Basic Analysis – Gently Done Topological Vector Spaces
Basic Analysis – Gently Done Topological Vector Spaces
Basic Analysis – Gently Done Topological Vector Spaces
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124 <strong>Basic</strong> <strong>Analysis</strong><br />
Remark 10.27 It is sometimes easier to check that a map T has a closed graph<br />
than to check that it is continuous. For the latter, it is necessary to show that<br />
if x n → x, then Tx n does, in fact, converge and has limit equal to Tx. To show<br />
that T has a closed graph, one starts with the hypotheses that both x n and Tx n<br />
converge, the first to x and the second to some y. All that remains is to show that<br />
Tx = y.<br />
The following application to operators on a Hilbert space is of interest. It says<br />
that a symmetric operator defined on the whole Hilbert space is bounded. This<br />
is of interest in quantum mechanics where symmetric operators (or self-adjoint<br />
operators, to be precise) are used to represent physically observable quantities. It<br />
turns out that these are often unbounded operators. The following theorem says<br />
that it is no use trying to define such objects on the whole space. Instead one uses<br />
dense linear subspaces as domains of definition for unbounded operators.<br />
Theorem 10.28 (Hellinger-Toeplitz) Suppose that T : H → H is a linear operator<br />
on a Hilbert space H such that<br />
〈Tx,y〉 = 〈x,Ty〉<br />
for every x,y ∈ H. Then T is continuous.<br />
Proof A Hilbert space is a Banach space, so is complete. We need only show that<br />
T has closed graph. So suppose that (x n ,Tx n ) → (x,y) in H×H. For any z ∈ H,<br />
However, Tx n → y and so<br />
〈Tx n ,z〉 = 〈x n ,Tz〉 → 〈x,Tz〉 = 〈Tx,z〉.<br />
〈y,z〉 = 〈Tx,z〉<br />
and we deduce that y = Tx. It follows that Γ(T) is closed and so T is a continuous<br />
linear operator on H.<br />
We shall end this chapter with a brief discussion of projections. Let X be a<br />
linear space and suppose that V and W are subspaces of X such that V ∩W = {0}<br />
and X = span{V,W}. Then any x ∈ X can be written uniquely as x = v + w<br />
with v ∈ V and w ∈ W. In other words, X = V ⊕W. Define a map P : X → V<br />
by Px = v, where x = v +w ∈ X, with v ∈ V and w ∈ W, as above. Evidently,<br />
P is a well-defined linear operator satisfying P 2 = P. P is called the projection<br />
onto V along W. We see that ranP = V (since Pv = v for all v ∈ V), and also<br />
kerP = W (since if x = v + w and Px = 0 then we have 0 = Px = v and so<br />
x = w ∈ W).<br />
Conversely, suppose that P : X → X is a linear operator such that P 2 = P,<br />
that is, P is an idempotent. Set V = ranP and W = kerP. Evidently, W is a<br />
Department of Mathematics King’s College, London