1995
DOI: 10.1103/physreva.51.809
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Theory for the linewidth of a bad-cavity laser

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Cited by 46 publications
(35 citation statements)
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“…); it remains an open problem to obtain a fully general linewidth theory. In this paper, we present a multimode laser-linewidth theory for arbitrary cavity structures and geometries that contains nearly all previously known effects [8][9][10][11][12] and also finds new nonlinear and multimode corrections. The theory is quantitative and makes no significant approximations; it simplifies, in the appropriate limits, to the Schawlow-Townes formula (2) with the well-known corrections.…”
Section: Introductionmentioning
confidence: 99%
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“…); it remains an open problem to obtain a fully general linewidth theory. In this paper, we present a multimode laser-linewidth theory for arbitrary cavity structures and geometries that contains nearly all previously known effects [8][9][10][11][12] and also finds new nonlinear and multimode corrections. The theory is quantitative and makes no significant approximations; it simplifies, in the appropriate limits, to the Schawlow-Townes formula (2) with the well-known corrections.…”
Section: Introductionmentioning
confidence: 99%
“…(This gain-saturation effect is called "spatial hole burning" [4] since it can be spatially inhomogeneous.) In the absence of noise, this results in a stable sinusoidal oscillation with an infinitesimal linewidth, but the presence of noise, which can be modeled by random current fluctuations J [10,29,44], perturbs the mode as depicted in Fig. 1(c), resulting in a finite linewidth.…”
Section: Introductionmentioning
confidence: 99%
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“…The mirrors were separated by 7 cm. A dressed cavity loss rate of ⌫ c /2 ϭ 200 MHz was achieved (''dressed'' means that bad-cavity effects are included 18 ). We varied the laser gain by changing the amplitude V RF of the rf power supply that drives the He-Xe gas discharge.…”
Section: Methodsmentioning
confidence: 99%