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Notice that the polynomials { Dj (ω;k) } 0 can be obtained from the canonical basis { 1,ω, ω2,... } by the Gramm-Schmidt procedure with the scalar product in the vector space of (real) polynomials defined as f,g = - f (ω) g (ω) S (k,ω) dω.
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Observe that Eq. coincides with Eq. (2.159) of if we identify the Nevanlinna static parameter τ (k) as the generalized viscoelastic relaxation time τm (k) and observe that by Eq. (2.146) of, U (k) =-I (k).
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