A new method for generation of a discharge in its own metal vapour of
an r.f.-excited electrode is described. The method is based on the r.f
. plasma jet (RPJ) system utilizing a small size r.f. nozzle in which
a hollow cathode-type discharge is generated. The nozzle outlet (targe
t) is sputtered and/or evaporated by the ion bombardment from the jet
discharge. The power density at the nozzle outlet reaches the order of
hundreds of watts per square centimetre even at reasonably low r.f. p
ower supply levels (above 100 W). A dense plasma containing a large am
ount of the nozzle metal ions can be generated inside the nozzle. Depe
nding on the nozzle material, at a definite critical value of the r.f.
power the discharge character can change to a particular kind of arc
(RPJ arc) in which metal ejection inside the self-heated nozzle is suf
ficient to generate a sustained discharge without any auxiliary gas. E
xperiments indicate that the generation of the RPJ arc can be consider
ed as a combination of a distributed discharge (diffuse) arc and a hig
h voltage arc. Optical emission spectra from an Mg RPJ generated plasm
a exhibit only Mg emission lines and Mg film growth rate reaches value
s above 4 mum min-1. Conditions for generation of self-sustained disch
arges in Ti and Cu nozzles are also discussed. The effect of the nozzl
e geometry on the generation of stable self-sustained discharges for d
eposition of thin films is explained. In most cases an enhanced thermi
onic electron emission from the metallic surface contributes to a posi
tive feedback to maintain the dense metal vapour plasma discharge. Dep
osition of Ti films in a plasma containing Ti vapours, Ti+ ions and lo
w partial pressure of Ar at regimes close to the RPJ arc is described.