Wüest M. 51 Wykes M. 82 Yamaguchi M. 17 Ybarra G. 129 Yubero F ...
Wüest M. 51 Wykes M. 82 Yamaguchi M. 17 Ybarra G. 129 Yubero F ...
Wüest M. 51 Wykes M. 82 Yamaguchi M. 17 Ybarra G. 129 Yubero F ...
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JUNE 28 WEDNESDAY AFTERNOON<br />
RIVA-SS-WeA-P.1 TiCr ALLOYS OF LOW SECONDARY ELECTRON EMISSION<br />
FOR ANTIMULTIPACTOR APPLICATIONS. G. G. Fuentes and R. J. Rodríguez, AIN-Centro<br />
de Ingeniería Avanzada de Superficies, Cordovilla, 31191, Pamplona, Spain. L. Galán, Departamento<br />
de Física Aplicada. Universidad Autónoma de Madrid. Cantoblanco. 28049-Madrid. Spain. I.<br />
Montero and J. L. Segovia, Instituto de Ciencia de Materiales de Madrid. CSIC. Cantoblonco.<br />
28049-Madrid. Spain<br />
TiCr alloys of low secondary electron emission have been investigated as potential anti-multipactor<br />
coatings. Cathodic-arc evaporation technique in Ar atmosphere was used. The ion energy can be<br />
controlled by the substrate biasing. Chemical state analysis and surface composition were obtained<br />
by X-ray Photoemission Spectroscopy (XPS). Depth profiling was performed by Glow Discharge<br />
Optical Emission Spectroscopy (GDOES). Scanning Electron Microscopy images show the formation<br />
of grains on the surface. The film composition is homogeneous, however, the composition of the<br />
grains varied with their size. Larger grains are richer in titanium, while small ones are rich in chromium<br />
as indicated by energy Dispersive X-ray analysis. Total secondary electron emission yield was<br />
determined by measuring the sample current to ground when bombarded by a primary electron beam<br />
of determined energy. The secondary electron emission coefficient of TiCr alloy exposed to air was<br />
lower than those of chromium or titanium coatings and their nitrides. The experimental secondary<br />
emission yield values together with a Montecarlo model of the secondary emission process were<br />
used to obtain the multipactor threshold.<br />
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