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In this method, the phase information has been not considered.
In this method, the phase change interface was determined based on the liquid fraction approach.
Using the two-station method, the phase velocity between A and B′ is measured under the condition that the wave front propagates as a plane wave.
In this method, the phase differences of individual subcarriers are weighted averaged with weights proportional to the squared channel gains in the respective frequencies.
In the proposed method, the phase of the PN sequences at each antenna is rotated differently and transmitted to prevent a PN sequence-canceling problem.
Further, by using our method the phase knowledge of response signals was well preserved in the reconstructed data and hence a more accurate estimate was obtained.
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The proposed PCAI8 method, the PCAI4 method, and the phase SPN method can achieve a 100% TPR at a low FPR on an image block of 512 × 512 pixels in our experimental environment.
With the central finite differences method, the phase-field does not match with its rotation and the solution is not any more isotropic.
In the proposed method, the phases of the PN sequences at each antenna are rotated differently and transmitted to prevent the PN sequence canceling problem.
In all methods, the phase shift patterns are optimized to match their Fourier transforms to a target reflection spectrum.
To conclude, it is interesting to note that for these three methods, the phase information is absent as in the case of the classical denoising approach.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com