ICMCTF2006 Session H3: High Power Impulse Magnetron Sputtering (HIPIMS)

Monday, May 1, 2006 2:30 PM in Room Terrace Pavilion

Monday Afternoon

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Start Invited? Item
2:30 PM H3-4 Progress in Characterization of High-Power Pulsed DC Magnetron Discharges for Ionized High-Rate Sputtering of Films
J. Vlcek, P. Kudlacek, A.D. Pajdarova, J. Lukas, J. Musil (University of West Bohemia, Czech Republic)
High-power pulsed dc magnetron discharges for ionized high-rate sputtering of metallic films were systematically investigated. The depositions were performed using unbalanced circular magnetrons of newly designed types with a directly water-cooled planar copper or titanium target of 100mm in diameter. The magnetron was driven by a pulsed dc power supply working in the frequency range from 0.5 to 50kHz with a maximum pulse voltage and maximum pulse current of 1kV and 120A, respectively. Time evolution of the magnetron voltage, the target current density (up to 1.5Acm-2) and the ion current density on the substrate (up to 0.45 and 0.15Acm-2 in the distance of 100 and 200mm, respectively) was measured to provide information on plasma conductivity, sputtering yield and total ion flux to the substrate. The deposition rate and the substrate ion current density per unit discharge power input were determined to investigate efficiency of magnetron sputtering, and formation and transfer of ions to the substrate, respectively. Time-resolved plasma diagnostics was carried out using optical emission spectroscopy, energy-resolved mass spectroscopy and Langmuir probe measurements to understand complex time-dependent processes in pulsed magnetron discharges. Time-averaged mass spectroscopy was performed at the substrate position to characterize ion energy distributions and composition of the total ion fluxes to the substrate over a wide range of conditions. Trends in the measured values of the deposition rate per unit discharge power input and the ionized fraction of sputtered particles in the flux to the substrate were explained on the basis of model predictions.
3:10 PM H3-6 Effect of Energetic HIPIMS Plasma on the Microstructure of TiN Thin Film
J. Bohlmark (Linköping University, Sweden); H. Stranning (Linköping University and Sandvik Tooling, Sweden); T.I. Selinder (Sandvik Tooling, Sweden); M. Lattemann, U. Helmersson (Linköping University, Sweden)
One of the important features with the high power impulse magnetron sputtering (HIPIMS) discharge is that it can be utilized for effective bombardment of the growing film by ions of the deposition species themselves. This is partly due to the high degree of ionization of the sputtered species that can be accelerated to the film, but also due to a higher intrinsic kinetic energy of the ions in the HIPIMS plasma as compared to conventional dc magnetron sputtering (dcMS). The ion energy, Ei, distributions recorded from the HIPIMS discharge are broad with a large fraction of highly energetic ions (about 50 % with Ei > 20 eV). The effect of the highly ionized conditions in combination with the large number of highly energetic ions was demonstrated using reactive deposition of TiN thin films onto substrates held at a floating potential. The obtained films showed a denser microstructure with a smoother surface for the HIPIMS case compared to films grown under similar conditions using dcMS. The observed preferential orientation for the HIPIMS films showed a (111) preferred orientation, similar to films grown using arc evaporations, while the dcMS produced films with a (100) orientation.
3:30 PM H3-7 Titanium Oxide Thin Films Deposited by High-Power Pulsed Magnetron Sputtering
S. Konstantinidis, J.P. Dauchot (Materia Nova, Belgium); M. Hecq (University of Mons-Hainaut, Belgium)

Ionized physical vapour deposition processes are of great interest for surface modification because the flexibility of the thin film deposition process can be increased by ionizing the metallic vapour.

Recently, High-Power Pulsed Magnetron (HPPM) discharges have been implemented to achieve high degree of ionization (≥50%). Nevertheless, the technique has to face a major problem: the deposition rate is minimized compared to conventional DC magnetron discharges. To overcome this drawback, a High-Power Pulsed Magnetron generator has been designed@footnote 1@ allowing to "calibrate" the pulse length with the deposition conditions. Pulse length is shortened in order to minimize the self-sputtering effect responsible of the decrease of the deposition rate ; the ionization degree of the metallic vapour being still significant.

This way, titanium oxide thin films have been deposited on glass and steel substrates using a 450 x 150 mm rectangular titanium target in argon-oxygen atmosphere. The average power delivered to the plasma is ranging between 1.5 and 2kW and peak current and voltages obtained are respectively reaching 200A and 900V.

