# Topic 3: Separable Hilbert spaces ## Infinite-dimensional Hilbert spaces Recall from Topic 1. [$L^2$ space](https://notenextra.trance-0.com/Math401/Math401_T1#section-3-further-definitions-in-measure-theory-and-integration) Let $\lambda$ be a measure on $\mathbb{R}$, or any other field you are interested in. A function is square integrable if $$ \int_\mathbb{R} |f(x)|^2 d\lambda(x)<\infty $$ ### $L^2$ space and general Hilbert spaces #### Definition of $L^2(\mathbb{R},\lambda)$ The space $L^2(\mathbb{R},\lambda)$ is the space of all square integrable, measurable functions on $\mathbb{R}$ with respect to the measure $\lambda$ (The Lebesgue measure). The Hermitian inner product is defined by $$ \langle f,g\rangle=\int_\mathbb{R} \overline{f(x)}g(x) d\lambda(x) $$ The norm is defined by $$ \|f\|=\sqrt{\int_\mathbb{R} |f(x)|^2 d\lambda(x)} $$ The space $L^2(\mathbb{R},\lambda)$ is complete. [Proof ignored here] > Recall the definition of [complete metric space](https://notenextra.trance-0.com/Math4111/Math4111_L17#definition-312). The inner product space $L^2(\mathbb{R},\lambda)$ is complete. #### Definition of general Hilbert space A Hilbert space is a complete inner product vector space. #### General Pythagorean theorem Let $u_1,u_2,\cdots,u_N$ be an orthonormal set in an inner product space $\mathscr{V}$ (may not be complete). Then for all $v\in \mathscr{V}$, $$ \|v\|^2=\sum_{i=1}^N |\langle v,u_i\rangle|^2+\left\|v-\sum_{i=1}^N \langle v,u_i\rangle u_i\right\|^2 $$ [Proof ignored here] #### Bessel's inequality Let $u_1,u_2,\cdots,u_N$ be an orthonormal set in an inner product space $\mathscr{V}$ (may not be complete). Then for all $v\in \mathscr{V}$, $$ \sum_{i=1}^N |\langle v,u_i\rangle|^2\leq \|v\|^2 $$ Immediate from the general Pythagorean theorem. ### Orthonormal bases An orthonormal subset $S$ of a Hilbert space $\mathscr{H}$ is a set all of whose elements have norm 1 and are mutually orthogonal. ($\forall u,v\in S, \langle u,v\rangle=0$) #### Definition of orthonormal basis An orthonormal subset of $S$ of a Hilbert space $\mathscr{H}$ is an orthonormal basis of $\mathscr{H}$ if there are no other orthonormal subsets of $\mathscr{H}$ that contain $S$ as a proper subset. #### Theorem of existence of orthonormal basis Every separable Hilbert space has an orthonormal basis. [Proof ignored here] #### Theorem of Fourier series Let $\mathscr{H}$ be a separable Hilbert space with an orthonormal basis $\{e_n\}$. Then for any $f\in \mathscr{H}$, $$ f=\sum_{n=1}^\infty \langle f,e_n\rangle e_n $$ The series converges to some $g\in \mathscr{H}$. [Proof ignored here] #### Fourier series in $L^2([0,2\pi],\lambda)$ Let $f\in L^2([0,2\pi],\lambda)$. $$ f_N(x)=\sum_{n:|n|\leq N} c_n\frac{e^{inx}}{\sqrt{2\pi}} $$ where $c_n=\frac{1}{2\pi}\int_0^{2\pi} f(x)e^{-inx} dx$. The series converges to some $f\in L^2([0,2\pi],\lambda)$ as $N\to \infty$. This is the Fourier series of $f$. #### Hermite polynomials The subspace spanned by polynomials is dense in $L^2(\mathbb{R},\lambda)$. An orthonormal basis of $L^2(\mathbb{R},\lambda)$ can be obtained by the Gram-Schmidt process on $\{1,x,x^2,\cdots\}$. The polynomials are called the Hermite polynomials. ### Isomorphism and $\ell_2$ space #### Definition of isomorphic Hilbert spaces Let $\mathscr{H}_1$ and $\mathscr{H}_2$ be two Hilbert spaces. $\mathscr{H}_1$ and $\mathscr{H}_2$ are isomorphic if there exists a surjective linear map $U:\mathscr{H}_1\to \mathscr{H}_2$ that is bijective and preserves the inner product. $$ \langle Uf,Ug\rangle=\langle f,g\rangle $$ for all $f,g\in \mathscr{H}_1$. When $\mathscr{H}_1=\mathscr{H}_2$, the map $U$ is called unitary. #### $\ell_2$ space The space $\ell_2$ is the space of all square summable sequences. $$ \ell_2=\left\{(a_n)_{n=1}^\infty: \sum_{n=1}^\infty |a_n|^2<\infty\right\} $$ An example of element in $\ell_2$ is $(1,0,0,\cdots)$. With inner product $$ \langle (a_n)_{n=1}^\infty, (b_n)_{n=1}^\infty\rangle=\sum_{n=1}^\infty \overline{a_n}b_n $$ It is a Hilbert space (every Cauchy sequence in $\ell_2$ converges to some element in $\ell_2$). ### Bounded operators and continuity Let $T:\mathscr{V}\to \mathscr{W}$ be a linear map between two vector spaces $\mathscr{V}$ and $\mathscr{W}$. We define the norm of $\|\cdot\|$ on $\mathscr{V}$ and $\mathscr{W}$. Then $T$ is continuous if for all $u\in \mathscr{V}$, if $u_n\to u$ in $\mathscr{V}$, then $T(u_n)\to T(u)$ in $\mathscr{W}$. Using the delta-epsilon language, we can say that $T$ is continuous if for all $\epsilon>0$, there exists a $\delta>0$ such that if $\|u-v\|<\delta$, then $\|T(u)-T(v)\|<\epsilon$. #### Definition of bounded operator A linear map $T:\mathscr{V}\to \mathscr{W}$ is bounded if $$ \|T\|=\sup_{\|u\|=1}\|T(u)\|< \infty $$ #### Theorem of continuity and boundedness A linear map $T:\mathscr{V}\to \mathscr{W}$ is continuous if and only if it is bounded. [Proof ignored here] #### Definition of bounded Hilbert space The set of all bounded linear operators in $\mathscr{V}$ is denoted by $\mathscr{B}(\mathscr{V})$.