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Near–Far Resistance to NBI

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Near–Far Resistance to NBI

We first consider the situation in which there is NBI but no MAI. Let the NBI signal i be an arbitrary discrete-time wide-sense stationary process, with autocorrelation matrix Ri, which is nonnegative definite. Suppose that the spectral decomposition of Ri is given by

Equation 7.132

graphics/07equ132.gif


where l1,...,lN and u1,...,uN are the nonnegative eigenvalues and the corresponding orthogonal eigenvectors of Ri. Since

Equation 7.133

graphics/07equ133.gif


using (7.77) we obtain

Equation 7.134

graphics/07equ134.gif


When the NBI signal power is increased, the nonzero ll's increase proportionally. Therefore, it is seen from (7.134) that the near–far resistance to NBI is nonzero if and only if Ri has at least one zero eigenvalue and the corresponding eigenvector is not orthogonal to s. On the other hand, if Ri has full rank, the near–far resistance to NBI is zero.


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