Related Experiment Video
Updated: Sep 11, 2025

12:14
The Generation of Higher-order Laguerre-Gauss Optical Beams for High-precision Interferometry
Published on: August 12, 2013
21.9K
Generalized Airy derivative transform of a Gaussian beam
Optics Express
|August 13, 2025
Summary
A new generalized Airy derivative transform extends beam generation capabilities beyond conventional Airy beams. This method offers an alternative pathway for creating specific light beams with controllable propagation characteristics.
Area of Science:
- Optics and Photonics
- Beam Shaping and Transformation
Background:
- The conventional Airy transform converts Gaussian beams into Airy beams.
- The need exists for generating a broader range of specific beams.
Purpose of the Study:
- To propose a generalized Airy derivative transform.
- To extend the functionality of Airy transforms for generating diverse beams.
Main Methods:
- Derivation of analytical expressions for beam characteristics (center of mass, spot dimension, divergence, M-square factor) using light intensity moments.
- Investigation of transformed Gaussian beam propagation in free space.
- Experimental demonstration of the first-order Airy derivative transform.
Main Results:
- The generalized Airy derivative transform includes the conventional Airy transform as a zeroth-order case.
- Transformed Gaussian beams exhibit ballistic trajectories during free-space propagation.
- The light field during propagation is a sum of Airy function derivatives with modified weighting factors.
Conclusions:
- The generalized Airy derivative transform provides a versatile method for generating specific beams.
- Experimental realization is straightforward and generalizable.
- This broadens the applicability of Airy transforms in optics.
Related Concept Videos
Deflection of a Beam
374
Accurately determining beam deflection and slope under various loading conditions in structural engineering is crucial for ensuring safety and structural integrity. Singularity functions offer a streamlined approach to analyzing beams, especially when multiple loading functions complicate the bending moment equation.
Singularity functions, described in an earlier lesson, are powerful mathematical tools that represent discontinuities within a function commonly encountered in structural loading...
Singularity functions, described in an earlier lesson, are powerful mathematical tools that represent discontinuities within a function commonly encountered in structural loading...
374
Elastic Curve from the Load Distribution
256
The structural behavior of beams under distributed loads is critical for engineering analysis, which focuses on predicting how beams bend and react under such conditions. Different types of beams (e.g., cantilever, supported, or overhanging) behave differently under distributed load conditions.
For all beams, the analysis of the beam's reaction to distributed loads begins by understanding the relationship between a beam's load and the resulting shear forces and bending moments.
For all beams, the analysis of the beam's reaction to distributed loads begins by understanding the relationship between a beam's load and the resulting shear forces and bending moments.
256
Gauss's Law
7.9K
If a closed surface does not have any charge inside where an electric field line can terminate, then the electric field line entering the surface at one point must necessarily exit at some other point of the surface. Therefore, if a closed surface does not have any charges inside the enclosed volume, then the electric flux through the surface is zero. What happens to the electric flux if there are some charges inside the enclosed volume? Gauss's law gives a quantitative answer to this question.
7.9K
Gauss's Law: Planar Symmetry
8.3K
A planar symmetry of charge density is obtained when charges are uniformly spread over a large flat surface. In planar symmetry, all points in a plane parallel to the plane of charge are identical with respect to the charges. Suppose the plane of the charge distribution is the xy-plane, and the electric field at a space point P with coordinates (x, y, z) is to be determined. Since the charge density is the same at all (x, y) - coordinates in the z = 0 plane, by symmetry, the electric field at P...
8.3K
Gauss's Law: Cylindrical Symmetry
8.0K
A charge distribution has cylindrical symmetry if the charge density depends only upon the distance from the axis of the cylinder and does not vary along the axis or with the direction about the axis. In other words, if a system varies if it is rotated around the axis or shifted along the axis, it does not have cylindrical symmetry. In real systems, we do not have infinite cylinders; however, if the cylindrical object is considerably longer than the radius from it that we are interested in,...
8.0K
Gauss's Law: Spherical Symmetry
7.9K
A charge distribution has spherical symmetry if the density of charge depends only on the distance from a point in space and not on the direction. In other words, if the system is rotated, it doesn't look different. For instance, if a sphere of radius R is uniformly charged with charge density ρ0, then the distribution has spherical symmetry. On the other hand, if a sphere of radius R is charged so that the top half of the sphere has a uniform charge density ρ1 and the bottom half...
7.9K

