“…In the numerical experiments given below,H k = H (x k , y k ) + E k , where E k is a positive-semidefinite modification chosen to ensure that the inertia of the regularized equations (5.5) is (n, m, 0). If the inertia is correct, then E k = 0; otherwise E k is defined implicitly by modifying the eigenvalues associated with the spectral decomposition of H (x k , y k ) (see Greenstadt [31]). Other, more practical approaches include: (i) modifying an inertia-controlling factorization of the KKT matrix [19,21]; (ii) using a positive-definite quasi-Newton approximation to H (x k , y k ) [24,29,30,44]; and (iii) adding increasing positive multiples of the identity matrix to H (x k , y k ) until the inertia is correct [53].…”