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Distributed Bragg reflector laser null for frequency modulation

机译:用于频率调制的分布式布拉格反射镜零位

摘要

PURPOSE: To select a Bragg wavelength longer than the characteristic wavelength of a gain medium by frequency modulating a distributed Bragg reflector laser having a feedback structure in frequency modulation transmitter for a light wave system. CONSTITUTION: A guide layer 26, an active layer 27, and a ptype four element cap layer 29 are formed sequentially on a substrate 23 and an isolation trench 32 is made in a part of a heterostructure for the purpose of electric isolation between a Bragg reflective region and a gain region. The feedback structure of the laser includes a corrugated lattice 31 formed in the guide layer 26. A lattice period effective on the guide region of the laser in the Bragg reflector region is determined according to formula I. In the formula I, Λeff is an effective period, λp is the substantial gain peak or the characteristic wavelength at maximum gain for the gain region of semiconductor structure, M is the order of the lattice of 1 or above, and n is the modal or effective refractive index for the waveguide mode of the semiconductor laser. According to the structure, the laser is controlled to emit a light wave signal having Bragg wavelength longer than the characteristic wavelength of the laser.
机译:目的:通过在光波系统的调频发射机中对具有反馈结构的分布式布拉格反射器激光器进行频率调制,以选择比增益介质的特征波长更长的布拉格波长。构成:在基板23上依次形成引导层26,有源层27和p型四元素覆盖层29,并在异质结构的一部分中形成隔离沟槽32,以实现布拉格反射之间的电隔离。区域和增益区域。激光器的反馈结构包括在引导层26中形成的波纹晶格31。根据公式I确定在布拉格反射器区域中的激光器的引导区域上有效的晶格周期。在公式I中,Λeff是有效的。周期,λp是半导体结构的增益区域的最大增益峰值或最大增益处的特征波长,M是1或更高晶格的量级,n是该波导模式的模态或有效折射率半导体激光器。根据该结构,控制激光器以发出布拉格波长长于激光器的特征波长的光波信号。

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