Phototransistor with quantum well base structure
AssigneeAT&T Corp.
InventorNaresh Chand
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Abstract
A long wavelength (6 to 20 .mu.m) phototransistor is described which has n-doped silicon as emitter and collector regions bracketing a base region having a quantum well structure made up of alternating layers of p-doped silicon germanium and undoped silicon, The silicon germanium layer adjacent to the emitter region is thicker and has a higher percentage of germanium in order to provide a quantum well that is wider and deeper than the other quantum wells in the base region thereby resulting in a larger current and optical gain. The silicon barrier layer of the quantum well closest to the collector region is p-doped in order to reduce the leakage current of the base-collector junction.
Claims7
A phototransistor comprising emitter, base, collector regions, said emitter and collector regions being doped such that they are of the same conductivity type, said base region being doped such that it is the opposite conductivity type, and means for conductively coupling to said emitter and collector regions such that an output signal can be developed in response to an external light beam impinging on said phototransistor, characterized in that said base region comprises multiple layers of semiconductor material in a quantum well structure, the material in each layer being chosen such that the bandgap between its valance and conduction bands is different from the bandgap in adjacent layers and such that there is no substantial discontinuity in the conduction band between adjacent layers and the difference in bandgap between adjacent layers primarily causes discontinuities in the valance bands, whereby the quantum wells are primarily in the valance band.
A photodetector for developing an output signal in response to an external light beam, said photodetector comprising multiple layers of semiconductor material arranged to form a quantum well structure having a first layer and a last layer, the material of said multiple layers being chosen such that each layer has a bandgap between its valance and conduction bands different from the bandgap of adjacent layers thereby forming quantum wells in alternate layers with barrier layers between, said barrier layers being undoped and the alternate layers having the quantum wells being doped such that they are all of a first conductivity type, first means for conductively coupling to said first layer, and a second means for conductively coupling to said last layer, said output signal appearing between said first and second coupling means when said light beam impinges on said multiple layers, characterized in that said first and second coupling means includes semiconductor material having a dopant such that they are both of a conductivity type opposite to said first conductivity type, and said last layer of said quantum well structure is a layer having a quantum well, said last layer being thicker and having a smaller bandgap than the other layers having quantum wells.
Dependencies are inferred from the claim text.