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Extra resources for Radar Target Imaging

Example text

16 represents an optimum receiver for polarization-based disturbance cancellation: it implements the above-described optimum procedure. In such a scheme, CHS means change sign, alb means division, and the double frame box is used to indicate an operation giving rise to a complex output. Some suboptimum procedures. 23]. It can be verified that their performances are characterized by a limited loss of cancellation ratio with respect to the optimum procedure, when the hypotheses made for this technique still hold.

1,4J, and is then seen to represent the reflected wave of Fig. 1; this calculation is not explicitly presented here. 5,6J as a tool for analyzing radar scattering phenomena in real time and in frequency space. 14a) , a=1 with complex amplitudes Ra and exponents Sa. 14b) , Sa where S = jw, and Wa = 1m Sa are the natural frequencies (eigenfrequencies) of the target. 14c) where r", = - 2 Resa is the full width at half maximum of the ath resonance. 14d) 52 H. Uberall The Laplace transform of the scattering amplitude thus has poles in the complex s plane (located in the second quadrant); equivalently, the Fourier transform has poles in the complex frequency (m) plane, located in the first quadrant.

Poelman: "On using orthogonally polarized noncoherent receiving channels to detect target echoes in Gaussian noise," IEEE Trans. c. Vannicola, S. Lis: "Polarization vector signal processing for Radar clutter suppression," in Inverse Methods in Electromagnetic Imaging, Part II, ed. M. Boerner et a!. (D. , Hingham, MA 1985) pp. L. Van Trees: Detection, Estimation and Modulation Theory, Part III (Wiley, New York, 1971) M. Born, E. R. Huynen, "Phenomenological theory of radar targets," in Electromagnetic Scattering, ed.

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