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Two separate circular interference fringe systems were formed due to the two solutions and they were recorded on a PC using a CCD camera.
Fig. 6 Circular interference model from [152].
The Newton's ring experimental setup for recording circular interference fringes is shown in Fig. 7.
The circular interference model in [152] enables to map arbitrary node locations onto circles with equivalently spaced nodes.
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Since for circular cylinders interference effects caused by vortex shedding are pronounced, the present work tries to clarify to which extent turbulence effects are reducing the interference in this case.
In order to beat the multipath interference circular polarization was employed.
We assume that BSs have circular transmission and interference regions, where the radius of the transmission region of each BS is denoted by RBS, and the radius of the interference region of each BS is denoted by Rint.
However, these receivers assume implicitly or explicitly circular (or proper) interferences and become suboptimal for noncircular (or improper) interferences.
In addition, with the circular polarization self-interference suppression higher than 70 dB was achieved independently of the environment.
A quarter-wave plate (QWP) before the camera converts the two polarized beams to right- and left-handed circular polarization to produce interference fringes at the pixelated phase mask.
Interference of two circular waves - Wavelength (decreasing bottom to top) and Wave centers distance (increasing to the right).
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