% setting up filter parameters and the svd of the input-to-state response thetamid=1.325; [A,B]=cjordan(5,0.88*exp(thetamid*1i)); % obtaining state statistics R=dlsim_complex(A,B,y'); sv=Rsigma(A,B,th); plot(th(:),sv(:));
Input-to-state filter and state covarianceThe first step to explain the high resolution spectral analysis tools is to consider the input-to-state
filter below and the corresponding
the state statistics.
The process
Then the filter transfer function is ![]() A positive semi-definite matrix ![]() for some row-vector ![]() the sample state covariance matrix. If the matrix ![]() the filter is a tapped delay line:
The corresponding state covariance The input-to-state filter works as a “magnifying glass” or, as type of bandpass filter, amplifying the harmonics in a particular frequency interval.
Shaping of the filter is accomplished via selection of the eigenvalues of ![]() The routine dlsim_complex.m generate the state covariance matrix (dlsim_real.m for
real valued problem).
The following figure plots % setting up filter parameters and the svd of the input-to-state response thetamid=1.325; [A,B]=cjordan(5,0.88*exp(thetamid*1i)); % obtaining state statistics R=dlsim_complex(A,B,y'); sv=Rsigma(A,B,th); plot(th(:),sv(:));
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