Almost Periodic Solutions to Difference Equations

Cover Almost Periodic Solutions to Difference Equations
Almost Periodic Solutions to Difference Equations
Alvin Bayliss
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7)), (9. 5) w ^, = U(kB, - k6 ) + k 0(l)w .
n+1 h n n It is clear that this will hold uniformly in k and h if k + k/h is sufficiently small, i. E. If we are in a region (9. 6) k + ^ = 0(1) .
h Of course restrictions of the form (9. 6) are included in (9. 4) Also note from the explicit definition of the full linear term in (9. 5) (see (2. 11)) the last term in (9. 5) will be uniform in k and h. For the rest of this section this will be understood for all "O" signs unless stated otherwise.
If W (
...k, h) is the fundamental solution to (9. 5) it is n clear that all we must show is that in a region of the form (9. 4) we will have _i -a k(n-j) (9. 7) IIW W. II j, n j — 1 — where the constants K^ and a, are independent of k and h. Following the procedure of Section 3 we let (9. 8) v = T(kB, - k6, )w^ n n n n -87- and we then have in a region of the form (9. 6) (9. 9) v„, = L(kB - k6 )v^ + k 0(1) v^ n+l n n n n Using the structure of the block diagonal operator L(z) derived in Theorem 1 we can write this as (9.

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