1992
DOI: 10.1016/0039-6028(92)90167-5
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Surface dynamics of ordered Cu3Au(001) studied by elastic and inelastic helium atom scattering

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Cited by 49 publications
(28 citation statements)
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“…The apparatus has been described in detail elsewhere. 40 Briefly, helium was expanded through a 20 m nozzle source that was cooled by a closed-cycle helium refrigerator to generate a nearly monochromatic ͑⌬v / v Յ 1%͒ supersonic neutral atom beam. Primarily, a 46 meV beam ͑wave vector, k i = 9.4 Å −1 ; nozzle temperature, T n ϳ 213 K͒ was used for the experiments, while a 17.5 meV beam ͑k i = 5.73 Å −1 and T n ϳ 81 K͒ was employed for measurements of the specular angular width.…”
Section: Materials and Experimental Methodsmentioning
confidence: 99%
“…The apparatus has been described in detail elsewhere. 40 Briefly, helium was expanded through a 20 m nozzle source that was cooled by a closed-cycle helium refrigerator to generate a nearly monochromatic ͑⌬v / v Յ 1%͒ supersonic neutral atom beam. Primarily, a 46 meV beam ͑wave vector, k i = 9.4 Å −1 ; nozzle temperature, T n ϳ 213 K͒ was used for the experiments, while a 17.5 meV beam ͑k i = 5.73 Å −1 and T n ϳ 81 K͒ was employed for measurements of the specular angular width.…”
Section: Materials and Experimental Methodsmentioning
confidence: 99%
“…24 The crystal-to-ionizer distance was however shortened from 1.0234 m to 0.5705 m, which when added to a constant chopper-to-crystal distance of 0.4996 m, produced a total flight path of 1.0701 m (shortened from a total distance of 1.5230 m for the long mode). Inelastic helium time-of-flight experiments (described below) were performed with the detector in both configurations, providing greater angular resolution in the long mode, whereas greater intensity was produced in the short mode.…”
Section: Methodsmentioning
confidence: 99%
“…26 The apparatus consisted of three regions: a differentially pumped beam source, a UHV sample chamber, and a rotatable detector arm with a total flight path of 1.0778 m (chopperto-crystal distance of 0.4996 m, crystal-to-ionizer distance of 0.5782 m). A nearly mono-energetic beam of atoms ( v/v ≤ 1%, FWHM) was produced by the supersonic expansion of helium through a nozzle source, the center of which was captured by a conical skimmer and collimated by two apertures into a 4 mm spot at the sample.…”
Section: B Helium Atom Scattering Techniquesmentioning
confidence: 99%