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Spectral Theory in Hilbert Space

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APPENDIX C<br />

L<strong>in</strong>ear first order systems<br />

In this appendix we will prove some standard results about l<strong>in</strong>ear<br />

first order systems of differential equations which are used <strong>in</strong> the text.<br />

We will prove no more than we actually need, although the theorems<br />

have easy generalizations to non-l<strong>in</strong>ear equations, more complicated parameter<br />

dependence, etc. The first result is the standard existence and<br />

uniqueness theorem, Theorem 13.1, which also implies Theorem 10.1.<br />

Theorem. Suppose A is an n × n matrix-valued function with locally<br />

<strong>in</strong>tegrable entries <strong>in</strong> an <strong>in</strong>terval I, and that B is an n × 1 matrixvalued<br />

function, locally <strong>in</strong>tegrable <strong>in</strong> I. Assume further that c ∈ I and<br />

C is an n × 1 matrix. Then the <strong>in</strong>itial value problem<br />

(C.1)<br />

<br />

u ′ = Au + B <strong>in</strong> I,<br />

u(c) = C,<br />

has a unique n × 1 matrix-valued solution u with locally absolutely cont<strong>in</strong>uous<br />

entries def<strong>in</strong>ed <strong>in</strong> I.<br />

Corollaries 13.2 and 10.2 are immediate consequences of the theorem.<br />

Corollary. Let A and I be as <strong>in</strong> the previous theorem. Then the<br />

set of solutions to u ′ = Au <strong>in</strong> I is an n-dimensional l<strong>in</strong>ear space.<br />

Proof. It is clear that any l<strong>in</strong>ear comb<strong>in</strong>ation of solutions is also<br />

a solution, so the set of solutions is a l<strong>in</strong>ear space. We must show<br />

that it has dimension n. Let uk solve the <strong>in</strong>itial value problem with<br />

uk(c) equal to the k:th column of the n × n unit matrix. If u is any<br />

solution of the equation, and the components of u(c) are x1, . . . , xn,<br />

then the function x1u1+· · ·+xnun is also a solution with the same <strong>in</strong>itial<br />

data. It therefore co<strong>in</strong>cides with u, and it is clear that no other l<strong>in</strong>ear<br />

comb<strong>in</strong>ation of u1, . . . , un has the same <strong>in</strong>itial data as u. It follows<br />

that u1, . . . , un is a basis for the space of solutions, which therefore is<br />

n-dimensional. <br />

F<strong>in</strong>ally we shall prove Theorem 15.1.<br />

Theorem. A solution u(x, λ) of Ju ′ + Qu = λW u with <strong>in</strong>itial<br />

data <strong>in</strong>dependent of λ is an entire function of λ, locally uniformly with<br />

respect to x.<br />

129

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