Rayleigh length

In optics and especially laser science, the Rayleigh length or Rayleigh range, , is the distance along the propagation direction of a beam from the waist to the place where the area of the cross section is doubled.[1] A related parameter is the confocal parameter, b, which is twice the Rayleigh length.[2] The Rayleigh length is particularly important when beams are modeled as Gaussian beams.

Gaussian beam width as a function of the axial distance . : beam waist; : confocal parameter; : Rayleigh length; : total angular spread

ExplanationEdit

For a Gaussian beam propagating in free space along the   axis with wave number  , the Rayleigh length is given by [2]

 

where   is the wavelength (the vacuum wavelength divided by  , the index of refraction) and   is the beam waist, the radial size of the beam at its narrowest point. This equation and those that follow assume that the waist is not extraordinarily small;  .[3]

The radius of the beam at a distance   from the waist is [4]

 

The minimum value of   occurs at  , by definition. At distance   from the beam waist, the beam radius is increased by a factor   and the cross sectional area by 2.

Related quantitiesEdit

The total angular spread of a Gaussian beam in radians is related to the Rayleigh length by[1]

 

The diameter of the beam at its waist (focus spot size) is given by

 .

These equations are valid within the limits of the paraxial approximation. For beams with much larger divergence the Gaussian beam model is no longer accurate and a physical optics analysis is required.

See alsoEdit

ReferencesEdit

  1. ^ a b Siegman, A. E. (1986). Lasers. University Science Books. pp. 664–669. ISBN 0-935702-11-3.
  2. ^ a b Damask, Jay N. (2004). Polarization Optics in Telecommunications. Springer. pp. 221–223. ISBN 0-387-22493-9.
  3. ^ Siegman (1986) p. 630.
  4. ^ Meschede, Dieter (2007). Optics, Light and Lasers: The Practical Approach to Modern Aspects of Photonics and Laser Physics. Wiley-VCH. pp. 46–48. ISBN 3-527-40628-X.