2018
DOI: 10.1063/1.5029385
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Fast resolution change in neutral helium atom microscopy

Abstract: In neutral helium atom microscopy, a beam of atoms is scanned across a surface. Though still in its infancy, neutral helium microscopy has seen a rapid development over the last few years. The inertness and low energy of the helium atoms (less than 0.1 eV) combined with a very large depth of field and the fact that the helium atoms do not penetrate any solid material at low energies open the possibility for a non-destructive instrument that can measure topology on the nanoscale even on fragile and insulating s… Show more

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Cited by 6 publications
(4 citation statements)
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“…That is to say O 2 S is the image of the source at the sample. For the zone plate microscope it is the demagnified image of the skimmer or the source limiting aperture [77], σ A is the Airy disk contribution from edge diffraction from the zone plate or pinhole and σ cm is a chromatic aberration term that appears for the case of the zone plate. The first equation holds under the assumption that the Fresnel number is smaller than 1, which is the case for the limit of small pinholes.…”
Section: Helium Optics / Resolution Limitsmentioning
confidence: 99%
See 1 more Smart Citation
“…That is to say O 2 S is the image of the source at the sample. For the zone plate microscope it is the demagnified image of the skimmer or the source limiting aperture [77], σ A is the Airy disk contribution from edge diffraction from the zone plate or pinhole and σ cm is a chromatic aberration term that appears for the case of the zone plate. The first equation holds under the assumption that the Fresnel number is smaller than 1, which is the case for the limit of small pinholes.…”
Section: Helium Optics / Resolution Limitsmentioning
confidence: 99%
“…2.2.3. This design has the additional advantage that it enables fast resolution change by changing in-situ between different collimating apertures [77].…”
Section: Microscopes With Micro-skimmersmentioning
confidence: 99%
“…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%
“…Contrast in scanning helium microscopy has similarities with the origins of contrast in scanning electron microscopy, both of which involve rastering a focused or collimated beam across the sample and the collection of a fraction of the backscattered signal. In the case of helium atoms, a narrow spot can be generated via simple pinhole collimation, as used in the current work; 3 via diffractive focusing with a Fresnel zone plate or similar; [6][7][8] or through the use of atom mirrors. [9][10][11][12] Since the local surface position and orientation affect the resulting distribution of scattered particles, topographic contrast is evident in both cases.…”
mentioning
confidence: 99%