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convolution (denoted by *) of the optical pulse shape, the reflective impulse response of the fiber, and the impulse response of the receiver: y(t) = p(t) * f(t) * r(t) where y(t) is the receiver output p(t) is the optical pulse shape f(t) is the impulse response of the fiber on reflection r(t) is the receiver impulse response By properly shaping the optical pulse and then correlating the receiver output with the known optical pulse shape, we can enjoy the noise advantages of a wide, energetic pulse and still obtain the high resolution of a narrow pulse. The result of the correlation (denoted by ) is p(t) y(t) = [p(t) p(t)] * f(t) * r(t) where y(t) is the receiver output p(t) is the optical pulse shape f(t) is the impulse response of the fiber on reflection r(t) is the receiver impulse response When the autocorrelation of the optical pulse approximates a delta function, we obtain the same measurement as if we had used a narrow optical pulse (Nazarathy et al., 1989). The best solution applicable within the constraints of reflectometry calls for using a family of four pulse shapes. The envelope of each pulse is a binary code designed so that the sum of the autocorrelations of the four pulses is a delta function. To obtain a reflectometer trace, reflections are measured in response to each of the four coded pulses. Each reflection is correlated with the corresponding code, and the four resulting correlations are added together to obtain the reflected signal versus time or distance. The correlation technique allows a given noise level to be achieved with fewer measured pulses, hence more quickly, than without correlation.
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