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Woo Young Lee Lecture Notes on Operator Theory

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CHAPTER 1.<br />

FREDHOLM THEORY<br />

1.3 Definiti<strong>on</strong>s and Examples<br />

In the sequel X and Y denote complex Banach spaces.<br />

Definiti<strong>on</strong> 1.3.1. An operator T ∈ B(X, Y ) is called a Fredholm operator if T X<br />

is closed, α(T ) < ∞ and β(T ) < ∞. In this case we define the index of T by the<br />

equality<br />

index (T ) := α(T ) − β(T ).<br />

In the below we shall see that the c<strong>on</strong>diti<strong>on</strong> “ T X is closed ” is automatically fulfilled<br />

if β(T ) < ∞.<br />

Example 1.3.2. If X and Y are both finite dimensi<strong>on</strong>al then any operator T ∈<br />

B(X, Y ) is Fredholm and<br />

indeed recall the “rank theorem”<br />

which implies<br />

index(T ) = dim X − dim Y :<br />

dim X = dim T −1 (0) + dim T X,<br />

index(T ) = dim T −1 (0) − dim Y/T X<br />

= dim X − dim T X − (dim Y − dim T X)<br />

= dim X − dim Y.<br />

Thus in particular, if T ∈ B(X) with dim X < ∞ then T is Fredholm of index zero.<br />

Example 1.3.3. If K ∈ B(X) is a compact operator then T = I − K is Fredholm of<br />

index 0. This follows from the Fredholm theory for compact operators.<br />

Example 1.3.4. If U is the unilateral shift operator <strong>on</strong> l 2 , then<br />

index U = −1 and index U ∗ = −1.<br />

With U and U ∗ , we can build a Fredholm operator whose index is equal to an arbitrary<br />

prescribed integer. Indeed if<br />

[ ] U<br />

p<br />

0<br />

T =<br />

0 U ∗q : l 2 ⊕ l 2 → l 2 ⊕ l 2 ,<br />

then T is Fredholm, α(T ) = q, β(T ) = p, and hence index T = q − p.<br />

10

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