1999
DOI: 10.1016/s0143-8166(00)00005-1
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Correction and correlation formation of probing field in fiber laser Doppler anemometers and vibrometers

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“…{P(x2,y2).Af(x2,y2)}* -{s} (2) Applying the convolution theorem, the field distribution in the back focal plane of correlator can be represented by relation: W(x3 ,y3) z{u} = QM* p M ® S where * and 0 are correlation and convolution operators respectively. The exact form of amplitude distribution of output field of such two-stage correlator has been derived in [5] for the case of periodical phase distribution of wave Q.…”
Section: The Theoretical Background Of the Methodsmentioning
confidence: 99%
“…{P(x2,y2).Af(x2,y2)}* -{s} (2) Applying the convolution theorem, the field distribution in the back focal plane of correlator can be represented by relation: W(x3 ,y3) z{u} = QM* p M ® S where * and 0 are correlation and convolution operators respectively. The exact form of amplitude distribution of output field of such two-stage correlator has been derived in [5] for the case of periodical phase distribution of wave Q.…”
Section: The Theoretical Background Of the Methodsmentioning
confidence: 99%