Texture and Stress Evolution in HfN Films Sputter-Deposited at Oblique Angles
Source abstract
Abstract
In this study, polycrystalline hafnium nitride (HfN) thin films were grown by oblique angle deposition (OAD) technique to investigate the relationship between column tilt angle, texture development and residual stress evolution with varying inclination angle α of the substrate. The films (~1 μm thickness) were grown at various angles (α = 5°, 25°, 35°, 65°, 75°, and 85°) with respect to the substrate normal by reactive magnetron sputtering at 0.3 Pa and 300 °C. The film morphology, crystal structure and residual stress state were characterized by scanning electron microscopy and X-ray diffraction (XRD), including pole figure and sin2ψ measurements. All HfN films had a cubic, NaCl-type crystal structure with an [111] out-of-plane orientation and exhibited a biaxial texture for α ≥ 35°. XRD pole figures reveal that the crystal habit of the grains consists of {100} facets constituting triangular-base pyramids, with a side and a corner facing the projection of the incoming particle flux (indicative of a double in-plane alignment). A columnar microstructure was formed for α ≥ 35°, with typical column widths of 100 nm. It is observed that the column tilt angle β increases monotonously for α ≥ 35°, reaching β = 34° at α = 85°. This variation at microscopic scale is correlated with the tilt angle of the (111) crystallographic planes, changing from −24.8 to 11.3° with respect to the substrate surface. The residual stress changes from strongly compressive (~−5 GPa at α = 5°) to negligible or slightly tensile for α ≥ 35°. The observed trends are compared to previous works of the literature and discussed based on existing crystal growth and stress models, as well as in light of energy and angular distribution of the incident particle flux calculated by Monte Carlo. Importantly, a decrease of the average kinetic energy of Hf particles from 22.4 to 17.7 eV is found with increasing α due to an increase number of collisions.
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Research context
OpenAlex topics: Metal and Thin Film Mechanics · Optical Coatings and Gratings · GaN-based semiconductor devices and materials
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Institut Pprime, Département Physique et Mécanique des Matériaux, Université de Poitiers-CNRS-ENSMA, SP2MI, Téléport 2, 86962 Futuroscope-Chasseneuil, France
Département Physique, Université d’Etat d’Haïti-Ecole Normale Supérieure, Laboratoire des Sciences pour l’Environnement et l’Energie (LS2E), HT6115 Canapé-Vert, Port-au-Prince, Haiti
Funding
Agence Nationale de la Recherche
References (60)
Show source-provided references
1. Optical thin-film materials with low refractive index for broadband elimination of Fresnel reflection10.1038/nphoton.2007.26 ↗
2. Sculptured thin films and glancing angle deposition: Growth mechanics and applications10.1116/1.580562 ↗
3. Glancing angle deposition: Fabrication, properties, and applications of micro- and nanostructured thin films10.1116/1.2764082 ↗
4. Perspectives on oblique angle deposition of thin films: From fundamentals to devices10.1016/j.pmatsci.2015.06.003 ↗
5. Glancing angle sputter deposited nanostructures on rotating substrates: Experiments and simulations10.1063/1.3018145 ↗
6. Structure zone model for extreme shadowing conditions10.1016/j.tsf.2012.11.007 ↗
7. Nanostructured Ti thin films by magnetron sputtering at oblique angles10.1088/0022-3727/49/4/045303 ↗
8. Critical angles in DC magnetron glad thin films10.1016/j.vacuum.2016.07.012 ↗
9. Synthesis of nanostructured Ti thin films by combining glancing angle deposition and magnetron sputtering: A joint experimental and modeling study10.1016/j.tsf.2017.06.006 ↗
10. Influence of the sputtering pressure on the morphological features and electrical resistivity anisotropy of nanostructured titanium films10.1016/j.apsusc.2017.05.175 ↗
11. Kinetic energy-induced growth regimes of nanocolumnar Ti thin films deposited by evaporation and magnetron sputtering10.1088/1361-6528/ab3cb2 ↗
12. Multi-component nanostructure design by atomic shadowing10.1016/j.tsf.2008.05.049 ↗
13. Using the macroscopic scale to predict the nano-scale behavior of YSZ thin films10.1016/j.surfcoat.2013.10.034 ↗
14. Texture and microstructure in co-sputtered Mg-M-O (M = Mg, Al, Cr, Ti, Zr, and Y) films10.1063/1.4718431 ↗
15. W-Cu sputtered thin films grown at oblique angles from two sources: Pressure and shielding effects10.1016/j.surfcoat.2017.09.062 ↗
16. Biaxially aligned titanium nitride thin films deposited by reactive unbalanced magnetron sputtering10.1016/j.surfcoat.2004.09.012 ↗
17. Study of structure development of titanium nitride on inclined substrates10.1016/j.surfcoat.2011.04.093 ↗
