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Woo Young Lee Lecture Notes on Operator Theory

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CHAPTER 4.<br />

WEIGHTED SHIFTS<br />

This completes the proof.<br />

□<br />

To prove Theorem 4.4.3 we need:<br />

Lemma 4.4.7. ([CuF3, Lemma 2.3]) Let α ≡ {α n } ∞ n=0 be a strictly increasing weight<br />

sequence. If W α is 2-hyp<strong>on</strong>ormal then the sequence of quotients<br />

Θ n := u n+1<br />

u n+2<br />

(n ≥ 0)<br />

is bounded away from 0 and from ∞. More precisely,<br />

1 ≤ Θ n ≤ u 1<br />

u 2<br />

( ||Wα || 2<br />

α 0 α 1<br />

) 2<br />

for sufficiently large n.<br />

In particular, {u n } ∞ n=0 is eventually decreasing.<br />

We are ready for:<br />

Proof of Theorem 4.4.3. By Theorem 4.4.2, W α is strictly positively quadratically<br />

hyp<strong>on</strong>ormal, in the sense that all coefficients of d n (t) are positive for all n ≥ 0. Note<br />

that finite rank perturbati<strong>on</strong>s of α affect a finite number of values of u n , v n and w n .<br />

More c<strong>on</strong>cretely, if α ′ is a perturbati<strong>on</strong> of α in the weights {α 0 , · · · , α N }, then u n , v n ,<br />

w n and p n are invariant under α ′ for n ≥ N + 3. In particular, p n ≥ 0 for n ≥ N + 3.<br />

Claim 1. For n ≥ 3, 0 ≤ i ≤ n + 1,<br />

c(n, i) =u n c(n − 1, i) + p n−1 c(n − 2, i − 1) +<br />

where<br />

+ v n · · · v 3 ρ i−n+1 ,<br />

(cf. [CuF3, Proof of Theorem 4.3]).<br />

n∑<br />

k=4<br />

p k−2<br />

⎛<br />

⎝<br />

n∏<br />

j=k<br />

⎧<br />

0 (i < n − 1)<br />

⎪⎨<br />

u 0 p 1 (i = n − 1)<br />

ρ i−n+1 =<br />

v 0 p 1 + v 2 p 0 (i = n)<br />

⎪⎩<br />

v 0 v 1 v 2 (i = n + 1)<br />

Proof of Claim 1. We use inducti<strong>on</strong>. For n = 3, 0 ≤ i ≤ 4,<br />

v j<br />

⎞<br />

⎠ c(k − 3, i − n + k − 2)<br />

(4.19)<br />

c(3, i) = u 3 c(2, i) + v 3 c(2, i − 1) − w 2 c(1, i − 1)<br />

)<br />

= u 3 c(2, i) + v 3<br />

(u 2 c(1, i − 1) + v 2 c(1, i − 2) − w 1 c(0, i − 2) − w 2 c(1, i − 1)<br />

)<br />

= u 3 c(2, i) + p 2 c(1, i − 1) + v 3<br />

(v 2 c(1, i − 2) − w 1 c(0, i − 2)<br />

= u 3 c(2, i) + p 2 c(1, i − 1) + v 3 ρ i−2 ,<br />

129

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