CHEM02200704003 Nilamadhab Pandhy - Homi Bhabha National ...
CHEM02200704003 Nilamadhab Pandhy - Homi Bhabha National ...
CHEM02200704003 Nilamadhab Pandhy - Homi Bhabha National ...
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Chapter 3<br />
various industrial applications because of, (a) its simplicity and reliability, (b) capability for<br />
operating in different physical conditions, (3) sputtering sources can be designed up to industrial<br />
scale, and (4) as an alternative to meet the functional and economical industrial requirements<br />
compared to the traditional process. Moreover, the process limitations in conventional sputtering<br />
process, such as low deposition rate, low ionisation efficiency in plasma, and substrate heating<br />
effect is not encountered in magnetron sputtering. Today, magnetron sputtering technology is<br />
largely used in different applications such as (a) decorative coating on items in everyday life such<br />
as jewellery and glasses (b) in semi-conductor industries for application in Si integrated circuits,<br />
and (c) to improve the surface properties of base material particularly wear, load bearing and<br />
corrosion resistance etc [58-60]. The driving force for the fast development of magnetron<br />
sputtering technology is due to the requirement of advanced thin films with prescribed physical<br />
and functional properties in many diverse technological applications.<br />
The basic sputtering process has been known for many years. In the basic sputtering<br />
process, a target (cathode) is bombarded by energetic ions generated in a glow discharge plasma<br />
situated in front of the plasma. The bombardment process causes the removal i.e. sputtering of the<br />
target atoms, which may then condense as a thin film on the substrate. However, secondary<br />
electrons are also generated from the target surface as a result of ion bombardment and these<br />
electrons do not significantly contribute in maintaining the plasma and cause unnecessary heating<br />
of the substrate.<br />
Magnetrons make use of the fact that a magnetic field configured parallel to the target<br />
surface can constrain secondary electron motion to the vicinity of the target [61,62]. The<br />
schematic of magnetron sputtering is shown in Fig. 3.2 [62]. The magnets are arranged in such a<br />
way that one pole is placed at the central axis of the target and the second pole is formed by a ring<br />
of magnets arranged around the outer edge of the target.