18. Fabrication of TiN nanostructure as a hydrogen peroxide sensor by oblique angle deposition10.1186/1556-276X-9-105 ↗
19. Nanostructured porous CrN thin films by oblique angle magnetron sputtering for symmetric supercapacitors10.1016/j.jallcom.2019.07.325 ↗
20. Oblique angle deposition of nanocolumnar TiZrN films via reactive magnetron co-sputtering technique: The influence of the Zr target powers10.1016/j.cap.2019.05.002 ↗
21. Nanocolumnar TiN thin film growth by oblique angle sputter-deposition: Experiments vs. simulations10.1016/j.matdes.2018.09.023 ↗
22. Conductive nitrides: Growth principles, optical and electronic properties, and their perspectives in photonics and plasmonics10.1016/j.mser.2017.11.001 ↗
23. Plasmonic efficiencies of nanoparticles made of metal nitrides (TiN, ZrN) compared with gold10.1038/srep38647 ↗
24. Laser- synthesized TiN nanoparticles as promising plasmonic alternative for biomedical applications10.1038/s41598-018-37519-1 ↗
25. Chiral plasmonics10.1126/sciadv.1602735 ↗
26. Biaxial alignment in sputter deposited thin films10.1016/j.tsf.2006.06.027 ↗
27. Flux engineering to control in-plane crystal and morphological orientation10.1021/cg300469s ↗
28. Tunable electrical and optical properties of hafnium nitride thin films10.1063/1.3327329 ↗
29. Examining the Performance of Refractory Conductive Ceramics as Plasmonic Materials: A Theoretical Approach10.1021/acsphotonics.5b00409 ↗
30. Noyan, I.C., and Cohen, J.B. (1987). Residual Stress Measurement by Diffraction and Interpretation, Springer.10.1007/978-1-4613-9570-6 ↗
31. Stress and preferred orientation in nitride-based PVD coatings10.1016/j.surfcoat.2007.08.029 ↗
32. Review Article: Stress in thin films and coatings: Current status, challenges, and prospects10.1116/1.5011790 ↗
33. Mobility and carrier density in materials with anisotropic conductivity revealed by van der Pauw measurements10.1103/PhysRevB.70.165307 ↗
34. The metal flux from a rotating cylindrical magnetron: A Monte Carlo simulation10.1088/0022-3727/41/20/205307 ↗
35. Ziegler, J.F., Biersack, J.P., and Littmark, U. (1985). The Stopping and Range of Ions in Matter, Pergamon Press.10.1007/978-1-4615-8103-1_3 ↗
36. Evaluation of effective threshold displacement energies and other data required for the calculation of advanced atomic displacement cross-sections10.1016/j.nucet.2017.08.007 ↗
37. A theoretical model for the electrical properties of chromium thin films sputter deposited at oblique incidence10.1088/0022-3727/44/21/215301 ↗
38. Influence of sputtering parameters on the formation process of high-quality and low-resistivity HfN thin film10.1143/JJAP.38.2097 ↗
39. Low temperature (Ts/Tm < 0.1) epitaxial growth of HfN/MgO(001) via reactive HiPIMS with metal-ion synchronized substrate bias10.1116/1.5052702 ↗
40. Growth and physical properties of epitaxial HfN layers on MgO(001)10.1063/1.1759783 ↗
41. International Center for Diffraction Data: Card No. 45-0946, ICDD.
42. Reduced atomic shadowing in HiPIMS: Role of the thermalized metal ions10.1016/j.apsusc.2017.10.133 ↗
43. Microfractography of thin films
44. Modeling and Characterization of Columnar Growth in Evaporated-Films10.1016/0040-6090(93)90378-3 ↗
45. Tilting angle of nanocolumnar films fabricated by oblique angle deposition10.1116/1.4710999 ↗
46. Nanocolumnar growth of thin films deposited at oblique angles: Beyond the tangent rule
47. Texture mechanisms and microstructure of biaxial thin films grown by oblique angle deposition10.1002/pssb.201248010 ↗
48. Evolutionary Selection, a principle governing growth orientation
49. Double in-plane alignment in biaxially textured thin films10.1063/1.4903932 ↗
50. Trends in the elastic response of binary early transition metal nitrides10.1103/PhysRevB.85.064101 ↗
51. Hard superconducting nitrides10.1073/pnas.0500174102 ↗
52. Intrinsic stress in sputter-deposited thin films10.1080/10408439208244586 ↗
53. Stress and strain in polycrystalline thin films10.1016/j.tsf.2007.03.007 ↗
54. Atom insertion into grain boundaries and stress generation in physically vapor deposited films10.1063/1.4817669 ↗
55. A kinetic model for stress generation in thin films grown from energetic vapor fluxes10.1063/1.4946039 ↗
56. In situ stress evolution during magnetron sputtering of transition metal nitride thin films10.1063/1.2985814 ↗
57. Influence of particle and energy flux on stress and texture development in magnetron sputtered TiN films10.1088/0022-3727/46/5/055301 ↗
58. Stress, phase stability and oxidation resistance of ternary Ti-Me-N (Me = Zr, Ta) hard coatings10.1016/j.tsf.2012.10.119 ↗
59. Residual stress in obliquely deposited MgF2 thin films10.1364/AO.47.00C266 ↗
60. Effects of oblique-angle deposition on intrinsic stress evolution during polycrystalline film growth10.1016/j.actamat.2014.05.060 ↗