journal article·2018-12-28Open access

Control over the Phase Formation in Metastable Transition Metal Nitride Thin Films by Tuning the Al+ Subplantation Depth

Grzegorz Greczynski, Stanislav Mráz, Marcus Hans, Jun Lu, Lars Hultman, Jochen M. Schneider

Coatings· Volume 9· Issue 1

Abstract

The performance of transition metal nitride based coatings deposited by magnetron sputtering, in a broad range of applications including wear-protective coatings on cutting tools and components in automotive engines, is determined by their phase content. The classical example is the precipitation of thermodynamically-favored wurtzite-AlN while alloying TiN with Al to obtain ternary single phase NaCl-structure films with improved high-temperature oxidation resistance. Here, we report on reactive high-power impulse and direct current magnetron co-sputtering (HiPIMS/DCMS) growth of Ti0.31Al0.69N and Zr0.48Al0.52N thin films. The Al concentrations are intentionally chosen to be higher than theoretically predicted solubility limits for the rock salt structure. The goal is to investigate the effect of the incident Al+ energy EAl+, controlled by varying the amplitude of the substrate bias applied synchronously with the Al+-rich portion of the ion flux from the Al-HiPIMS source, on the crystalline phase formation. For EAl+ ≤ 60 eV, films contain predominantly the wurtzite phase. With increasing EAl+, and thus, the Al subplantation depth, the relative fraction of the NaCl structure increases and eventually for EAl+ > 250 eV, Ti0.31Al0.69N and Zr0.48Al0.52N layers contain more than 95% of the rock salt phase. Thus, the separation of the film forming species in time and energy domains determines the phase formation of Ti0.31Al0.69N and Zr0.48Al0.52N layers and enables the growth of the cubic phase outside of the predicted Al concentration range. The new film growth concept can be applied to the entire family of multinary transition metal aluminum nitrides, where one of the metallic film constituents is available in the ionized form while the other arrives as neutral.
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Research context

OpenAlex topics: Metal and Thin Film Mechanics · Semiconductor materials and devices · Diamond and Carbon-based Materials Research

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

Affiliations

Thin Film Physics Division, Department of Physics, Chemistry and Biology (IFM), Linköping University, SE-581 83 Linköping, Sweden

Materials Chemistry, RWTH Aachen University, Kopernikusstr. 10, D-52074 Aachen, Germany

Funding

Deutsche Forschungsgemeinschaft · VINNOVA · Knut och Alice Wallenbergs Stiftelse · Åforsk Foundation · Vetenskapsrådet · Carl Tryggers Stiftelse för Vetenskaplig Forskning · Stiftelsen för Strategisk Forskning

References (53)

