2001
DOI: 10.1063/1.1405795
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Construction of a low velocity metastable helium atomic beam

Abstract: A bright metastable atom source at 80 K Rev. Sci. Instrum. 72, 2558 (2001); 10.1063/1.1372169 Continuous, dense, highly collimated sodium beam Rev. Sci. Instrum. 71, 3668 (2000)We have constructed an atomic beam of metastable helium atoms He͑2 3 S) with a mean velocity of 300 m/s ͑15 K͒ and a yield of 3ϫ10 12 atoms/s sr. The metastable atoms are produced in a dc discharge in a cryogenic environment cooled by liquid helium. Using a hexapole magnetic lens, we have increased further the beam intensity by focusing… Show more

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Cited by 18 publications
(15 citation statements)
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“…This is achieved by transverse collimation of the beam of metastable atoms using two-dimensional (2D) transverse radiative pressure forces (Aspect et al, 1990;Hoogerland et al, 1996b;Metcalf and van der Straten, 1999;Morita and Kumakura, 1991;Partlow et al, 2004;Rasel et al, 1999;Rooijakkers et al, 1996;Shimizu et al, 1987Shimizu et al, , 1990Vansteenkiste et al, 1991), focussing in a hexapole (Woestenenk et al, 2001) or 2D magneto-optical compression (Labeyrie et al, 1999;Schiffer et al, 1997;Scholz et al, 1994). For maximum efficiency, the collimation zone, which has a typical length of several to a few tens of cm, has to be implemented as close as possible to the source, typically directly after the skimmer.…”
Section: B Intense and Slow Beams Of Metastable Atomsmentioning
confidence: 99%
See 1 more Smart Citation
“…This is achieved by transverse collimation of the beam of metastable atoms using two-dimensional (2D) transverse radiative pressure forces (Aspect et al, 1990;Hoogerland et al, 1996b;Metcalf and van der Straten, 1999;Morita and Kumakura, 1991;Partlow et al, 2004;Rasel et al, 1999;Rooijakkers et al, 1996;Shimizu et al, 1987Shimizu et al, , 1990Vansteenkiste et al, 1991), focussing in a hexapole (Woestenenk et al, 2001) or 2D magneto-optical compression (Labeyrie et al, 1999;Schiffer et al, 1997;Scholz et al, 1994). For maximum efficiency, the collimation zone, which has a typical length of several to a few tens of cm, has to be implemented as close as possible to the source, typically directly after the skimmer.…”
Section: B Intense and Slow Beams Of Metastable Atomsmentioning
confidence: 99%
“…4). The source is cooled by liquid nitrogen (Kawanaka et al, 1993) or in some cases even by liquid helium (Aspect et al, 1988;Carnal and Mlynek, 1991;Swansson et al, 2004;Woestenenk et al, 2001) for a reduction of the initial mean velocity of the resulting atomic beam.…”
Section: A Discharge Sourcesmentioning
confidence: 99%
“…There were several attempts to combine a nozzle with electrical or laser discharge scheme to produce these species. In most cases the excitation process warms the supersonic jet, or contaminates it with sputtered electrode material [47][48][49][50][51][52]. We have developed a new type of electrode less Dielectric Barrier Discharge [53][54][55][56] source that does not heat the jet or contaminates it [57].…”
Section: Ionic Clusters and Radical Sourcesmentioning
confidence: 99%
“…8 These methods are somewhat cumbersome, however, and in addition do not work for the heavier RGs since these would simply condense at such low temperatures.…”
Section: Introductionmentioning
confidence: 99%