Jove
Visualize
Contact Us
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Concept Videos

Conservation of Angular Momentum: Application01:18

Conservation of Angular Momentum: Application

A system's total angular momentum remains constant if the net external torque acting on the system is zero. Examples of such systems include a freely spinning bicycle tire that slows over time due to torque arising from friction, or the slowing of Earth's rotation over millions of years due to frictional forces exerted on tidal deformations. However in the absence of a net external torque, the angular momentum remains conserved. The conservation of angular momentum principle requires a change...
Conservation of Angular Momentum01:09

Conservation of Angular Momentum

A system's total angular momentum remains constant if the net external torque acting on the system is zero. Considering a system that consists of n tiny particles, the angular momentum of any tiny particle may change, but the system's total angular momentum would remain constant. The principle of conservation of angular momentum only considers the net external torque acting on the system. While there are internal forces exerted by different particles within the system that also produce internal...
Angular Momentum about an Arbitrary Axis01:11

Angular Momentum about an Arbitrary Axis

Imagine a rigid body with a mass denoted as 'm', which has its center of mass at point G and is rotating around an inertial reference frame. The angular momentum at an arbitrary point P can be calculated by taking the cross product of the position vector and linear momentum vector for each individual mass element.
The velocity of a mass element comprises its translational velocity and the relative velocity instigated by the body's rotation. Substituting the velocity equation into the angular...
Angular Momentum: Single Particle01:10

Angular Momentum: Single Particle

Angular momentum is directed perpendicular to the plane of the rotation, and its magnitude depends on the choice of the origin. The perpendicular vector joining the linear momentum vector of an object to the origin is called the “lever arm.” If the lever arm and linear momentum are collinear, then the magnitude of the angular momentum is zero. Therefore, in this case, the object rotates about the origin such that it lies on the rim of the circumference defined by the lever arm magnitude.
The...

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

Unifying methods for optimal control in non-Markovian quantum systems via process tensors.

The Journal of chemical physics·2024
Same author

Cross Determination of Exciton Coherence Length in J-Aggregates.

The journal of physical chemistry letters·2022
Same author

Device for inductive heating and focusing of laser produced plasma.

The Review of scientific instruments·2019
Same author

Tuning behaviour of slotted vernier widely tunable lasers.

Optics express·2019
Same author

A Front Line Club Suggested.

The Hospital·2018
Same author

Mechanism of large optical nonlinearity in gold nanoparticle films.

Optics letters·2018

Related Experiment Video

Updated: Jun 10, 2026

The Generation of Higher-order Laguerre-Gauss Optical Beams for High-precision Interferometry
12:14

The Generation of Higher-order Laguerre-Gauss Optical Beams for High-precision Interferometry

Published on: August 12, 2013

Generation of continuously tunable fractional optical orbital angular momentum using internal conical diffraction.

D P O'Dwyer1, C F Phelan, Y P Rakovich

  • 1School of Physics, Trinity College Dublin, Dublin 2, Ireland.

Optics Express
|August 20, 2010
PubMed
Summary

This study explores internal conical diffraction in biaxial crystals, demonstrating an all-optical method to generate light beams with fractional orbital angular momentum (OAM) using elliptically polarized light.

More Related Videos

A Photonic System for Generating Unconditional Polarization-Entangled Photons Based on Multiple Quantum Interference
07:56

A Photonic System for Generating Unconditional Polarization-Entangled Photons Based on Multiple Quantum Interference

Published on: September 5, 2019

Direct Imaging of Laser-driven Ultrafast Molecular Rotation
10:52

Direct Imaging of Laser-driven Ultrafast Molecular Rotation

Published on: February 4, 2017

Related Experiment Videos

Last Updated: Jun 10, 2026

The Generation of Higher-order Laguerre-Gauss Optical Beams for High-precision Interferometry
12:14

The Generation of Higher-order Laguerre-Gauss Optical Beams for High-precision Interferometry

Published on: August 12, 2013

A Photonic System for Generating Unconditional Polarization-Entangled Photons Based on Multiple Quantum Interference
07:56

A Photonic System for Generating Unconditional Polarization-Entangled Photons Based on Multiple Quantum Interference

Published on: September 5, 2019

Direct Imaging of Laser-driven Ultrafast Molecular Rotation
10:52

Direct Imaging of Laser-driven Ultrafast Molecular Rotation

Published on: February 4, 2017

Area of Science:

  • Optics and Photonics
  • Condensed Matter Physics

Background:

  • Gaussian light beams with spin angular momentum (SAM) exhibit unique diffraction patterns in biaxial crystals.
  • Internal conical diffraction of circularly polarized light results in a superposition of Bessel-like beams with distinct SAM and orbital angular momentum (OAM) properties.

Purpose of the Study:

  • To investigate the internal conical diffraction of elliptically polarized light in biaxial crystals.
  • To demonstrate an all-optical method for generating light beams with tunable fractional orbital angular momentum (OAM).

Main Methods:

  • Incident elliptically polarized Gaussian light beams along the optic axis of a biaxial crystal.
  • Analysis of the resulting hollow cone of light and its constituent Bessel-like beams.
  • Characterization of spin and orbital angular momentum properties of the generated beams.

Main Results:

  • Elliptically polarized light undergoes internal conical diffraction, producing a hollow cone beam.
  • The emergent beam is a superposition of zero and first-order Bessel-like beams with different polarizations and OAM.
  • An all-optical process is demonstrated to generate light beams with fractional OAM up to +/- 1h.

Conclusions:

  • Internal conical diffraction in biaxial crystals offers a versatile platform for manipulating light's angular momentum.
  • The study presents a novel all-optical method for generating fractional OAM beams, with potential applications in optical manipulation and communication.