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The effect of magnetic field strength and geometry on the deposition rate and ionized flux fraction in the HiPIMS discharge

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    SYSNO ASEP0519372
    Document TypeJ - Journal Article
    R&D Document TypeJournal Article
    Subsidiary JOstatní články
    TitleThe effect of magnetic field strength and geometry on the deposition rate and ionized flux fraction in the HiPIMS discharge
    Author(s) Hajihoseini, H. (IS)
    Čada, Martin (FZU-D) RID, ORCID, SAI
    Hubička, Zdeněk (FZU-D) RID, ORCID, SAI
    Ünaldi, S. (FR)
    Raadu, M.A. (SE)
    Brenning, N. (FR)
    Gudmundsson, J.T. (IS)
    Lundin, D. (FR)
    Number of authors8
    Source TitlePlasma. - : MDPI
    Roč. 2, č. 2 (2019), s. 201-221
    Number of pages21 s.
    Languageeng - English
    CountryCH - Switzerland
    Keywordsionized physical vapor deposition ; magnetron sputtering ; high power impulse magnetron sputtering (HiPIMS) ; ionized flux fraction ; deposition rate
    Subject RIVBL - Plasma and Gas Discharge Physics
    OECD categoryFluids and plasma physics (including surface physics)
    R&D ProjectsEF16_019/0000760 GA MŠMT - Ministry of Education, Youth and Sports (MEYS)
    GA19-00579S GA ČR - Czech Science Foundation (CSF)
    Method of publishingOpen access
    Institutional supportFZU-D - RVO:68378271
    DOI10.3390/plasma2020015
    AnnotationWe explored the effect of magnetic field strength B and geometry (degree of balancing) on the deposition rate and ionized flux fraction Fflux in dc magnetron sputtering (dcMS) and high power impulse magnetron sputtering (HiPIMS) when depositing titanium. The HiPIMS discharge was run in two different operating modes. The first one we refer to as “fixed voltage mode” where the cathode voltage was kept fixed at 625 V while the pulse repetition frequency was varied to achieve the desired time average power (300 W). The second mode we refer to as “fixed peak current mode” and was carried out by adjusting the cathode voltage to maintain a fixed peak discharge current and by varying the frequency to achieve the same average power. Our results show that the dcMS deposition rate was weakly sensitive to variations in the magnetic field while the deposition rate during HiPIMS operated in fixed voltage mode changed from 30% to 90% of the dcMS deposition rate as B decreased.
    WorkplaceInstitute of Physics
    ContactKristina Potocká, potocka@fzu.cz, Tel.: 220 318 579
    Year of Publishing2020
    Electronic addresshttp://hdl.handle.net/11104/0304364
Number of the records: 1  

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