光脉冲通过法布里-珀罗干涉仪的传输

A. Kastler
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引用次数: 37

摘要

在第一部分中,作者回顾了法布里·珀罗干涉仪的经典理论,该理论适用于干涉仪被长持续时间的相干振动光束照射的情况。在第二部分,他研究了方形脉冲如何通过法布里·珀罗干涉仪传输。定义了表征该仪器的两个持续时间参数τ和τ'。τ表示在两个板之间向前和向后运动的光路的持续时间,τ'表征由于连续多次反射引起的光束指数衰减的持续时间。在脉冲持续时间Θ0 > τ的情况下,涌现振动逐渐叠加,并计算输出脉冲强度作为时间函数的分布。当Θ0 < τ时,连续分离的脉冲不重叠。本文讨论了探测器接收到的信号的傅里叶分析。在第三部分中,表明了信号频谱与法布里·佩罗号的光谱之间的类比。在第四部分中,已经确定了在时域中接受光脉冲的佩罗反射的光的轮廓,在第五部分中已经确定了存储在法布里·佩罗中的光能的平衡。
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Transmission of light pulse through a Fabry-Perot interferometer
In the first part the author reviews the classical theory of the Fabry Perot interferometer that is applicable when the interferometer is illuminated by a light beam of coherent vibrations having long duration. In the second part, he studies how a pulse of square form is transmitted through a Fabry Perot interferometer. The two parameters of duration τ and τ' that characterize the instrument were defined. τ represents the duration of light path for a forward and backward motion between the two plates and τ' characterises the duration of the exponential attenuation of the beam due to the successive multiple reflections it suffers. In the case of the pulse having duration Θ0 > τ the emergent vibrations superpose progressively and the profile of intensity of the output pulse as a function of time is calculated. In case when Θ0 < τ the successive separated pulses do not overlap. The Fourier analysis of the signal received by a detector has been discussed in this case. In part III, the analogy between the spectrum of the signal and the optical spectrum of the Fabry Perot has been shown. In part IV, the profile of the light reflected by the Febry Perot receiving a light pulse, in the time domain, has been established and in part V the balance of light energy stored in the Fabry Perot has been established.
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