CrNx Films Prepared by DC Magnetron Sputtering and High-Power Pulsed Magnetron Sputtering : A Comparative Study

CrNx (0 ≤ x ≤ 0.91) films synthesized using highpower pulsed magnetron sputtering, also known as high-power impulse magnetron sputtering (HiPIMS), have been compared with those made by conventional direct-current (dc) magnetron sputtering (DCMS) operated at the same average power. The HiPIMS deposition rate relative to the DCMS rate was found to decrease linearly with increasing emission strength from the Cr ions relative to Cr neutrals, in agreement with the predictions of the target-pathway model. The low deposition rate in HiPIMS is thus a direct consequence of the high ionization level (∼56%) of the target material and effective capturing of Cr ions by the cathode potential. Although the HiPIMS deposition rate did not exceed 40% of the DCMS rate, the drop in the relative deposition rate upon increasing the N2-to-Ar flow ratio, fN2/Ar , was found to be similar for both sputtering techniques. Films prepared by HiPIMS contained similar amounts of atomic nitrogen as the dc-sputtered samples grown at the same fN2/Ar , indicating that the nitride formation at the substrate takes place mostly during the time period of the high-power pulses, and the N2 uptake between the pulses is negligible. The microstructure evolution in the two types of CrNx films, however, differed clearly from each other. A combination of a high substrate bias and a high flux of doubly charged Cr ions present during the HiPIMS discharge led to a disruption of the grain growth and renucleation, which resulted in column-free films with nanosized grains not observed in the conventional DCMS-based process. The comparison of nanoindentation hardness as a function of fN2/Ar revealed superior properties of HiPIMS-sputtered films in the entire range of gas compositions.

[1]  L. Hultman,et al.  Microstructure control of CrNx films during high power impulse magnetron sputtering , 2010 .

[2]  E. Wallin,et al.  Cross-field ion transport during high power impulse magnetron sputtering , 2008 .

[3]  U. Helmersson,et al.  Ionized physical vapor deposition (IPVD): A review of technology and applications , 2006 .

[4]  J. Musil,et al.  High-power pulsed sputtering using a magnetron with enhanced plasma confinement , 2007 .

[5]  A. Anders Deposition rates of high power impulse magnetron sputtering: Physics and economics , 2010 .

[6]  W. Sproul,et al.  The structure and properties of chromium nitride coatings deposited using dc, pulsed dc and modulated pulse power magnetron sputtering , 2010 .

[7]  P. Kelly,et al.  Magnetron sputtering: a review of recent developments and applications , 2000 .

[8]  C. Mitterer,et al.  Microstructure and mechanical/thermal properties of Cr–N coatings deposited by reactive unbalanced magnetron sputtering , 2001 .

[9]  P. Sigmund Sputtering of single and multiple component materials , 1980 .

[10]  R. Snyders,et al.  The physical reason for the apparently low deposition rate during high-power pulsed magnetron sputtering , 2008 .

[11]  J. Schneider,et al.  A novel pulsed magnetron sputter technique utilizing very high target power densities , 1999 .

[12]  S. Konstantinidis,et al.  Titanium oxide thin films deposited by high-power impulse magnetron sputtering , 2006 .

[13]  W. Münz,et al.  A new method for hard coatings: ABSTM (arc bond sputtering) , 1992 .

[14]  J. Alami,et al.  Spatial electron density distribution in a high-power pulsed magnetron discharge , 2005, IEEE Transactions on Plasma Science.

[15]  L. Hultman,et al.  Time and energy resolved ion mass spectroscopy studies of the ion flux during high power pulsed magnetron sputtering of Cr in Ar and Ar/N2 atmospheres , 2010 .

[16]  C. Christou,et al.  Ionization of sputtered material in a planar magnetron discharge , 2000 .

[17]  W. Sproul,et al.  High Power Pulsed Reactive Sputtering of Zirconium Oxide and Tantalum Oxide , 2004 .

[18]  L. Hultman,et al.  Comparison of microstructure and mechanical properties of chromium nitride-based coatings deposited by high power impulse magnetron sputtering and by the combined steered cathodic arc/unbalanced magnetron technique , 2004 .

[19]  I. Petrov,et al.  High power pulsed magnetron sputtered CrNX films , 2003 .

[20]  C. Reinhard,et al.  Influence of the bias voltage on the structure and mechanical performance of nanoscale multilayer CrAlYN∕CrN physical vapor deposition coatings , 2009 .

[21]  D. Christie Target material pathways model for high power pulsed magnetron sputtering , 2005 .

[22]  Matthias Wuttig,et al.  On the relationship between the peak target current and the morphology of chromium nitride thin films deposited by reactive high power pulsed magnetron sputtering , 2009 .

[23]  U. Helmersson,et al.  The ion energy distributions and ion flux composition from a high power impulse magnetron sputtering discharge , 2006 .

[24]  Arutiun P. Ehiasarian,et al.  Ionization of sputtered metals in high power pulsed magnetron sputtering , 2005 .

[25]  G. Pharr,et al.  An improved technique for determining hardness and elastic modulus using load and displacement sensing indentation experiments , 1992 .

[26]  Jeffrey Hopwood,et al.  Ionized physical vapor deposition , 2000 .

[27]  K. Bobzin,et al.  Mechanical properties and oxidation behaviour of (Al,Cr)N and (Al,Cr,Si)N coatings for cutting tools deposited by HPPMS , 2008 .

[28]  C. Reinhard,et al.  CrAlYN/CrN superlattice coatings deposited by the combined high power impulse magnetron sputtering/unbalanced magnetron sputtering technique , 2006 .

[29]  A. Matthews,et al.  Structure, mechanical and tribological properties of nitrogen-containing chromium coatings prepared by reactive magnetron sputtering , 1999 .

[30]  W. Münz,et al.  Structure and mechanical properties of CrN/TiN multilayer coatings prepared by a combined HIPIMS/UBMS deposition technique , 2008 .

[31]  Erik René Kieft,et al.  Refinement of Monte Carlo simulations of electron–specimen interaction in low-voltage SEM , 2008 .

[32]  M. Kiuchi,et al.  The formation of chromium/nitrogen phases by nitrogen ion implantation during chromium deposition as a function of ion-to-atom arrival ratio , 1997 .

[33]  D. B. Lewis,et al.  Chromium nitride coatings grown by unbalanced magnetron (UBM) and combined arc/unbalanced magnetron (ABS™) deposition techniques , 1996 .

[34]  S. Konstantinidis,et al.  High power pulsed magnetron sputtering: A review on scientific and engineering state of the art , 2010 .

[35]  M. W. Thompson Physical mechanisms of sputtering , 1981 .