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Electro-optical method for polarimetric measurement

机译:电光法进行极化测量

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When passing a pulsing beam of polarize light of a light emitter diode (LED) or a semiconductor laser thru an optical system and two photodiodes spatially arranged at 90° to each other and both with their detection surfaces parallel to the transmission shaft of light, and polarization axis oriented at 45° of the vertices of the edges where the photodiodes join, in the outputs of two operational amplifiers, e have two signals with the same shape in time, i.e. a pulse train with the same phase, but when you turn the polarization plane, change the radiance of the light projected onto the photodiodes, being out of phase signals to the outputs of the amplifiers, where the difference between the fronts of the pulses is proportional to the angle of rotation of the plane of polarization of polarization light. In a digital circuit phase discriminator, a puls e is obtained equal to the time difference between two sides of the rise time in the output of two amplifiers. The width of this is directly proportional to the value of rotation the plane of polarization of light, that is, the greater the rotation, the greater the width of this.
机译:当通过光学系统和半导体激光器的脉冲光束通过光学系统和两个光电二极管彼此以90°设置在90°时,并且与它们的检测表面平行于光,并且在两个运算放大器的输出中,在两个运算放大器的输出中,偏振轴以45°定向,在两个运算放大器的输出中,E具有相同形状的两个信号,即具有相同阶段的脉冲序列,但是当你转动时偏振平面,将突出到光电二极管上的光的辐射改变为放大器的输出的相位信号,其中脉冲前部之间的差与偏振光偏振平面的旋转角度成比例。在数字电路相位鉴别器中,获得脉冲E等于两个放大器的输出中的上升时间的两侧之间的时间差。这的宽度与旋转值的旋转值直接成比例,即光的偏振平面,即旋转越大,宽度越大。

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