Spectral Theory in Hilbert Space
Spectral Theory in Hilbert Space
Spectral Theory in Hilbert Space
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18 3. HILBERT SPACE<br />
Two subspaces M and N are said to be orthogonal if every element<br />
<strong>in</strong> M is orthogonal to every element <strong>in</strong> N. Then clearly M ∩ N = {0}<br />
so the direct sum of M and N is def<strong>in</strong>ed. In the case at hand this is<br />
called the orthogonal sum of M and N and denoted by M ⊕ N. Thus<br />
M ⊕ N is the set of all sums u + v with u ∈ M and v ∈ N. If M and<br />
N are closed, orthogonal subspaces of H, then their orthogonal sum is<br />
also a closed subspace of H (Exercise 3.5). If A is an arbitrary subset<br />
of H we def<strong>in</strong>e<br />
A ⊥ = {u ∈ H | 〈u, v〉 = 0 for all v ∈ A}.<br />
This is called the orthogonal complement of A. It is easy to see that<br />
A ⊥ is a closed l<strong>in</strong>ear subspace of H, that A ⊂ B implies B ⊥ ⊂ A ⊥ and<br />
that A ⊂ (A ⊥ ) ⊥ (Exercise 3.6).<br />
When M is a l<strong>in</strong>ear subspace of H an alternative way of writ<strong>in</strong>g<br />
M ⊥ is H ⊖ M. This makes sense because of the follow<strong>in</strong>g theorem of<br />
central importance.<br />
Theorem 3.7. Suppose M is a closed l<strong>in</strong>ear subspace of H. Then<br />
M ⊕ M ⊥ = H.<br />
Proof. M ⊕ M ⊥ is a closed l<strong>in</strong>ear subspace of H so if it is not<br />
all of H, then it has a non-trivial normal u by Lemma 3.6. But if u is<br />
orthogonal to both M and M ⊥ , then u ∈ M ⊥ ∩ (M ⊥ ) ⊥ which shows<br />
that u cannot be = 0. The theorem follows. <br />
A nearly obvious consequence of Theorem 3.7 is that M ⊥⊥ = M<br />
for any closed l<strong>in</strong>ear subspace M of H (Exercise 3.7).<br />
A l<strong>in</strong>ear form ℓ on H is complex-valued l<strong>in</strong>ear function on H. Naturally<br />
ℓ is said to be cont<strong>in</strong>uous if ℓ(uj) → ℓ(u) whenever uj → u. The<br />
set of cont<strong>in</strong>uous l<strong>in</strong>ear forms on a Banach space B (or a more general<br />
topological vector space) is made <strong>in</strong>to a l<strong>in</strong>ear space <strong>in</strong> an obvious way.<br />
This space is called the dual of B, and is denoted by B ′ . A cont<strong>in</strong>uous<br />
l<strong>in</strong>ear form on a Banach space B has to be bounded <strong>in</strong> the sense that<br />
there is a constant C such that |ℓ(u)| ≤ Cu for any u ∈ B. For<br />
suppose not. Then there exists a sequence of elements u1, u2, . . . of<br />
B for which |ℓ(uj)|/uj → ∞. Sett<strong>in</strong>g vj = uj/ℓ(uj) we then have<br />
vj → 0 but |ℓ(vj)| = 1 → 0, so ℓ can not be cont<strong>in</strong>uous. Conversely, if<br />
ℓ is bounded by C then |ℓ(uj) − ℓ(u)| = |ℓ(uj − u)| ≤ Cuj − u → 0 if<br />
uj → u, so a bounded l<strong>in</strong>ear form is cont<strong>in</strong>uous. The smallest possible<br />
bound of a l<strong>in</strong>ear form ℓ is called the norm of ℓ, denoted ℓ.<br />
It is easy to see that provided with this norm B ′ is complete, so the<br />
dual of a Banach space is a Banach space (Exercise 3.8). A familiar<br />
example is given by the space L p (Ω, µ) for 1 ≤ p < ∞, where Ω is<br />
a doma<strong>in</strong> <strong>in</strong> R n and µ a Radon measure def<strong>in</strong>ed <strong>in</strong> Ω. The dual of<br />
this space is Lq (Ω, µ), where q is the conjugate exponent to p, <strong>in</strong> the<br />
sense that 1 1 + = 1. A simple example of a bounded l<strong>in</strong>ear form on<br />
p q<br />
a <strong>Hilbert</strong> space H is ℓ(u) = 〈u, v〉, where v is some fixed element of