Section 3.2 Hilbert spaces
Definition 3.2.1. Hilbert space.
A Hilbert space is a vector space which a scalar product that is complete with respect to the induced metric space structure.Subsection 3.2.1 Example: scalar products on \(C^\infty([0,1])\)
The \(L^2\) scalar product. Set
\begin{equation*}
\langle f,g\rangle_{L^2} = \int_0^1 f(s)g(s)\;ds
\end{equation*}
if \(\bK=\bR\) and
\begin{equation*}
\langle f,g\rangle_{L^2} = \int_0^1 f(s)\overline{g(s)}\;ds
\end{equation*}
if \(\bK=\bC\text{.}\) One can easily verify that \(\langle \cdot,\cdot\rangle_{L^2}\) is a scalar product on \(C^\infty([0,1])\text{.}\) The corresponding norm is the \(L^2\) norm and so the completion of this space is \(L^2([0,1])\text{.}\) Hence, \(L^2([0,1])\) is a Hilbert space.
The \(H^k\) scalar product. Set
\begin{equation*}
\langle f,g\rangle_{H^k} = \langle f,g\rangle_{L^2} + \langle f',g'\rangle_{L^2} + \dots + \langle f^{(k)},g^{(k)}\rangle_{L^2}.
\end{equation*}
The corresponding norm is the \(H^k\) norm and so the completion of this space is \(H^k([0,1])\) (see Subsection 3.1.2). Hence, \(H^k([0,1])\) is a Hilbert space.Subsection 3.2.2 Some fundamental results on Hilbert spaces
The existence of a scalar product has several fundamental consequences.Definition 3.2.2. Orthogonality.
If \(u,v\in H\) are such that \(\langle u,v \rangle = 0\text{,}\) we say that \(u\) and \(v\) are orthogonal and we write sometimes \(u\perp v\text{.}\) We say that two sets \(A,B\subset H\) are othogonal when all vectors of \(A\) are orthogonal to all vectors of \(B\text{.}\) The orthogonal complement of \(M\) in \(H\) is the set
\begin{equation*}
M^\perp :=\{u\in H: \langle u,v\rangle =0, \quad\mbox{for all}\quad v\in M\}.
\end{equation*}
Proposition 3.2.3. Orthogonal complement.
Let \(M\subset H\text{.}\) Its orthogonal complement \(M\perp\) is a closed linear subspace of \(H\text{.}\)Proof.
Proposition 3.2.5. Proximality.
Let \(M\) be a closed linear subspace of \(H\text{.}\) Then:- \(M\) is proximal, i.e., for each \(v\in H\) there is a unique closest vector \(u\in M\) such that\begin{equation*} \|v-u\| = \min_{w\in M}\|v-w\|. \end{equation*}
- The \(u\) above is the unique element of \(M\) such \((v-u)\perp M\text{.}\)
Proof.
\begin{align*}
\|u_n-u_m\|^2 & = 2\|v-u_n\|^2+2\|v-u_m\|^2-4\|v-\frac{u_n+u_m}{2}\|^2\leq\\
& \leq 2(\|v-u_n\|^2-d^2) + 2(\|v-u_m\|^2-d^2)
\end{align*}
and, by construction, by taking \(m\) and \(n\) large enough, we can make the two summands above as small as we please. Since \(M\) is closed and \(H\) is complete, there is a \(u\in M\) with \(u_n\to u\text{.}\) Hence, by continuity, \(\|v-u\| = \lim \|v-u_n\| = \inf_{w\in M}\|v-w\|\text{.}\) Now we want an explicit parametrization of this minimum. For that we take a \(y\in M\) and consider
\begin{equation*}
D(t) := \|v-(u-ty)\|^2 = \|v-u+ty\|^2 = \|v-u\|^2 + 2t(v-u,y) + t^2 \|y\|^2.
\end{equation*}
We know that \(D(t)\) is minimal for \(t=0\text{,}\) hence
\begin{equation*}
D′(t) = 2\langle v-u,y\rangle =0, \qquad \mbox{for all }\quad\quad y\in M.
\end{equation*}
This means \(v-u\in M^\perp\text{.}\) To show uniqueness of \(u\text{,}\) we assume that there in another minimizer \(u'\text{.}\) Then
\begin{equation*}
0 = \langle v-u,u-u'\rangle = \langle v-u',u-u'\rangle.
\end{equation*}
By substracting the two, we get that \(\|u-u'\|=0\text{,}\) i.e. \(u=u'\text{.}\)Proposition 3.2.6. Orthogonal decomposition.
Let \(M\subset H\) be a closed linear subspace. Then \(M\oplus M^\perp\text{.}\) In particular, every closed linear subset of a Hilbert space is complemented.Proof.
\begin{equation*}
P_M :H\to M, \quad P_M x = P_M(u+v) = u,
\end{equation*}
where \(x=u+v\) is the unique decomposition of Proposition \ref{p:decompose}. The projection has the property
\begin{equation*}
P_M^2=P_M, \qquad \mbox{and} \qquad \|P_M\|_{op} \leq 1,
\end{equation*}
where we will introduce the operator norm in the next chapter. We can take this orthogonal decomposition to the extreme, by decomposing with respect to one-dimensional subspaces. Doing this we quite naturally arrive at a Schauder basis. Proposition 3.2.7. Schauder basis.
Let \(H\) be a Hilbert space. Then the following conditions are equivalent:- \(H\) has a Schauder basis;
- \(H\) has a orthonormal Schauder basis;
- \(H\) is separable.
Proof.
\begin{equation*}
\|v-\sum_{n=0}^k \langle v,e_n\rangle e_n\|^2 = \langle v-\sum_{n=0}^k \langle v,e_n\rangle e_n, v-\sum_{n=0}^k \langle v,e_n\rangle e_n\rangle
\end{equation*}
Hence, \(\{e_n\}\) is a Schauder basis for \(H\text{.}\)Proposition 3.2.8. Unit ball.
The unit sphere in an infinite dimensional Hilbert space is not compact.Proof.
\begin{equation*}
\|e_n - e_m\|^2 = (e_n-e_m, e_n-e_m) = \|e_n\|^2 + \|e_m\|^2 = 2
\end{equation*}
for all \(n \neq m\text{.}\) Hence, \(\{e_j\}\) is a bounded sequence, but not a Cauchy sequence, and it does not converge in \(\overline{B_1(0)}\text{.}\)