scholarly journals Low-energy plasmons in quantum-well and surface states of metallic thin films

2011 ◽  
Vol 84 (16) ◽  
Author(s):  
V. M. Silkin ◽  
T. Nagao ◽  
V. Despoja ◽  
J. P. Echeverry ◽  
S. V. Eremeev ◽  
...  
Keyword(s):  
Thin Films ◽  
Quantum Well ◽  
Surface States ◽  
Low Energy ◽  
Metallic Thin Films

scholarly journals Metallic thin films on stepped surfaces: lateral scattering of quantum well states

2014 ◽  
Vol 16 (12) ◽  
pp. 123025 ◽  
Author(s):  
F Schiller ◽  
Z M Abd El-Fattah ◽  
S Schirone ◽  
J Lobo-Checa ◽  
M Urdanpilleta ◽  
...  
Keyword(s):  
Thin Films ◽  
Quantum Well ◽  
Metallic Thin Films ◽  
Stepped Surfaces ◽  
Quantum Well States

scholarly journals Adsorption Capacity of Metallic Thin Films after Bombarding by Low-Energy Ar$^{+}$ Ions

2020 ◽  
Vol 42 (5) ◽  
pp. 621-630
Author(s):  
M. O. Vasylyev ◽  
◽  
S. I. Sidorenko ◽  
I. O. Kruhlov ◽  
D. I. Trubchaninova ◽  
...  
Keyword(s):  
Thin Films ◽  
Adsorption Capacity ◽  
Low Energy ◽  
Metallic Thin Films

Rocking Beam Microarea Diffraction Applied to Metallic thin Films

1976 ◽  
Vol 34 ◽  
pp. 396-397
Author(s):  
R. H. Geiss
Keyword(s):  
Thin Films ◽  
Electron Diffraction ◽  
Small Area ◽  
Objective Lens ◽  
Electron Optics ◽  
Metallic Thin Films ◽  
Transmission Electron Diffraction ◽  
Transmission Electron ◽  
Sample Height ◽  
Scanning Transmission

The theory and practical limitations of micro area scanning transmission electron diffraction (MASTED) will be presented. It has been demonstrated that MASTED patterns of metallic thin films from areas as small as 30 Åin diameter may be obtained with the standard STEM unit available for the Philips 301 TEM. The key to the successful application of MASTED to very small area diffraction is the proper use of the electron optics of the STEM unit. First the objective lens current must be adjusted such that the image of the C2 aperture is quasi-stationary under the action of the rocking beam (obtained with 40-80-160 SEM settings of the P301). Second, the sample must be elevated to coincide with the C2 aperture image and its image also be quasi-stationary. This sample height adjustment must be entirely mechanical after the objective lens current has been fixed in the first step.

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