap Emission from Ge p-i-n Heterojunction Photodiodes
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Room Temperature Direct Band Gap Emission from Ge p-i-n Heterojunction Photodiodes

机译:Ge p-i-n异质结光电二极管的室温直接带隙发射

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Room temperature direct band gap emission is observed for Si-substrate-based Ge p-i-n heterojunction photodiode structures operated under forward bias. Comparisons of electroluminescence with photoluminescence spectra allow separating emission from intrinsic Ge (0.8 eV) and highly doped Ge (0.73 eV). Electroluminescence stems from carrier injection into the intrinsic layer, whereas photoluminescence originates from the highly n-doped top layer because the exciting visible laser wavelength is strongly absorbed in Ge. High doping levels led to an apparent band gap narrowing from carrier-impurity interaction. The emission shifts to higher wavelengths with increasing current level which is explained by device heating. The heterostructure layer sequence and the light emitting device are similar to earlier presented photodetectors. This is an important aspect for monolithic integration of silicon microelectronics and silicon photonics.
机译:对于在正向偏压下运行的基于硅衬底的Ge p-i-n异质结光电二极管结构,观察到了室温直接带隙发射。将电致发光与光致发光光谱进行比较,可以将发射从本征Ge(0.8 eV)和高掺杂Ge(0.73 eV)中分离出来。电致发光源于向本征层中注入载流子,而光致发光源于高度n掺杂的顶层,因为激发的可见激光波长被Ge强烈吸收。高掺杂水平导致明显的带隙因载流子-杂质相互作用而变窄。随着电流水平的增加,发射会转移到更高的波长,这可以通过器件加热来解释。异质结构层序列和发光器件类似于较早提出的光电探测器。这是硅微电子和硅光子的单片集成的重要方面。

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