Show source-provided references
1. Industrial deposition of binary, ternary, and quaternary nitrides of titanium, zirconium, and aluminum10.1116/1.574948 ↗
2. Microstructural design of hard coatings10.1016/j.pmatsci.2006.02.002 ↗
3. Multicomponent and multilayer physically vapour deposited coatings for cutting tools10.1016/0257-8972(92)90169-B ↗
4. Titanium aluminum nitride films: A new alternative to TiN coatings10.1116/1.573713 ↗
5. Mechanical properties and machining performance of Ti1−xAlxN-coated cutting tools10.1016/j.surfcoat.2004.04.056 ↗
6. Effects of Al content on hardness, lattice parameter and microstructure of Ti1−xAlxN films10.1016/S0257-8972(99)00491-0 ↗
7. Thermal stability of arc evaporated high aluminum-content Ti1−xAlxN thin films10.1116/1.1503784 ↗
8. Self-organized nanostructures in the Ti–Al–N system10.1063/1.1608464 ↗
9. Thermal decomposition products in arc evaporated TiAlN/TiN multilayers10.1063/1.2998588 ↗
10. Phase stability and alloy-related trends in Ti–Al–N, Zr–Al–N and Hf–Al–N systems from first principles10.1016/j.surfcoat.2011.09.019 ↗
11. Phase stabilities and thermal decomposition in the Zr1−xAlxN system studied by ab initio calculation and thermodynamic modeling10.1016/j.actamat.2007.10.050 ↗
12. Mixing and decomposition thermodynamics of c−Ti1−xAlxN from first-principles calculations10.1103/PhysRevB.75.045123 ↗
13. Crystallite size-dependent metastable phase formation of TiAlN coatings10.1038/s41598-017-16567-z ↗
14. Crystal growth and microstructure of polycrystalline Ti1−xAlxN alloy films deposited by ultra-high-vacuum dual-target magnetron sputtering10.1016/0040-6090(93)90244-J ↗
15. Design and characterization of a compact two-target ultrahigh vacuum magnetron sputter deposition system: Application to the growth of epitaxial Ti1−xAlxN alloys and TiN/Ti1−xAlxN superlattices10.1116/1.578279 ↗
16. Characterization of Zr–Al–N films synthesized by a magnetron sputtering method10.1016/j.surfcoat.2004.07.036 ↗
17. Influence of the aluminum incorporation on the structure of sputtered ZrNx films deposited at low temperatures10.1016/j.vacuum.2009.03.012 ↗
18. Microstructure and nanohardness properties of Zr–Al–N and Zr–Cr–N thin films10.1116/1.1924579 ↗
19. Experimental and computational study on the phase stability of Al-containing cubic transition metal nitrides10.1088/0022-3727/43/3/035302 ↗
20. Extended metastable Al solubility in cubic VAlN by metal-ion bombardment during pulsed magnetron sputtering: Film stress vs subplantation10.1063/1.4991640 ↗
21. Microstructure, chemical states, and mechanical properties of magnetron co-sputtered V1−xAlxN coatings10.1016/j.surfcoat.2013.05.023 ↗
22. Unprecedented Al supersaturation in single-phase rock salt structure VAlN films by Al+ subplantation10.1063/1.4977813 ↗
23. A novel pulsed magnetron sputter technique utilizing very high target power densities10.1016/S0257-8972(99)00292-3 ↗
24. Role of Tin+ and Aln+ ion irradiation (n = 1, 2) during Ti1-xAlxN alloy film growth in a hybrid HIPIMS/magnetron mode10.1016/j.surfcoat.2012.04.024 ↗
25. Control of Ti1−xSixN nanostructure via tunable metal-ion momentum transfer during HIPIMS/DCMSco-deposition10.1016/j.surfcoat.2015.09.001 ↗
26. Novel strategy for low-temperature, high-rate growth of dense, hard, and stress-free refractory ceramic thin films10.1116/1.4884575 ↗
27. Strategy for tuning the average charge state of metal ions incident at the growing film during HIPIMS deposition10.1016/j.vacuum.2015.02.027 ↗
28. Selectable phase formation in VAlN thin films by controlling Al+ subplantation depth10.1038/s41598-017-17846-5 ↗
29. (2018, December 27). Available online: https://www.cemecon.de/en/coating-plants/cc-800-hipims.
30. Venting temperature determines surface chemistry of magnetron sputtered TiN films10.1063/1.4940974 ↗
31. A combined segmented anode gas ionization chamber and time-of-flight detector for heavy ion elastic recoil detection analysis10.1063/1.4963709 ↗
32. Unprecedented thermal stability of inherently metastable titanium aluminum nitride by point defect engineering10.1080/21663831.2016.1233914 ↗
33. (1998). The JCPDS Database, Data Set Number: 25-1133, International Center for Diffraction Data.
34. (1998). The JCPDS Database, Data Set Number: 35-0753, International Center for Diffraction Data.
35. Synthesis of aluminum nitride monocrystals
36. Birkholz, M. (2006). Residual stress analysis. Thin Film Analysis by X-Ray Scattering, Wiley-VCH.10.1002/3527607595 ↗
37. (1998). The JCPDS Database, Data Set Number: 35-0768, International Center for Diffraction Data.
38. (1998). The JCPDS Database, Data Set Number: 38-1420, International Center for Diffraction Data.
39. The first ~1 Å from the surface was not considered in the fraction calculation of the implanted Al+.
40. TRIDYN—Binary collision simulation of atoms collisions and dynamic composition changes in solids10.1016/0010-4655(88)90148-8 ↗
41. Structural and mechanical evolution of reactively and non-reactively sputtered Zr–Al–N thin films during annealing10.1016/j.surfcoat.2014.01.049 ↗
42. Nanolabyrinthine ZrAlN thin films by self-organization of interwoven single-crystal cubic and hexagonal phases
43. Formation of polyhedral N2 bubbles during reactive sputter deposition of epitaxial TiN (100) films10.1063/1.343570 ↗
44. A simple model for the formation of compressive stress in thin films by ion bombardment10.1016/0040-6090(93)90201-Y ↗
45. Magnetron-sputtered superhard materials10.1016/S0257-8972(97)00159-X ↗
46. Mechanical integrity in PVD coatings due to the presence of residual stresses10.1016/S0040-6090(01)01043-4 ↗
47. Residual stresses in PVD hard coatings10.1016/0257-8972(95)02581-2 ↗
48. Lide, D.R. (2003). CRC Handbook of Chemistry and Physics, CRC Press. [84th ed.].
49. Microstructure modification of TiN by ion bombardment during reactive sputter deposition10.1016/0040-6090(89)90713-X ↗
50. Microstructural evolution during film growth10.1116/1.1601610 ↗
51. Correlative plasma-surface model for metastable Cr–Al–N: Frenkel pair formation and influence of the stress state on the elastic properties10.1063/1.4985172 ↗
52. Peak amplitude of target current determines deposition rate loss during high power pulsed magnetron sputtering10.1016/j.vacuum.2015.11.004 ↗
53. Gas rarefaction effects during high power pulsed magnetron sputtering of groups IVb and VIb transition metals in Ar10.1116/1.4989674 ↗