1989
DOI: 10.1007/bf00694192
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Polarization properties and frequency stabilization of an internal mirror He-Ne laser emitting at 543.5 nm wavelength

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Cited by 19 publications
(2 citation statements)
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“…As light source we employed a continuous randomly polarized He-Ne laser of 5 mW and wavelength 543 nm (Melles-Griot 05-LGR-193). These are He-Ne lasers with internal mirrors attached to the tube, which operate at two orthogonally linearly polarized modes where the orientation of the linear state rapidly changes in time on a nanosecond scale, thus resulting in a light source with random polarization [43]. In all experiments, the laser was left turned on for at least one hour to achieve a stable output.…”
Section: Methodsmentioning
confidence: 99%
“…As light source we employed a continuous randomly polarized He-Ne laser of 5 mW and wavelength 543 nm (Melles-Griot 05-LGR-193). These are He-Ne lasers with internal mirrors attached to the tube, which operate at two orthogonally linearly polarized modes where the orientation of the linear state rapidly changes in time on a nanosecond scale, thus resulting in a light source with random polarization [43]. In all experiments, the laser was left turned on for at least one hour to achieve a stable output.…”
Section: Methodsmentioning
confidence: 99%
“…The light source is a cw randomly polarized He-Ne laser of 5 mW and wavelength 543 nm (Melles-Griot 05-LGR-193). These are He-Ne lasers with internal mirrors attached to the tube, which operate at two orthogonally linearly polarized modes where the orientation of the linear state rapidly changes in time on a nanosecond scale, thus resulting in a light source with random polarization [14].…”
Section: Geometric Phase Grating Polarization State Generatormentioning
confidence: 99%