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Chromium and titanium film deposition using a hot refractory anode vacuum arc plasma source

โœ Scribed by I.I. Beilis; A. Shnaiderman; R.L. Boxman


Publisher
Elsevier Science
Year
2008
Tongue
English
Weight
480 KB
Volume
203
Category
Article
ISSN
0257-8972

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โœฆ Synopsis


The radially expanding plasma jet generated in a Hot Refractory Anode Vacuum Arc (HRAVA) was used to deposit thin chromium and titanium films on glass substrates. The arc was sustained between a water-cooled cylindrical cathode and a non-consumed cylindrical tungsten anode separated by a 10 mm gap, for time periods up to 120 s, operating with a current (I) of 200-300 A. The chromium cathode was 30 mm diameter and 20 mm height, and was used with 32 mm diameter, 30 mm height anode. The titanium cathode was 60 mm diameter, 25 mm height and was used with a 60 mm diameter, 15 mm height anode. Thin films were deposited on glass substrates exposed to the anodic plasma. A mechanical shutter controlled the deposition onset and exposure duration time. The distance from the arc axis to the substrate (L) was varied between 80 and 145 mm. The film thickness was measured by a profilometer, and macro-particles (MP) presence on the coating surface was examined by optical microscopy. It was found that the deposition rate of Cr films increased with arc current and reached ~1.4 ยตm/min at I =300 A, L = 80 mm. The total MP flux was less than 1 mm -2 min -1 for I =300 A, L = 110 mm. The deposition rate of Ti films reached 1.8 ยตm/min at I = 300 A, L = 100 mm.


๐Ÿ“œ SIMILAR VOLUMES


Metallic film deposition using a vacuum
โœ Isak I. Beilis; Raymond L. Boxman ๐Ÿ“‚ Article ๐Ÿ“… 2009 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 994 KB

Conventional metallic film deposition techniques are compared with the hot refractory anode vacuum arc (HRAVA) developed in the last decade. In the HRAVA process, the anode is heated by the arc, and a dense plasma plume of cathode material is formed by re-evaporation of cathode material from the ano