The vibrationally resolved participator Auger spectra of selectively excited C 1s(2σ)−12π1 vibrational states in carbon monoxide

1995 ◽  
Vol 102 (19) ◽  
pp. 7317-7324 ◽  
Author(s):  
S. J. Osborne ◽  
A. Ausmees ◽  
S. Svensson ◽  
A. Kivimäki ◽  
O.‐P. Sairanen ◽  
...  
1996 ◽  
Vol 253 (5-6) ◽  
pp. 377-382 ◽  
Author(s):  
B. Schimmelpfennig ◽  
S.D. Peyerimhoff

1981 ◽  
Vol 111 (3) ◽  
pp. 452-460 ◽  
Author(s):  
M.D. Baker ◽  
N.D.S. Canning ◽  
M.A. Chesters

1991 ◽  
Vol 95 (9) ◽  
pp. 6634-6644 ◽  
Author(s):  
L. S. Cederbaum ◽  
P. Campos ◽  
F. Tarantelli ◽  
A. Sgamellotti

Author(s):  
A. J. Bleeker ◽  
P. Kruit

Combining of the high spatial resolution of a Scanning Transmission Electron Microscope and the wealth of information from the secondary electrons and Auger spectra opens up new possibilities for materials research. In a prototype instrument at the Delft University of Technology we have shown that it is possible from the optical point of view to combine STEM and Auger spectroscopy [1]. With an Electron Energy Loss Spectrometer attached to the microscope it also became possible to perform coincidence measurements between the secondary electron signal and the EELS signal. We measured Auger spectra of carbon aluminium and Argon gas showing energy resolutions better than 1eV [2]. The coincidence measurements on carbon with a time resolution of 5 ns yielded basic insight in secondary electron emission processes [3]. However, for serious Auger spectroscopy, the specimen needs to be in Ultra High Vacuum. ( 10−10 Torr ). At this moment a new setup is in its last phase of construction.


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