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The Rayleigh length (or Rayleigh range) of a laser beam is the distance from the beam waist (in the propagation direction) where the beam radius is increased by a factor of the square root of 2. For a circular beam, this means that the mode area is doubled at this point.
For Gaussian beams, the Rayleigh length is determined by the waist radius w0 and the wavelength λ:
where the wavelength λ is the vacuum wavelength divided by the refractive index n of the material.
For beams with imperfect beam quality and a given waist radius, the Rayleigh length is effectively decreased by the so-called M2 factor. This implies that such beams have a larger beam divergence for a given beam waist radius.
The effective Rayleigh length is a convenient quantity for calculations in the context of focused laser beams. Essentially, it determines the depth of focus. There can thus be a trade-off between a more strongly focused beam with higher optical intensity in the focus, and a less strongly focused beam with longer Rayleigh length, i.e. larger depth of focus. For example, the highest laser gain in a laser medium can be achieved when the focused pump beam has a Rayleigh length of the order of the length of the gain medium: weaker focusing reduces the pump intensity, whereas stronger focusing leads to a strong divergence, which limits the effective interaction length. Similar arguments apply to nonlinear interactions, e.g. frequency doubling, even though some more sophisticated aspects such as the Gouy phase shift come into play in such situations, where phase matching is important.
The article on laser beams contains a paragraph titled “Limitations for the Focusing of Laser Beams”, where the effective Rayleigh length plays an important role.
The older literature often uses the confocal parameter b, which is two times the Rayleigh length.
See also: Gaussian beams, laser beams, collimated beams, Gouy phase shift, beam quality, M2 factor, wavelength
and other articles in the category general optics
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