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Coherence length

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Title: Coherence length  
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Coherence length

In physics, coherence length is the propagation distance over which a coherent wave (e.g. an electromagnetic wave) maintains a specified degree of coherence. Wave interference is strong when the paths taken by all of the interfering waves differ by less than the coherence length. A wave with a longer coherence length is closer to a perfect sinusoidal wave. Coherence length is important in holography and telecommunications engineering.

This article focuses on the coherence of classical electromagnetic fields. In quantum mechanics, there is a mathematically analogous concept of the quantum coherence length of a wave function.


In radio-band systems, the coherence length is approximated by

L={c \over n\, \Delta f},

where c is the speed of light in a vacuum, n is the refractive index of the medium, and \Delta f is the bandwidth of the source.

In optical communications, the coherence length L is given by [1]

L={2 \ln(2) \over \pi n} {\lambda^2 \over \Delta\lambda},

where \lambda is the central wavelength of the source, n is the refractive index of the medium, and \Delta\lambda is the spectral width of the source. If the source has a Gaussian spectrum with FWHM spectral width \Delta\lambda, then a path offset of ±L will reduce the fringe visibility to 50%.

Coherence length is usually applied to the optical regime.

The expression above is a frequently used approximation. Due to ambiguities in the definition of spectral width of a source, however, the following definition of coherence length has been suggested:

The coherence length can be measured using a Michelson interferometer and is the optical path length difference of a self-interfering laser beam which corresponds to a 1/e=37\% fringe visibility,[2] where the fringe visibility is defined as

V = {I_\max - I_\min \over I_\max + I_\min} ,\,

where I is the fringe intensity.

In long-distance transmission systems, the coherence length may be reduced by propagation factors such as dispersion, scattering, and diffraction.


Multimode helium–neon lasers have a typical coherence length of 20 cm, while the coherence length of singlemode ones can exceed 100 m. Semiconductor lasers reach some 100 m. Singlemode fiber lasers with linewidths of a few kHz can have coherence lengths exceeding 100 km. Similar coherence lengths can be reached with optical frequency combs due to the narrow linewidth of each tooth. Non-zero visibility is present only for short intervals of pulses repeated after cavity length distances up to this long coherence length.

See also


  1. ^ Drexler, Fujimoto (2008). Optical Coherence Tomography. Springer Berlin Heidelberg.  
  2. ^ Ackermann, Gerhard K. (2007). Holography: A Practical Approach. Wiley-VCH.  
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