1 research outputs found

    Perturbation analysis of a matrix differential equation xË™=ABx\dot x=ABx

    Full text link
    Two complex matrix pairs (A,B)(A,B) and (A′,B′)(A',B') are contragrediently equivalent if there are nonsingular SS and RR such that (A′,B′)=(S−1AR,R−1BS)(A',B')=(S^{-1}AR,R^{-1}BS). M.I. Garc\'{\i}a-Planas and V.V. Sergeichuk (1999) constructed a miniversal deformation of a canonical pair (A,B)(A,B) for contragredient equivalence; that is, a simple normal form to which all matrix pairs (A+A~,B+B~)(A + \widetilde A, B+\widetilde B) close to (A,B)(A,B) can be reduced by contragredient equivalence transformations that smoothly depend on the entries of A~\widetilde A and B~ \widetilde B. Each perturbation (A~,B~)(\widetilde A,\widetilde B) of (A,B)(A,B) defines the first order induced perturbation AB~+A~BA\widetilde{B}+\widetilde{A}B of the matrix ABAB, which is the first order summand in the product (A+A~)(B+B~)=AB+AB~+A~B+A~B~(A +\widetilde{A})(B+\widetilde{B}) = AB + A\widetilde{B}+\widetilde{A}B+ \widetilde A \widetilde B. We find all canonical matrix pairs (A,B)(A,B), for which the first order induced perturbations AB~+A~BA\widetilde{B}+\widetilde{A}B are nonzero for all nonzero perturbations in the normal form of Garc\'{\i}a-Planas and Sergeichuk. This problem arises in the theory of matrix differential equations x˙=Cx\dot x=Cx, whose product of two matrices: C=ABC=AB; using the substitution x=Syx = Sy, one can reduce CC by similarity transformations S−1CSS^{-1}CS and (A,B)(A,B) by contragredient equivalence transformations (S−1AR,R−1BS)(S^{-1}AR,R^{-1}BS)
    corecore