Open AccessExperimental verification of deposition rate increase, with maintained high ionized flux fraction, by shortening the HiPIMS pulse
Author(s) -
Tetsuhide Shimizu,
Michal Zanáška,
R P Villoan,
Nils Brenning,
Ulf Helmersson,
Daniel Lundin
Publication year - 2021
Publication title -
plasma sources science and technology
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.9
H-Index - 108
eISSN - 1361-6595
pISSN - 0963-0252
DOI - 10.1088/1361-6595/abec27
Subject(s) - high power impulse magnetron sputtering , analytical chemistry (journal) , ionization , ion , sputter deposition , afterglow , materials science , pulse duration , plasma , chemistry , sputtering , atomic physics , nanotechnology , optics , thin film , laser , physics , organic chemistry , gamma ray burst , quantum mechanics , astronomy , chromatography
High power impulse magnetron sputtering (HiPIMS) is an ionized physical vapor deposition technique, providing a high flux of metal ions to the substrate. However, one of the disadvantages for industrial use of this technique is a reduced deposition rate compared to direct current magnetron sputtering (dcMS) at equal average power. This is mainly due to a high target back-attraction probability of the metal ions with typical values in the range 70%–90% during the pulse. In order to reduce this effect, we focused on the contribution of ion fluxes available immediately after each HiPIMS pulse; a time also known as afterglow. Without a negative potential on the target at this stage of the HiPIMS process, the back-attracting electric field disappears allowing remaining ions to escape the magnetic trap and travel toward the substrate. To quantify the proposed mechanism, we studied the effect of HiPIMS pulse duration on the outward flux of film-forming species in titanium discharges, which are known to exhibit more than 50% reduction in deposition rate compared to dcMS. By shortening the HiPIMS pulse length, it was found that the contribution to the outward flux of film-forming species from the afterglow increases significantly. For example, HiPIMS discharges at a constant peak current density of about 1.10 A cm −2 showed a 45% increase of the deposition rate, by shortening the pulse duration from 200 to 50 μ s. Ionized flux fraction measurements, using a gridless quartz crystal micro-balance-based ion meter, showed that this increase of the deposition rate could be achieved without compromising the ionized flux fraction, which remained approximately constant. The key to the achieved optimization of HiPIMS discharges lies in maintaining a high peak discharge current also for short pulse lengths to ensure sufficient ionization of the sputtered species.