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Inner Product Spaces and Hilbert Spaces

2.1 Inner Product Spaces

An inner product space is a vector space HH with an inner product ,:H×HC\langle \cdot, \cdot \rangle : H \times H \to \mathbb{C} satisfying:

  1. x,x0\langle x, x\rangle \geq 0 with equality iff x=0x = 0.
  2. x,y=y,x\langle x, y\rangle = \overline{\langle y, x\rangle}.
  3. αx+βy,z=αx,z+βy,z\langle \alpha x + \beta y, z\rangle = \alpha\langle x, z\rangle + \beta\langle y, z\rangle.

Every inner product induces a norm: x=x,x\|x\| = \sqrt{\langle x, x\rangle}.

Example 1. Cn\mathbb{C}^n with x,y=i=1nxiyi\langle x, y\rangle = \sum_{i=1}^n x_i \overline{y_i}.

Example 2. L2(μ)L^2(\mu) with f,g=fgdμ\langle f, g\rangle = \int f \overline{g}\, d\mu.

2.2 Orthogonality

Vectors x,yHx, y \in H are orthogonal (written xyx \perp y) if x,y=0\langle x, y\rangle = 0.

Theorem 2.1 (Pythagorean Theorem). If xyx \perp y, then x+y2=x2+y2\|x + y\|^2 = \|x\|^2 + \|y\|^2.

Theorem 2.2 (Parallelogram Law). In any inner product space:

x+y2+xy2=2x2+2y2\|x + y\|^2 + \|x - y\|^2 = 2\|x\|^2 + 2\|y\|^2

Theorem 2.3 (Polarization Identity). In a complex inner product space:

x,y=14(x+y2xy2+ix+iy2ixiy2)\langle x, y\rangle = \frac{1}{4}\left(\|x + y\|^2 - \|x - y\|^2 + i\|x + iy\|^2 - i\|x - iy\|^2\right)

Theorem 2.4 (Cauchy-Schwarz Inequality). x,yxy|\langle x, y\rangle| \leq \|x\| \cdot \|y\| with equality iff xx and yy are linearly dependent.

2.3 Hilbert Spaces

A Hilbert space is a complete inner product space.

Theorem 2.5 (Orthogonal Projection). Let MM be a closed subspace of a Hilbert space HH. For every xHx \in H, there exists a unique yMy \in M (the orthogonal projection of xx onto MM) such that xyMx - y \perp M. We write y=PM(x)y = P_M(x).

Theorem 2.6 (Orthogonal Decomposition). If MM is a closed subspace of HH, then H=MMH = M \oplus M^\perp, where M={xH:xM}M^\perp = \{x \in H : x \perp M\}.

2.4 Orthonormal Bases

A set {ei}iIH\{e_i\}_{i \in I} \subseteq H is an orthonormal system if ei,ej=δij\langle e_i, e_j\rangle = \delta_{ij}.

Theorem 2.7 (Bessel”s Inequality). If {ei}i=1n\{e_i\}_{i=1}^n is an orthonormal set, then i=1nx,ei2x2\sum_{i=1}^n |\langle x, e_i\rangle|^2 \leq \|x\|^2.

Theorem 2.8. A Hilbert space is separable if and only if it admits a countable orthonormal basis.

Theorem 2.9 (Parseval’s Identity). If {en}\{e_n\} is an orthonormal basis for HH, then for every xHx \in H:

x2=n=1x,en2andx=n=1x,enen\|x\|^2 = \sum_{n=1}^{\infty} |\langle x, e_n\rangle|^2 \quad \text{and} \quad x = \sum_{n=1}^{\infty} \langle x, e_n\rangle e_n

2.5 Riesz Representation Theorem

Theorem 2.10 (Riesz Representation). Let HH be a Hilbert space. For every bounded linear functional φH\varphi \in H^*, there exists a unique yHy \in H such that φ(x)=x,y\varphi(x) = \langle x, y\rangle for all xHx \in H. Moreover, φH=yH\|\varphi\|_{H^*} = \|y\|_H.

Proof. If φ=0\varphi = 0, take y=0y = 0. Otherwise, ker(φ)\ker(\varphi) is a closed subspace, so H=ker(φ)ker(φ)H = \ker(\varphi) \oplus \ker(\varphi)^\perp. Take zker(φ)z \in \ker(\varphi)^\perp with z=1\|z\| = 1. Then y=φ(z)zy = \overline{\varphi(z)} \cdot z satisfies φ(x)=x,y\varphi(x) = \langle x, y\rangle for all xx. Uniqueness follows from the polarization identity. \blacksquare

Corollary 2.11. Every Hilbert space is isometrically isomorphic to its dual: HHH \cong H^* (anti-linearly).