An apparent weakness in the arguments within the derivation of [1, Appendix] is identified using explicit numerical examples which further demonstrate that the results are of limited benefit. Our prior experience in specifying linear system realizations [2], [3] alerted us to an apparent problem with the new alternative procedure offered in [1, Appendix], as a potentially more straightforward way to achieve a multi-input multi-output (MIMO) linear system realization from a matrix power spectrum or, equivalently, from a given matrix correlation function by explicitly delineating both the structure and parameter values of an underlying white noise-driven Linear Time Invariant (LTI) state variable model that provides such a vector random process as its output. The arguments for the derivation of the matrix Lyapunov equation (that the variance/cross-covariance matrix satisfies ) [5, pp. 222-226] are quite familiar to many analysts but fall short in Ref. [1]’s attempt to extend them in its overly concise but appealing result, where Eq. A4 equates a function of one variable on the left hand side 2 to a function of two variables on the right hand side as an obvious impossibility. Among the beneficial results offered in [2], [3] is a non degenerate statistically stationary 2-channel numerical example: 3 Ryy(τ ) = 1 6 e−2|τ| + 1 6 e−|τ| .. 1 4 e−2|τ| · · · · · · · · · 1 4e −2|τ| .. 12e −|τ| ⇔ Syy(s) = [ 2−s (4−s2)(1−s2) 1 (4−s2) 1 (4−s2) 1 (1−s2) ] = W (−s)W (s), (1) where these second order statistics correspond to a demonstrable closed-form solution both for the intermediate (non-unique [3]) matrix spectral factorization (MSF): W (s) ≡ [ −s−(√7/2) (2+s)(1+s) −1/2 (2+s)(1+s) −s−(√7/2) (2+s)(1+s) 3/2 (2+s)(1+s) ] = H(sI − F )−1G (2) (where details of accomplishing the MSF here are provided in [2, Appendix B]) and for the resulting associated linear system realization: d dt x(t) = F1x(t) +G1w′(t) = 0 1 0 0 −1 −3 0 0 0 0 0 1 0 0 −2 −3 x(t) + −1 0 (6−√7)/2 −1/2 −1 0 (6−√7)/2 3/2 w′(t), (3) ∗Research funded by TeK Associates’ IR&D Contract No. 07-101, 9 Meriam St., Suite 7-R, Lexington, MA 02420-5336, USA. Tel./Fax: (781) 862-5870, thomas h kerr @ msn.com, www.TeKAssociates.biz 1Precise regularity conditions guranteeing that the steady-state constant symmetric positive definite matrix solution Px can be obtained from Eq. A7 with dPx(t)/dt ≡ 0 is that F have only eigenvalues with real parts strictly negative and that (F,L) be a controllable pair, where Q = LLT (and where L is a factor resulting from a Choleski decomposition of Q) [4]. 2In using this form, at this point in the derivation in [1], the assumption of stationarity had not yet been invoked as a slight mis-step of prematurely using an assumption that is invoked later. 3The power spectrum matrix depicted here on the right hand side of Eq. 1 consists of elements represented in the frequency domain by the bilateral Laplace transform, which relates to the Fourier transform via the substitution s = ω.
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