Compact Operators - Main Theorem
The Spectral Theorem for Compact Self-Adjoint Operators extends the diagonalization of symmetric matrices to infinite dimensions, providing a complete understanding of their structure.
Let be a separable Hilbert space and a compact self-adjoint operator. Then:
- All eigenvalues of are real
- Eigenvectors corresponding to distinct eigenvalues are orthogonal
- There exists an orthonormal basis of consisting of eigenvectors of
- The eigenvalues satisfy and
- For any ,
This theorem shows that compact self-adjoint operators are "diagonalizable" with respect to an orthonormal basis, just like finite-dimensional symmetric matrices.
The proof proceeds by constructively finding eigenvalues and eigenvectors:
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Let . There exists a unit vector with
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Consider and restrict to . Since is self-adjoint,
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Repeat the process on to find and , then continue inductively
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Compactness ensures
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The span of is dense in , giving an orthonormal basis
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Sturm-Liouville Problems: The operator on with appropriate boundary conditions has compact resolvent, so its eigenvalue problem has complete orthonormal solutions
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Vibrating String: Normal modes of a vibrating string are eigenfunctions of a compact self-adjoint operator
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Heat Equation: Solutions can be expanded in eigenfunctions:
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Quantum Mechanics: Energy eigenstates of certain Hamiltonians form complete orthonormal systems
This theorem is one of the most important results in functional analysis. It provides the theoretical foundation for Fourier series, quantum mechanics, and the solution of PDEs via separation of variables and eigenfunction expansions.
The spectral theorem transforms abstract operator theory into concrete computations with eigenvalues and eigenvectors.