In theory, collimated light does not disperse with distance. Really, collimated light will disperse a little as it travels over distance. Diffraction prevents scientists from creating a perfectly collimated beam with no divergence.
Light can be roughly collimated by using a collimator – a device which narrows a beam of particles or waves.
Etymology[change | change source]
Sources[change | change source]
Lasers[change | change source]
Laser light from crystal and some gas lasers is highly collimated because it is formed in an optical cavity between two parallel mirrors, in addition to being coherent. The divergence of high-quality laser beams is commonly less than 1 milliradian, and can be much less for large-diameter beams. Laser diodes emit less collimated light due to their short cavity, and therefore higher collimation requires a collimating lens.
Synchrotron light[change | change source]
Distant sources[change | change source]
Lenses and mirrors[change | change source]
A perfect parabolic mirror will bring parallel rays to a focus at a single point. Conversely, a point source at the focus of a parabolic mirror will produce a beam of collimated light. Since the source needs to be small, such an optical system cannot produce much optical power. Spherical mirrors are easier to make than parabolic mirrors and they are often used to produce approximately collimated light. Many types of lenses can also produce collimated light from point-like sources.
References[change | change source]
- Lewis, Charlton T. (2010). "collimo". A Latin Dictionary. Oxford; Medford: Clarendon Press; Perseus Digital Library.
- Pfister, J. & Kneedler, J.A. (s.d.). A guide to lasers in the OR.