The increase of the target power density causes not only the depositio
n rate increase, but also gives the possibility of introducing a new w
ay of magnetron sputtering. With high sputtering rates, the secondary
ions of sputtered metal begin to play an important role. In the extrem
e case, the discharge can be sustained with secondary ions only in a s
o-called 'pure' self-sputtering. When this phenomenon occurs the magne
tron sputtering process can go on at the final pressure of the vacuum
set, (i.e. 4 x 10(-4) Pa). If means that during self-sputtering (SSS)
sustained on metal ions the contamination by inert gas particles has b
een eliminated. The author has proposed an observation of the relation
between the minimum values of the target current, (target current den
sity, target power density) and the working gas (argon) pressure, at w
hich the discharge still exists, as an 'instrument' of the SSS effect.
The paper presents a relation I-Tmin (i(Tmin); P-Tmin) versus P-wmin,
which was measured during Cu, Ag, Ti, Ni, Ta, Al and stainless steel
sputtering. The current-voltage characteristics have been measured. Th
e 'pure' SSS effect has been observed during Cu, Ta, Ag and stainless
steel sputtering. For other materials, the target current increase cau
sed a decrease of the sputtering process pressure. Planar magnetrons o
f very high efficiency were used. Targets of 50, 100 and 200 mm in dia
meter were sputtered at power densities up to 300 W/cm(2).