DocumentCode
752873
Title
What is the confocal parameter?
Author
Brorson, Stuart D.
Author_Institution
Dept. of Electr. Eng. & Comput. Sci., MIT, Cambridge, MA, USA
Volume
24
Issue
3
fYear
1988
fDate
3/1/1988 12:00:00 AM
Firstpage
512
Lastpage
515
Abstract
A novel derivation is presented of the Gaussian beam as a limit of the solution to the full wave equation. Usually, the functional form of the Gaussian beam is found by a two-step process. First, the Green´s function of the paraxial wave equation is identified. Then, since the paraxial wave equation is invariant under translation, the z -axis variable is replaced by z +jb . It is shown that when starting with a solution of the full three-dimensional Helmholtz equation in spherical coordinates, performing the transformation z →z +jb corresponds physically to causing the phase fronts of the solution to become ellipsoids. The separation of the foci of the ellipsoids is 2b , where b is the confocal parameter of the beam. In the paraxial limit the ellipsoidal solution becomes a Gaussian beam. Adopting this approach to Gaussian beams allows a simple, geometrical interpretation of the optical resonator stability criterion
Keywords
geometrical optics; wave equations; Gaussian beam; Green´s function; confocal parameter; full three-dimensional Helmholtz equation; full wave equation; optical resonator stability criterion; paraxial wave equation; spherical coordinates; z-axis variable; Ellipsoids; Geometry; Helium; Optical resonators; Partial differential equations; Stability criteria;
fLanguage
English
Journal_Title
Quantum Electronics, IEEE Journal of
Publisher
ieee
ISSN
0018-9197
Type
jour
DOI
10.1109/3.155
Filename
155
Link To Document