An ideal laser emits coherent radiation which has a δ-function spectral distribution. Such coherent radiation contains only single-frequency components. In practice, however, a laser emits a quasi-monochromatic radiation which contains a finite spread in its frequency distribution. This frequency spread can be due to spontaneous emission, multi-longitudinal mode operation, as well as other perturbations. Depending on the quality of the laser, this finite spread can range anywhere from zero to multigigahertz.
L. DrescherO. KornilovT. WittingV. ShokeenM. J. J. VrakkingB. Schütte
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