Woo Young Lee Lecture Notes on Operator Theory
Woo Young Lee Lecture Notes on Operator Theory
Woo Young Lee Lecture Notes on Operator Theory
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CHAPTER 4.<br />
WEIGHTED SHIFTS<br />
For example, given α 0 < α 1 < α 2 , W (α0,α ̂ is the recursive weighted shift whose<br />
1,α 2)<br />
weights are calculated according to the recursive relati<strong>on</strong><br />
αn+1 2 1<br />
= φ 1 + φ 0<br />
αn<br />
2 ,<br />
where φ 0 = − α2 0 α2 1 (α2 2 −α2 1 ) and φ<br />
α 2 1 = − α2 1 (α2 2 −α2 0 ) . In this case, W<br />
1 −α2 0<br />
α 2 1 −α2 ̂<br />
0<br />
(α0<br />
is subnormal<br />
with 2-atomic Berger measure. Write W x(α0 ̂ for the weighted shift whose<br />
,α 1 ,α 2 )<br />
,α 1 ,α 2 )<br />
weight sequence c<strong>on</strong>sists of the initial weight x followed by the weight sequence of<br />
W<br />
.<br />
(α0,α ̂ 1,α 2)<br />
By the Density Theorem ([CuF2, Theorem 4.2 and Corollary 4.3]), we know that<br />
if W α is a subnormal weighted shift with weights α = {α n } and ϵ > 0, then there<br />
exists a n<strong>on</strong>zero compact operator K with ||K|| < ϵ such that W α +K is a recursively<br />
generated subnormal weighted shift; in fact W α + K = W for some m ≥ 1, where<br />
̂α(m)<br />
α (m) : α 0 , · · · , α m . The following result shows that K cannot generally be taken to<br />
be finite rank.<br />
Theorem 4.4.1. (Finite Rank Perturbati<strong>on</strong>s of Subnormal Shifts) If W α is a subnormal<br />
weighted shift then there exists no n<strong>on</strong>zero finite rank operator F (≠ cP {e0 }) such<br />
that W α + F is a subnormal weighted shift. C<strong>on</strong>cretely, suppose W α is a subnormal<br />
weighted shift with weight sequence α = {α n } ∞ n=0 and assume α ′ = {α n} ′ is a n<strong>on</strong>zero<br />
perturbati<strong>on</strong> of α in a finite number of weights except the initial weight; then W α ′ is<br />
not subnormal.<br />
We next c<strong>on</strong>sider the selfcommutator [(W α + s W 2 α) ∗ , W α + s W 2 α]. Let W α be a<br />
hyp<strong>on</strong>ormal weighted shift. For s ∈ C, we write<br />
D(s) := [(W α + s W 2 α) ∗ , W α + s W 2 α]<br />
and we let<br />
⎡<br />
⎤<br />
q 0 ¯r 0 0 . . . 0 0<br />
r 0 q 1 ¯r 1 . . . 0 0<br />
D n (s) := P n [(W α +s Wα) 2 ∗ , W α +s Wα]P 2 0 r 1 q 2 . . . 0 0<br />
n =<br />
⎢ .<br />
.<br />
.<br />
. .. . . , (4.7)<br />
⎥<br />
⎣ 0 0 0 . . . q n−1 ¯r n−1<br />
⎦<br />
0 0 0 . . . r n−1 q n<br />
where P n is the orthog<strong>on</strong>al projecti<strong>on</strong> <strong>on</strong>to the subspace generated by {e 0 , · · · , e n },<br />
⎧<br />
q n := u n + |s| 2 v n<br />
⎪⎨ r n := s √ w n<br />
u n := αn 2 − αn−1<br />
2 (4.8)<br />
v n := αnα 2 n+1 2 − αn−1α 2 n−2<br />
2 ⎪⎩<br />
w n := αn(α 2 n+1 2 − αn−1) 2 2 ,<br />
122