Low energy electron microscopy of surface processes

Vacuum ◽  
1990 ◽  
Vol 41 (1-3) ◽  
pp. 5-10 ◽  
Author(s):  
E Bauer ◽  
M Mundschau ◽  
W Swiech ◽  
W Telieps
Keyword(s):  
Electron Microscopy ◽  
Low Energy ◽  
Energy Electron ◽  
Surface Processes ◽  
Low Energy Electron

Low Energy Electron Microscopy of Surface Processes on Clean Si(111) and Si (100)

1989 ◽  
Vol 159 ◽  
Author(s):  
E. Bauer ◽  
M. Mundschau ◽  
W. Swiech ◽  
W. Telieps
Keyword(s):  
Electron Microscopy ◽  
Phase Transitions ◽  
Crystal Growth ◽  
Surface Defects ◽  
Low Energy ◽  
Energy Electron ◽  
Surface Processes ◽  
Surface Phase ◽  
Surface Phase Transitions ◽  
Low Energy Electron

ABSTRACTLow energy electron microscopy (LEEM) is briefly introduced and its application to the study of surface defects, surface phase transitions on Si(111), crystal growth and sublimation on Si(100) is illustrated.

The potential of the scanning low energy electron microscopy for the examination of aluminum based alloys and composites

Microscopy ◽  
2005 ◽  
Vol 54 (2) ◽  
pp. 109-117 ◽  
Author(s):  
Kenji Matsuda ◽  
Susumu Ikeno ◽  
Ilona Müllerová ◽  
Luděk Frank
Keyword(s):  
Electron Microscopy ◽  
Low Energy ◽  
Energy Electron ◽  
Low Energy Electron

Spin Polarized Low Energy Electron Microscopy (Spleem) of Single and Combined Layers of Co, Cu, and Pd on W (110)

1993 ◽  
Vol 313 ◽  
Author(s):  
Helmut Poppa ◽  
Heiko Pinkvos ◽  
Karsten Wurm ◽  
Ernst Bauer
Keyword(s):  
Electron Microscopy ◽  
Band Structure ◽  
Film Growth ◽  
Magnetic Domain ◽  
Low Energy ◽  
Energy Electron ◽  
Magnetic Studies ◽  
Deposition Rates ◽  
Spin Polarized ◽  
Low Energy Electron

ABSTRACTIn-situ recording of ultra-thin film growth by Low Energy Electron Microscopy (LEEM) results in accurate determinations of monolayer metal deposition rates for difficult to calibrate deposition geometries. Deposition rates and growth features were determined for Cu and Co on W (110) allowing for thickness control at the submonolayer level. Also, the transparencies of non-Magnetic overlayers of Pd (111) and Cu (111) to very low energy spin polarized electrons were compared and qualitatively explained by band structure considerations. Cu (111) is much more transparent than Pd (111) so that magnetic domain structures can be observed through at least 4 nmof Cu (111). This suggests the use of Cu (111) and other metals of suitable band structure as protective layers for surface magnetic studies.

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