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The angular dependence of the reflectance and differential phases induced by reflection and transmission were presented.
The differential phases of target N, M, F are shown in Table 2, from which we can see that the differential phases are very close to the ideal differential phases calculated by − 2 π λ R bic 0 ; r − R bic new 0 ; r, where Rbicnew means the range corresponding to the second receiver.
The differences between the simulated and the target reflectance of 50% are less than 2% and differential phases are less than 5°in the range 1300 1320 nm and 1540 1550 nm for both p- and s-components.
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The attenuation projection is differentiated to bring it into a modality comparable to the differential phase projection using a Gaussian derivative filter.
The attenuation projection was differentiated to bring it into a comparable modality to the differential phase projection using a Gaussian-windowed derivative filter based on the Fourier derivative theorem.
differential phase experiment.
differential phase shift keying.
One application of this fiber is in the demodulation of differential phase shift keying (DPSK) signals.
The differential phase difference in step 2 presents a notch area in the low-frequency part.
Intermediate results were checked by the laser differential phase profilometer [10] and scanning electron microscope.
Step 3 selects the low-frequency part by searching the notch area of differential phase difference.
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