“…Let n = 2, m = 1 (so N = 3), denote the columns of I 3 by e i , i = 1, 2, 3, and let and clearly (β −1 , e 2 ) is an eigenpair of S, 0 is a double algebraic, simple geometric eigenvalue, e 3 is the corresponding eigenvector and e 1 is the generalised eigenvector or principal eigenvector of grade 2. This behaviour is generic in N × N problems with the block structure of (2) as was shown by Malkus [9], who considered the Weierstrass-Kronecker canonical form of (2), and Ericsson [5], who considered the Jordan form for the shift-invert transformation of a variety of generalised eigenvalue problems. (Incidently, both authors restrict attention to problems with symmetric A but several of their results, at least to do with Jordan structure, extend to the case when A is nonsymmetric).…”