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Active modulation of quantum well lasers by energy shifts in gain spectra with applied electric field

机译:通过施加电场的增益谱中的能量位移对量子阱激光器进行主动调制

摘要

Modulation of a semiconductor laser device is achieved at microwave frequencies by the application of transverse fields which produce energy shifts in the gain spectra of the laser device. The laser device is a PN diode which has a body portion constructed from a nonconductive material, with P and N type implants on opposite sides. The P and N implants define a transition region, or layer, on the order of 1 micron in width, in which is formed a quantum well having a thickness on the order of 50 to 100 Angstroms. Application of a bias voltage across the PN junction provides lasing of the device. An electrode on the surface of the transition layer allows application of a transverse electric field to the PN junction. This transverse field quenches the lasing of the device, to provide modulation of the laser. Quenching is produced by means of energy shifts in the gain spectra of the laser device, and since current flow through the PN junction is inhibited by the nonconductive material and thus flows primarily in the quantum wells, modulation of the current is possible at microwave frequencies at relatively low power levels.
机译:通过施加横向场在微波频率上实现半导体激光器装置的调制,该横向场在激光器装置的增益谱中产生能量偏移。激光设备是一个PN二极管,它的主体部分是由非导电材料制成的,在相对的一侧上有P型和N型注入。 P和N注入物限定了约1微米宽的过渡区或过渡层,在其中形成了厚度约50至100埃的量子阱。在PN结两端施加偏置电压会产生激光发射。过渡层表面上的电极允许向PN结施加横向电场。该横向场抑制了设备的发射,以提供对激光器的调制。淬火是通过激光器件增益谱中的能量偏移产生的,并且由于流经PN结的电流被非导电材料抑制,因此主要流向量子阱,因此在微波频率为190时调制电流是可能的。相对较低的功率水平。

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