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Auger electron spectroscopy
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Series: ASM Handbook
Volume: 10
Publisher: ASM International
Published: 15 December 2019
DOI: 10.31399/asm.hb.v10.a0006657
EISBN: 978-1-62708-213-6
... Abstract This article discusses the basic principles of and chemical effects in Auger electron spectroscopy (AES), covering various factors affecting the quantitative analyses of AES. The discussion covers instrumentation and sophisticated electronics typically used in AES for data acquisition...
Abstract
This article discusses the basic principles of and chemical effects in Auger electron spectroscopy (AES), covering various factors affecting the quantitative analyses of AES. The discussion covers instrumentation and sophisticated electronics typically used in AES for data acquisition and manipulation and various limitations of AES. Various examples highlighting the capabilities of the technique are also included.
Series: ASM Handbook Archive
Volume: 10
Publisher: ASM International
Published: 01 January 1986
DOI: 10.31399/asm.hb.v10.a0001770
EISBN: 978-1-62708-178-8
... Abstract This article describes the principles and applications of Auger electron spectroscopy (AES). It provides information on the instrumentation typically used in the AES, including an electron gun, an electron spectrometer, a secondary electron detector, and an ion gun. The article also...
Abstract
This article describes the principles and applications of Auger electron spectroscopy (AES). It provides information on the instrumentation typically used in the AES, including an electron gun, an electron spectrometer, a secondary electron detector, and an ion gun. The article also describes experimental methods and limitations of the AES, including elemental detection sensitivity, electron beam artifacts, sample charging, spectral peak overlap, high vapor pressure samples, and sputtering artifacts.
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Published: 15 January 2021
Fig. 1 Auger electron spectroscopy secondary-electron image with a 5 μm field of view (FOV) of the nickel surface after removal of approximately 12 nm of surface contamination
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Published: 01 January 1994
Fig. 1 Auger electron spectroscopy depth profile of polished aluminum alloy 2024-T3 solid solution matrix exposed to Alodine 1200S conversion coating solution for 5 min. Sputter rate approximately 300 Å/min (vs. SiO 2 ). Experiment details in Ref 7 . Source: Ref 4
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Published: 01 January 1994
Fig. 2 Auger electron spectroscopy depth profile of polished aluminum alloy 2024-T3 solid solution matrix exposed for 5 min to the same solution as in Fig. 1 without fluoride ion present. Sputter rate approximately 300 Å/min (vs. SiO 2 ). Experiment details in Ref 7 . Source: Ref 4
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Published: 01 January 1994
Fig. 5 Auger electron spectroscopy of a TiN coating in the derivative mode. At 383 eV, one of the major titanium peaks overlaps with the nitrogen (381 eV) peak. Source: Ref 10
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Published: 01 January 1994
Fig. 6 Factor analysis in Auger electron spectroscopy depth profiling of an oxidized (Cr,Pd)N coating. (a) Standard spectra of the components chromium nitride and chromium oxide. (b) Comparison of measured and synthesized spectra. (c) Depth profile of the principal components. Source: Ref 12
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Published: 01 January 2006
Fig. 5 Auger electron spectroscopy depth profile of a type 316L stainless steel surface. The exposed metal surface is on the left, and the composition with depth from the surface changes as one moves to the right. The base metal composition is reached at approximately 12.5 nm, or 35 atoms
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Published: 01 January 2002
Fig. 2 Auger electron spectroscopy survey spectra obtained from features observed in secondary electron microscopy photo of stainless steel ( Fig. 1 ). Point 1, large particle feature near center of Fig. 3 . Point 2, small particle feature. Point 3, control point off of defects
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Published: 01 January 2002
Fig. 3 Auger electron spectroscopy map of calcium contamination on stainless steel surface. Field of view, 1 μm
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in Adhesion, Friction, and Wear in Low-Pressure and Vacuum Environments
> Friction, Lubrication, and Wear Technology
Published: 31 December 2017
Fig. 2 Auger electron spectroscopy spectra of single-crystal aluminum pin surfaces. (a) Chemically polished surface; 3 keV electron beam. (b) Argon ion sputter-cleaned surface; 3 keV electron beam
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in Adhesion, Friction, and Wear in Low-Pressure and Vacuum Environments
> Friction, Lubrication, and Wear Technology
Published: 31 December 2017
Fig. 3 Auger electron spectroscopy spectra of single-crystal sapphire flat surfaces. (a) As-received surface; 2 keV electron beam. (b) Argon ion sputter-cleaned surface; 3 keV electron beam
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Published: 15 January 2021
Fig. 2 Auger electron spectroscopy survey spectra obtained from features observed in the secondary-electron image. Point 1: nickel surface; Point 2: nodular feature
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Published: 15 January 2021
Fig. 3 Auger electron spectroscopy high-energy-resolution spectra of the (a) silicon KLL and (b) nickel LMM peaks showing the nickel silicide at the interface of the nickel film and silicon wafer
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Published: 15 January 2021
Fig. 4 Auger electron spectroscopy overlay map of the sample surface showing multiple elements: carbon (red), nickel (blue), and silicon (green). FOV, field of view
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Published: 15 January 2021
Fig. 11 Auger electron spectroscopy depth profile using monoatomic argon sputtering through the nickel film. A nickel silicide is observed at the interface.
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Published: 15 December 2019
Fig. 19 Auger electron spectroscopy depth profiles of carbon-beryllium reactions. (a) As-deposited 200 nm carbon on beryllium substrate and after vacuum heating at (b) 450 °C (840 °F) for 30 min, (c) 550 °C (1020 °F) for 30 min, and (d) 600 °C (1110 °F) for 30 min. TZ, transition zone
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Published: 15 December 2019
Fig. 21 Auger electron spectroscopy depth profiles from Nb-SiC couples in the as-deposited condition and upon vacuum annealing at various temperatures and times. Source: Ref 61
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Published: 15 December 2019
Fig. 22 (a) Auger electron spectroscopy depth-profile measurement of Nb-SiC sample annealed at 1200 °C (2190 °F) for 2 h. (b) Silicon and (c) carbon Auger peak shapes at various sputter times (depths) in the profile, showing chemical-state changes. Source: Ref 61
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Published: 15 December 2019
Fig. 33 Auger electron spectroscopy analysis of an in situ fractured low-alloy steel showing (a) ferrite-ferrite boundaries with antimony and nickel enrichment, (b) ferrite-ferrite boundaries with no enrichment of antimony and nickel, (c) chromium-rich carbides, and (d) chromium sulfides
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