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The solution computed from the resulting two-dimensional dispersion-relation-preserving advection scheme can minimize the phase error.
The operation of arrays at millimetre and submillimetre wavelengths is very difficult and requires that the instrument be at very high and dry locations to minimize the phase distortions of signals as they propagate through the atmosphere.
The design of numerical methods for such general wave propagation problems is challenging because the energy conserving property has to be incorporated in the numerical algorithms in order to minimize the phase or shape errors after long time integration.
The former approach [18, 19] tries to minimize the error between the defocused halftone pattern and a sinusoidal fringe pattern while the latter approach [20] tries to minimize the phase error achieved with the defocused halftone patterns.
First, details of the binary tree-structured directional filter bank (DFB) are presented, including a modification to minimize the phase delay factor and necessary steps for handling rectangular images.
To minimize the phase distortions, this filter is implemented as a zero-phase forward and reverse digital filter [20].
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We appropriately formulate the design problem to obtain a simple linear optimization problem that minimizes the phase error of the 2-D recursive SHP DAF in the pth norm (Lp) sense.
The results illustrate that the AR model is successful in minimizing the phase error, but not the magnitude error.
We corrected the differential interferogram by minimizing the phase difference, Δφ, for the GCPs using equation (2): 00varphita varphi ={k}_0+{k}_1mathrm{R}mathrm{G}+{k }_2mathrm{A}mathrm{ Z(2).
By doing so and then by minimizing the phase difference for all depths between the two OCT signals of the two polarization channels, we could effectively align the spectrometers.
To minimize the intermediate phase, the first three layers are crystallized prior to the deposition of subsequent layers, and 340-nm-thick perovskite BST films have been fabricated at a process temperature of 625 °C.
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Since I tried Ludwig back in 2017, I have been constantly using it in both editing and translation. Ever since, I suggest it to my translators at ProSciEditing.

Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com