Optics, electromagnetic theory Definition
Optical vortex
Builds on Winding numberLaguerre–Gaussian modes
Definition
Let be a continuous complex scalar field on an open set , the transverse plane of a beam. Let be an isolated zero of . Take a small circle around inside on which has no zero. Let be the winding number around of the closed curve . So is the total change of along . The point is an optical vortex if , and is its topological charge.
Remarks
The integer does not depend on the choice of the small circle, by continuity of the winding number. A continuous field with a nonzero winding number around must vanish at , which is why vortices are dark points. In space, the zeros of a field generically form lines, called vortex lines.
Example: with equals in polar coordinates. Its only zero is the origin, and increases by around it, so the origin is a vortex of charge . The Laguerre–Gaussian mode with has a vortex of charge on its axis.
Non-example: vanishes at the origin, but it is real and positive elsewhere. Its phase is constant, so the winding number is and the origin is not a vortex.
Reading path
To understand this page from the ground up, read these 3 pages in order. The foundations come first.
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- no evidence level
- Laguerre–Gaussian modes concept
- Winding number concept
- Optical vortex definition
Further reading
About this page
| Tag | 6T5GT2RMWB |
|---|---|
| URI | m2://6T5GT2RMWB |
| Kind | definition |
| Writing | W0 stub |
| MSC | 78A10, 78A60 |
| Defines | Optical vortex |
| Uses | Winding number, Laguerre–Gaussian modes |
| Changed | 3 November 2026 |
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