phenomenon

optical vortex

A point of zero intensity in a light beam where the phase winds around, creating a corkscrew-like structure.
23 related articles

Description

An optical vortex is a point (or line) in a light beam where the intensity is exactly zero and the phase of the electromagnetic field winds around it in a spiral, like a corkscrew. This phase winding means that the light carries orbital angular momentum (OAM), a property distinct from the spin angular momentum associated with circular polarization. The vortex is a topological defect: the phase change around the singularity is an integer multiple of 2π, and this integer, called the topological charge, is a conserved quantity that cannot be changed by continuous deformations of the field. Optical vortices appear naturally in scattered light, in laser cavities with certain geometries, and can be generated deliberately using spiral phase plates or computer-generated holograms.

History

The concept of optical vortices was introduced in 1974 by John Nye and Michael Berry, who studied wave dislocations in radio waves and acoustics. The first experimental generation of an optical vortex was achieved in 1992 by Les Allen and colleagues, who also recognized that such beams carry orbital angular momentum. This work opened up the field of singular optics.

How it works

The electric field of an optical vortex can be described as E(r, θ) = A(r) e^{ilθ} e^{ikz}, where r is the radial distance, θ is the azimuthal angle, l is the topological charge, and k is the wavevector. At r = 0, the amplitude A(r) vanishes, creating a dark core. The phase e^{ilθ} means that as you go around the beam axis, the phase changes by 2πl, so the wavefronts form a helical surface. This helical structure gives the beam a 'twist' that can transfer angular momentum to particles, causing them to orbit around the vortex core. The dark center is a direct consequence of the phase singularity: the field must be zero there because the phase is undefined.

In practice

Optical vortices are used in optical tweezers to trap and rotate microscopic particles, in high-capacity optical communications where different OAM modes carry independent data streams, and in super-resolution microscopy to enhance imaging resolution beyond the diffraction limit.

Fun fact

The orbital angular momentum of an optical vortex can be transferred to a microscopic particle, causing it to spin around the beam axis — a phenomenon that has been used to create 'optical spanners' that rotate micro-rotors in lab-on-a-chip devices.

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