Journal
MEMOIRS OF THE AMERICAN MATHEMATICAL SOCIETY
Volume 275, Issue 1347, Pages 1-+Publisher
AMER MATHEMATICAL SOC
DOI: 10.1090/memo/1347
Keywords
Linear Hamiltonian PDEs; stability; index formula; exponential trichotomy; structural decomposition; spectral mapping; Hamiltonian perturbations
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In this paper, we study the properties of general linear Hamiltonian systems in a Hilbert space. By structural decomposition, we prove the linear exponential trichotomy and an instability index theorem for the system, and provide index information for pure imaginary eigenvalues. Moreover, we discuss several specific Hamiltonian PDEs, including dispersive long wave models, the 2D Euler equation for ideal fluids, and the 2D nonlinear Schrödinger equation with nonzero conditions at infinity.
Consider a general linear Hamiltonian system partial derivative tu = JLu in a Hilbert space X. We assume that L : X -> X* induces a bounded and symmetric bi-linear form < L center dot, center dot > on X, which has only finitely many negative dimensions n(-)( L). There is no restriction on the anti-self-dual operator J : X*superset of D(J) -> X. We first obtain a structural decomposition of X into the direct sum of several closed subspaces so that L is blockwise diagonalized and JL is of upper triangular form, where the blocks are easier to handle. Based on this structure, we first prove the linear exponential trichotomy of e(tJL). In particular, etJL has at most algebraic growth in the finite co-dimensional center subspace. Next we prove an instability index theorem to relate n(-)(L) and the dimensions of generalized eigenspaces of eigenvalues of JL, some of which may be embedded in the continuous spectrum. This generalizes and refines previous results, where mostly J was assumed to have a bounded inverse. More explicit information for the indexes with pure imaginary eigenvalues are obtained as well. Moreover, when Hamiltonian perturbations are considered, we give a sharp condition for the structural instability regarding the generation of unstable spectrum from the imaginary axis. Finally, we discuss Hamiltonian PDEs including dispersive long wave models (BBM, KDV and good Boussinesq equations), 2D Euler equation for ideal fluids, and 2D nonlinear Schrodinger equations with nonzero conditions at infinity, where our general theory applies to yield stability or instability of some coherent states.
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