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Space/time/frequency methods in adaptive radar - New Jersey ...

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subspace is formed us<strong>in</strong>g the rema<strong>in</strong><strong>in</strong>g L r eigenvector. The two matrices areformed as follows:65The <strong>in</strong>terference eigenvalues are used to form an r x r matrix, Air , and the noiseeigenvalues are used to form an (L r) x (L — r) matrix, A ,as follows:Us<strong>in</strong>g Qr, Q A r , and 'A, the desired signal free R may be expressedEquation 3.8 is an estimate of the true covariance matrix R. For low rank<strong>in</strong>terference, R can be decomposed <strong>in</strong>to <strong>in</strong>terference and white noise contributionsas followswhere the diagonal of the r x r matrixconsists of the r pr<strong>in</strong>cipal (largest) eigenvalues of R, the columns of C2r are thecorrespond<strong>in</strong>g eigenvectors, o -2 is the variance of the white noise, and the columns ofare the rema<strong>in</strong><strong>in</strong>g eigenvectors of R. The actual value of r is scenario dependent,but it is upper bounded by r < v — 1, for equidistant sampl<strong>in</strong>g <strong>in</strong> space and<strong>time</strong> and for a perfectly calibrated array [17]. The spectral decomposition of R<strong>in</strong> Equation 3.16 suggests a decomposition for the estimate R similar to Equation3.15. The noise eigenvalues of the true covariance matrix <strong>in</strong> Equation 3.16 are allthe same and given by the noise power a. However, the noise eigenvalues obta<strong>in</strong>edby decompos<strong>in</strong>g the covariance matrix estimate R <strong>in</strong> Equation 3.15 are go<strong>in</strong>g to bespread over a range of power which depend<strong>in</strong>g on the sample support size used to

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