Hamiltonian operator
Builds on ObservableStone's theorem on one-parameter unitary groupsUnitary operatorSchrödinger operatorSchrödinger equationMomentum operatorPosition operator
Definition
Let , and let be the complex Hilbert space of a quantum system. The Hamiltonian of the system is a self-adjoint operator on , the observable of total energy, that generates the time evolution. A state vector at time becomes at time .
Remarks
By Stone's theorem, is a strongly continuous one-parameter group of unitary operators, and every such group arises from exactly one self-adjoint . For , the curve is differentiable and solves the abstract Schrödinger equation .
Consider a particle of mass in with a real potential . Its Hamiltonian is built from the momentum operators and the position operators: It is the Schrödinger operator of the Schrödinger equation. One must check that it is self-adjoint on a suitable domain; for a bounded measurable this holds on the domain of the Laplacian, the Sobolev space .
Example: for a free particle on , . The Fourier transform turns it into multiplication by , a real function, so is self-adjoint with spectrum .
Non-example: the operator on is not self-adjoint. It would give , which is not unitary and makes the norm of a state vector grow.
Reading path
To understand this page from the ground up, read these 27 pages in order. The foundations come first.
Show the path as a graph
- no evidence level
- Adjoint of an unbounded operator concept
- Borel sigma-algebra concept
- Continuous functional calculus concept
- Densely defined operator concept
- Hilbert space concept
- Hilbert space adjoint concept
- Identity matrix object
- Matrix definition
- Momentum operator concept
- Observable concept
- Position operator concept
- Projection-valued measure concept
- Schrödinger equation concept
- Schrödinger operator concept
- Self-adjoint operator concept
- Spectrum of an operator concept
- Unbounded operator concept
- Unitary operator concept
- Transpose definition
- Conjugate transpose definition
- Normal matrix definition
- Unitary matrix definition
- Spectral theorem for normal matrices statement
- Spectral theorem for bounded normal operators statement
- Spectral theorem for unbounded self-adjoint operators statement
- Stone's theorem on one-parameter unitary groups statement
- Hamiltonian operator definition
Further reading
About this page
| Tag | F5252H0MFD |
|---|---|
| URI | m2://F5252H0MFD |
| Kind | definition |
| Writing | W0 stub |
| MSC | 81Q10, 47B25, 81Q05 |
| Defines | Hamiltonian operator |
| Uses | Observable, Stone's theorem on one-parameter unitary groups, Unitary operator, Schrödinger operator, Schrödinger equation, Momentum operator, Position operator |
| Changed | 3 November 2026 |
Markdown · JSON · Edit on GitHub
What this page needs for W1
- an inventory row: the row of the inventory that the node accounts for (0 of 1)
- a source with a locator (0 of 1)
The writing levels say how complete the text of a page is. They do not measure its truth.
What links here
No page links to this page yet.