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This paper presents 2 cyclostationarity detectors targeting different scenarios.
Hence, for detector-target separations above 9 mm an ability to localize the target in the angular domain is lost.
Instead, spectro-angular plots demonstrated quasi-continuous spectral bands as can be seen in Fig. 4 d) that displays the contour plot corresponding to a final 25-mm detector-target separation.
To go beyond a simple conceptual picture explaining the spectral shape of the RER in section 3.1, we calculated ln(1/RER) for various detector-target separations for 0° (Fig. 6, lines, left axis).
Following Eq. (1) and using experimental data for the RER and μeff from Fig. (6), we calculated values of K for selected wavelengths at various detector-target separations (Fig. 7(a) ).
The contour plot in Fig. 5(a) demonstrates the variations of the RER with changing the detector-target separation from 5 to 25 mm for all measured wavelengths along the actual direction of the void region (i.e., 10°) for 34 mm source-detector separation.
In this paper, the problem of enhancing the detection performance of detector for target in partially homogeneous background is addressed.
This paper introduces a new coherent detector for target detection in the clutter model of interest, which has explicit dependence on the clutter parameters.
As minimizing the PEPs can improve the BER performance of the VBLAST detector, our target is to design a unimodular matrix such that the PEPs will be minimized.
Fig. 8 Performance comparison of three detectors for target 1 and target 2. a target 1; b target 2.
The current status of these and other detector developments targeted at synchrotron science are briefly reviewed.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com