Abstract
To obtain laser action it is necessary not only to have an appropriate population inversion but also to ensure that the rate of stimulated emission, which depends on the intensity of the local radiation field, is high compared with loss mechanisms. This condition can often be met in pulsed systems even in the absence of a resonator, in so-called “mirrorless” lasers. In cw lasers, however, a resonator is invariably necessary to increase the intensity of radiation which is “circulating” in the laser medium; the intensity of the circulating radiation can be calculated by multiplying the output intensity of the laser by the inverse of the transmission coefficient of the output coupling optics.
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Douglas, N.G. (1989). Wavelength and Frequency Measurements. In: Millimetre and Submillimetre Wavelength Lasers. Springer Series in Optical Sciences, vol 61. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-540-46095-4_3
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DOI: https://doi.org/10.1007/978-3-540-46095-4_3
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