Math 2.0

Optics, electromagnetic theory Definition

Optical vortex

Builds on Winding numberLaguerre–Gaussian modes

Definition

Let U ⁣:Ω→ℂU \colon \Omega \to \C be a continuous complex scalar field on an open set Ω⊆ℝ2\Omega \subseteq \R^2, the transverse plane of a beam. Let p∈Ωp \in \Omega be an isolated zero of UU. Take a small circle CC around pp inside Ω\Omega on which UU has no zero. Let ℓ\ell be the winding number around 00 of the closed curve U∘CU \circ C. So 2πℓ2\pi\ell is the total change of arg⁡U\arg U along CC. The point pp is an optical vortex if ℓ≠0\ell \ne 0, and ℓ\ell is its topological charge.

Remarks

The integer ℓ\ell 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 pp must vanish at pp, which is why vortices are dark points. In space, the zeros of a field U(x,y,z)U(x, y, z) generically form lines, called vortex lines.

Example: U(x,y)=(x+iy)ℓe−(x2+y2)U(x, y) = (x + iy)^\ell e^{-(x^2 + y^2)} with ℓ≥1\ell \ge 1 equals rℓe−r2eiℓφr^\ell e^{-r^2} e^{i\ell\varphi} in polar coordinates. Its only zero is the origin, and arg⁡U=ℓφ\arg U = \ell\varphi increases by 2πℓ2\pi\ell around it, so the origin is a vortex of charge ℓ\ell. The Laguerre–Gaussian mode LGpℓ\mathrm{LG}_{p\ell} with ℓ≠0\ell \ne 0 has a vortex of charge ℓ\ell on its axis.

Non-example: U(x,y)=x2+y2U(x, y) = x^2 + y^2 vanishes at the origin, but it is real and positive elsewhere. Its phase is constant, so the winding number is 00 and the origin is not a vortex.

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  1. Laguerre–Gaussian modes concept
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Further reading

  1. Web https://en.wikipedia.org/wiki/Optical_vortex
About this page
Tag6T5GT2RMWB
URIm2://6T5GT2RMWB
Kinddefinition
WritingW0 stub
MSC78A10, 78A60
DefinesOptical vortex
UsesWinding number, Laguerre–Gaussian modes
Changed3 November 2026

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