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A.3. EXAMPLE 253<br />

where the eigenvec<strong>to</strong>r ˜w is structured as:<br />

⎛<br />

˜w =<br />

⎜<br />

⎝<br />

v<br />

λv<br />

µv<br />

λ 2 v<br />

λµv<br />

µ 2 v<br />

⎞<br />

. (A.27)<br />

⎟<br />

⎠<br />

This problem is of dimension 6n × 6n and the eigenvec<strong>to</strong>r ˜w only incorporates powers<br />

of λ and µ up till a <strong>to</strong>tal degree of m − 1 = 2. Note that the last equation represented<br />

by (A.26) equals M(µ, λ)v = 0 with the matrix M(µ, λ) as in Equation (A.16).

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