Hellinger–Toeplitz theorem
Statement
Let be a linear operator defined on the entire Hilbert space (not just a dense subspace) that is symmetric, meaning . Then is automatically bounded.
Why is it true?
This is the theorem that explains why unbounded operators are unavoidable in quantum mechanics: physically important symmetric operators like position, momentum, and the Hamiltonian genuinely cannot be defined on every vector of (only on a dense domain), because if they were, this theorem would force them to be bounded — but they demonstrably are not.
Proof sketch
We use the closed graph theorem (a standard consequence of the Baire category theorem): a linear operator defined on all of a Hilbert space is bounded if and only if its graph is closed in , i.e. whenever and , we must have .
Suppose and . We must show . For any fixed , symmetry gives for every .
Taking on both sides: the left side because and the inner product is continuous; the right side because . So (using symmetry once more on the right).
Since holds for every , we get for all ; taking gives , so . The graph of is therefore closed, and the closed graph theorem concludes is bounded.
Topics that use this theorem
Step-by-step proofs
No step-by-step proof yet for this theorem.
References
- Michael Reed, Barry Simon (1980). Methods of Modern Mathematical Physics I: Functional Analysis
- John B. Conway (2000). A Course in Operator Theory
- Werner Kirsch (2008). An Invitation to Random Schrödinger Operators · arXiv:0709.3707