Ordinary differential equations Definition
Schrödinger operator
Builds on LaplacianOrdinary differential equation
Definition
Let be an open interval and let be locally integrable. The one-dimensional Schrödinger operator with potential is the differential expression acting on functions such that and are locally absolutely continuous. More generally, for an open set and a real function on , the Schrödinger operator is , where is the Laplacian. The equation with is the time-independent Schrödinger equation.
Remarks
Example: for and , the function has . So , and solves the Schrödinger equation with . Non-example: is not a Schrödinger operator in this sense, because the potential is not real. In units where Planck's constant and the mass are normalised, is the energy operator of a quantum particle. To get a self-adjoint operator on one must also fix boundary conditions at the ends of when they are needed.
Reading path
To understand this page from the ground up, read these 13 pages in order. The foundations come first.
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- no evidence level
- Euclidean space object
- Function concept
- Ordinary differential equation concept
- Total derivative concept
- Function of several variables concept
- Vector-valued function concept
- Differentiable function of several variables concept
- Partial derivative concept
- Vector field concept
- Gradient concept
- Divergence concept
- Laplacian concept
- Schrödinger operator definition
Further reading
About this page
| Tag | W6QS1ME39J |
|---|---|
| URI | m2://W6QS1ME39J |
| Kind | definition |
| Writing | W0 stub |
| MSC | 34L40, 35J10, 81Q10 |
| Defines | Schrödinger operator |
| Uses | Laplacian, Ordinary differential equation |
| Changed | 2 November 2026 |
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