ConceptComplete

Compact Operators - Examples and Constructions

Approximation by finite-rank operators is a fundamental technique for studying compact operators, connecting abstract theory with concrete computations.

TheoremApproximation by Finite Rank

An operator TB(X,Y)T \in \mathcal{B}(X,Y) is compact if and only if it can be approximated in operator norm by finite-rank operators. That is, there exist finite-rank operators TnT_n such that TTn0\|T - T_n\| \to 0.

This characterization is extremely useful: to prove an operator is compact, it suffices to approximate it by finite-rank operators.

DefinitionHilbert-Schmidt Operators

Let HH be a Hilbert space with orthonormal basis {en}\{e_n\}. An operator TB(H)T \in \mathcal{B}(H) is Hilbert-Schmidt if THS2=n=1T(en)2<\|T\|_{HS}^2 = \sum_{n=1}^\infty \|T(e_n)\|^2 < \infty

The Hilbert-Schmidt norm HS\|\cdot\|_{HS} is independent of the choice of orthonormal basis.

TheoremHilbert-Schmidt Operators are Compact

Every Hilbert-Schmidt operator is compact. Moreover, the space of Hilbert-Schmidt operators forms a Hilbert space with inner product S,THS=n=1S(en),T(en)\langle S, T \rangle_{HS} = \sum_{n=1}^\infty \langle S(e_n), T(e_n) \rangle

Proof

For finite-rank projection PN=n=1N,enenP_N = \sum_{n=1}^N \langle \cdot, e_n \rangle e_n, we have TPNT2TPNTHS2=n=N+1T(en)20\|T - P_N T\|^2 \leq \|T - P_N T\|_{HS}^2 = \sum_{n=N+1}^\infty \|T(e_n)\|^2 \to 0

Thus TT is approximated by finite-rank operators PNTP_N T, hence compact.

ExampleIntegral Operators

Consider (Kf)(x)=Ωk(x,y)f(y)dy(Kf)(x) = \int_\Omega k(x,y) f(y) \, dy on L2(Ω)L^2(\Omega).

  1. Continuous kernel: If kC(Ω×Ω)k \in C(\Omega \times \Omega) and Ω\Omega is compact, then KK is compact

  2. L2L^2 kernel: If kL2(Ω×Ω)k \in L^2(\Omega \times \Omega), then KK is Hilbert-Schmidt, hence compact, with KHS2=ΩΩk(x,y)2dxdy\|K\|_{HS}^2 = \int_\Omega \int_\Omega |k(x,y)|^2 \, dx \, dy

  3. Degenerate kernel: If k(x,y)=i=1nfi(x)gi(y)k(x,y) = \sum_{i=1}^n f_i(x) g_i(y), then KK has finite rank

DefinitionTrace Class Operators

An operator TT on a Hilbert space is trace class if for some (equivalently all) orthonormal basis {en}\{e_n\}, T1=n=1T(en),en<\|T\|_1 = \sum_{n=1}^\infty \langle |T|(e_n), e_n \rangle < \infty where T=TT|T| = \sqrt{T^*T}. Trace class operators are compact.

Remark

The hierarchy is: trace class \subset Hilbert-Schmidt \subset compact \subset bounded. Each inclusion is strict, and each class has progressively weaker properties but broader applicability.

Understanding these operator classes is essential for quantum mechanics, where observables are represented by operators and trace class operators correspond to density matrices.