2012
DOI: 10.1088/0957-0233/23/10/105901
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A desktop supersonic free-jet beam source for a scanning helium microscope (SHeM)

Abstract: A simple design for an inexpensive, compact, desktop-sized helium free-jet beam source is described. The apparatus, which is Campargue-like in design and utilizes mostly off-the-shelf parts, is capable of producing a centreline intensity of 1.2 × 1019 atoms per second per steradian. The beam performance was investigated using a conventional ion gauge and a stagnation detector, with the latter being used to produce beam flux profiles. The profile of the macroskimmed beam has been experimentally demonstrated to … Show more

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Cited by 17 publications
(8 citation statements)
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References 21 publications
(28 reference statements)
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“…See Fig. 3 Around the same time as Witham and Sánchez, Barr et al had worked on a pinhole microscope with a slightly different design, using a skimmer in combination with a collimating pinhole aperture [34]. For a detailed discussion of different helium microscope designs see Section 6.…”
Section: Some Background Historymentioning
confidence: 99%
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“…See Fig. 3 Around the same time as Witham and Sánchez, Barr et al had worked on a pinhole microscope with a slightly different design, using a skimmer in combination with a collimating pinhole aperture [34]. For a detailed discussion of different helium microscope designs see Section 6.…”
Section: Some Background Historymentioning
confidence: 99%
“…In a Neutral Helium Microscope, atoms start their journey in the source. A typical SHeM source follows the design established for helium atom scattering (HAS) [36,34,37]: helium is accelerated in a supersonic expansion from a high pressure reservoir through a de-Laval nozzle 2 , into a vacuum chamber, known as the expansion chamber [38]. There, the central part of the beam is selected by a conically shaped aperture, called the skimmer 3 .…”
Section: The Helium Sourcementioning
confidence: 99%
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“…[10] and fig. 1 by Barr et al [14] small skimmers (often known as 'microskimmers' [15]) can be used to reduce the source size, but their narrow geometry means atoms backscattered into the beam from either the leading edge, or the internal skimmer walls, risks affecting the beam intensity significantly. An alternative is to introduce a second aperture behind the skimmer that, provided the volume is adequately pumped, will set the source size of the instrument whilst minimising additional beam interference [16].…”
Section: Free Jet Expansionmentioning
confidence: 99%
“…The source operates in an intermediate pressure regime [10] and consists of a nozzle (10 μm aperture) based on the design of Buckland et al [11] and a Beam Dynamics skimmer (100 μm aperture) that is used to sample the centerline atoms (producing the collimated beam) and separate the source chamber from the remainder of the apparatus. The nozzle can be moved with respect to the skimmer with an x-y-z manipulator (UHV Designs) and the pressure behind the nozzle, known as the stagnation pressure, can be controlled with a resolution of 1 bar.…”
Section: Design Of a Pinhole Shemmentioning
confidence: 99%