Films are characterized using Scanning Electron Microscopy, X-Ray Diffraction and Optical Transmission Spectroscopy. One of the major findings is the presence of a pure rutile phase on steel substrates (even without substrate bias) and the significant increase of the refractive index of the films deposited on glass compared to thin films deposited via conventional DC pulsed magnetron sputtering.

super 1@ M. Ganciu, M. Hecq, S. Konstantinidis, J.P. Dauchot, M. Touzeau, L. de Poucques, J. Bretagne, Eur. Patent Appl. n°4447072.2 / 22.03.2004.

3:50 PM H3-8 The Advantages and Disadvantages of High Power Pulsed Magnetron Sputtering
W.D. Sproul (Reactive Sputtering Consulting, LLC)

High power pulsed magnetron sputtering (HPPMS), which applies a very large power pulse to the target for a short period of time, results in a very high degree of ionization of the sputtered species. Typical peak power densities are on the order of 1,000 to 3,000 W per square centimeter with pulse durations of 100-150 microseconds. HPPMS is very much like the cathodic are process where there is a very high degree of ionization of the evaporant, but there are few if no droplets with HPPMS. The potential of HPPMS is to use these ionized species to improve the structure and properties of the deposited film. Alami et al.1 have shown that the ionized species follow field lines to a biased substrate producing a dense film in side wall features, and Petrov et al.2 have shown that for films grown with high ion-to- neutral ratios for the arriving species at the substrate a low bias voltages can be used to give fully dense films with low stress. HPPMS should allow the deposition of thick films. The major disadvantage of the HPPMS process is that its deposition rate is only 25-30% of the rate for an equivalent amount of power used during conventional DC sputtering. A model by Christie3 has been developed to explain this loss of rate for the HPPMS process, and the model provides insights that hopefully will bring a solution to this loss of rate issue. In this talk, the advantages and disadvantages for HPPMS as it is practiced today will be reviewed, and the needs to make this technology a commercial reality will be discussed.

1 J. Alami, P. O. Ã.. Persson, D. Music, J. T. Gudmundsson, J. Bohlmark, and U. Helmersson, J. Vac. Sci. Technol. A, 23 (2005) 278.

2 I. Petrov, P. B. Barna, L. Hultman, and J. E. Greene, Microstructural evolution during film growth, J. Vac. Sci. Technol. A, 21 (2003) S117.

3 D. J. Christie, J. Vac. Sci. Technol. A, 23 (2005) 330.

4:30 PM H3-10 Interface Microstructure Engineering by High Power Impulse Magnetron Sputtering for the Enhancement of Adhesion
A.P. Ehiasarian, C. Reinhard, P.Eh. Hovsepian (Sheffield Hallam University, United Kingdom); J.G. Wen, I. Petrov (University of Illinois at Urbana-Champaign)

An excellent adhesion of hard coatings to steel substrates is paramount in practically all application areas. Conventional methods utilise Ar glow etching or arc discharge pretreatments that have the disadvantage of producing weak interfaces or adding droplets respectively.

A new tool for interface engineering is high power impulse magnetron sputtering (HIPIMS). HIPIMS is based on conventional sputtering with extremely high peak power densities reaching 3 kWcm-2 at current densities of >2 Acm-2. HIPIMS of Cr and Nb was used to prepare interfaces on 304 stainless steel and M2 high speed steel (HSS). During the pretreatment, the substrates were biased to -600 V and -1000 V in the environment of a HIPIMS plasma. The bombarding flux density reached peak values of >100 mAcm-2 and consisted of highly ionised metal plasma containing a high proportion of Cr1+ and Nb1+ but also doubly charged metal ions Cr2+ and Nb2+ as observed by optical emission spectroscopy. The adhesion was evaluated for a coating consisting of a 0.5 µm thick CrN base layer and a 2.5 µm thick nanoscale multilayer stack of CrN/NbN with bilayer thickness of 3.4 nm with typical hardness of HK0.025 = 3100 and residual stress of -1.8 GPa. In the case of Cr HIPIMS pretreatment, the adhesion values on M2 HSS reached scratch test critical load values of LC = 70 N thus comparing well to LC = 51 N for interfaces pretreated by arc discharge plasmas. Cross-sectional transmission electron microscopy studies revealed a clean interface and large areas of epitaxial growth. The orientation of the coating grains was observed to change together with the orientation of the grains in the polycrystalline steel substrate. Due to the droplet-free pretreatment by HIPIMS, large scale defects in the coating are minimised and the protection capabilities of the coating against wear and corrosion are enhanced.

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