• 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 zz+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