2006
DOI: 10.7498/aps.55.4086
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Experimental study of laser collimation of Cr beam

Abstract: Laser collimation of Cr atomic beam using a transverse Doppler cooling scheme is studied. The frequency of laser is stabilized at 5±0.26MHz below the 7S3→7PO452Cr transition. The shortest size of the laser cooling beam is computed theoretically to be 13.7mm. Accordingly a Cr beam was collimated using a transverse Doppler cooling scheme. We obtained that the transverse distribution of Cr beam is less than 1/3 of the uncooled beam.

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Cited by 7 publications
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“…3 ) using a laser-induced fluorescence technique with stability less than 0.28 MHz (< 2π × 5 MHz). [15] Optical potential Result All depositions were carried out in a turbomolecular pumped vacuum system with typical pressure 10 −5 Pa. The chromium atomic beam is produced by thermal evaporation out of an orifice (Φ = 1 mm) of a ceramic crucible in a molecular beam epitaxy oven at 1650 • C. This leads to a typical deposition rate of 0.0125 nm/s at a distance of 0.8 m. Using Doppler cooling, a well collimated atomic beam with a divergence of <1 mrad is obtained.…”
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“…3 ) using a laser-induced fluorescence technique with stability less than 0.28 MHz (< 2π × 5 MHz). [15] Optical potential Result All depositions were carried out in a turbomolecular pumped vacuum system with typical pressure 10 −5 Pa. The chromium atomic beam is produced by thermal evaporation out of an orifice (Φ = 1 mm) of a ceramic crucible in a molecular beam epitaxy oven at 1650 • C. This leads to a typical deposition rate of 0.0125 nm/s at a distance of 0.8 m. Using Doppler cooling, a well collimated atomic beam with a divergence of <1 mrad is obtained.…”
mentioning
confidence: 99%
“…A detailed investigation of the transverse laser cooling of 52 Cr was described in Ref. [15]. The experimental setup of laser-focused atomic deposition is shown in Fig.…”
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