DIFFERENtIAl & DIFFERENCE EqUAtIONS ANd APPlICAtIONS
DIFFERENtIAl & DIFFERENCE EqUAtIONS ANd APPlICAtIONS
DIFFERENtIAl & DIFFERENCE EqUAtIONS ANd APPlICAtIONS
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BOUNDARY VALUE PROBLEMS ON THE HALF-LINE<br />
WITHOUT DICHOTOMIES<br />
JASON R. MORRIS AND PATRICK J. RABIER<br />
Given a piecewise continuous function A : R + → (C N )andaprojectionP 1 onto a subspace<br />
X 1 of C N , we investigate the injectivity, surjectivity and, more generally, the Fredholmness<br />
of the differential operator with boundary condition ( ˙u + Au,P 1 u(0)) acting on<br />
the “natural” space WA<br />
1,2 ={u : ˙u ∈ L 2 , Au ∈ L 2 }. It is not assumed that A is bounded or<br />
that ˙u + Au = 0 has any dichotomy, except to discuss the impact of the results on this special<br />
case. All the functional properties of interest, including the Fredholm index, can be<br />
related to a selfadjoint solution H of the Riccati differential inequality HA+ A ∗ H − Ḣ ≥<br />
ν(A ∗ A + H 2 ).<br />
Copyright © 2006 J. R. Morris and P. J. Rabier. This is an open access article distributed<br />
under the Creative Commons Attribution License, which permits unrestricted use, distribution,<br />
and reproduction in any medium, provided the original work is properly cited.<br />
1. Introduction<br />
The problem of interest is the existence and possible uniqueness of solutions in Sobolevlike<br />
spaces of the linear boundary value problem on R + = [0,∞),<br />
˙u + Au = f ,<br />
P 1 u(0) = ξ,<br />
(1.1)<br />
where A : R + → (C N )islocallyboundedandP 1 and P 2 are the projections associated<br />
with a given splitting C N = X 1 ⊕ X 2 .<br />
When P 1 = I, that is, X 1 = C N and X 2 ={0}, the familiar Cauchy problem is recovered,<br />
but, even in this case, the existence question in spaces constraining the possible<br />
behavior of the solutions at infinity (such as W 1,2 (R + ,C N )) does not follow from local<br />
existence and uniqueness and is far from being fully resolved. Furthermore, many concrete<br />
problems arise in the form (1.1) withP 1 ≠ I. For instance, second-order equations<br />
¨v + B ˙v + Cv = g with Dirichlet condition v(0) = ξ or Neumann condition ˙v(0) = ξ correspond<br />
to first-order systems (1.1) withN = 2M, C N = C M × C M , u = (v, ˙v), and P 1 the<br />
projection onto the first factor (Dirichlet) or the second one (Neumann). We will denote<br />
Hindawi Publishing Corporation<br />
Proceedings of the Conference on Differential & Difference Equations and Applications, pp. 825–833