Next Article in Journal
Statistical/Numerical Model of the Powder-Gas Jet for Extreme High-Speed Laser Material Deposition
Previous Article in Journal
Entropy Analysis of an MHD Synthetic Cilia Assisted Transport in a Microchannel Enclosure with Velocity and Thermal Slippage Effects
 
 
Search for Articles:
Title / Keyword
Author / Affiliation / Email
Journal
Article Type
 
 
Advanced Search
 
Section
Special Issue
Volume
Issue
Number
Page
 
Journals
Coatings
Volume 10
Issue 4
10.3390/coatings10040415
coatings-logo
Submit to this Journal Review for this Journal Propose a Special Issue
► Article Menu

Article Menu

share Share announcement Help format_quote Cite question_answer Discuss in SciProfiles
first_page
settings
Order Article Reprints
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

Oxidation Behavior and Structural Transformation of (CrTaTiVZr)N Coatings

by
Zue-Chin Chang
* and
Jun-Yang Liang
Department of Mechanical Engineering, National Chin-Yi University of Technology, Taichung 41170, Taiwan
*
Author to whom correspondence should be addressed.
Coatings 2020, 10(4), 415; https://doi.org/10.3390/coatings10040415
Submission received: 24 February 2020 / Revised: 14 April 2020 / Accepted: 20 April 2020 / Published: 22 April 2020
Browse Figures
Versions Notes

Abstract

:
(CrTaTiVZr)N coatings were prepared on Si substrates through the reactive magnetron sputtering system to investigate the oxidation behaviors and structural evolution of the coatings at different annealing temperatures in air. The (CrTaTiVZr)N coating had a face-centered cubic structure with an oxidation temperature of up to 300 °C, but its surface changed into the amorphous oxide phase and then into the rutile TiO2 phase when the annealing temperature was increased to 500 °C. The rutile TiO2 phase continued to grow, and an additional solid solution phase of body-centered tetragonal I41/amd was formed at annealing temperatures beyond 600 °C. The high annealing temperature promoted the oxidation to progress along the thickness direction and synergistically developed the porosity. As a result, the hardness and the electrical performance of the coating deteriorated. The hardness decreased from 34.30 GPa to 1.52 GPa, and the electrical resistivity increased from 142 µΩ·cm to 17.5 Ω·cm.

1. Introduction

The use of high-entropy alloys (HEAs) comprising at least five principal elements with concentrations between 5 at.% and 35 at.% has good potential in the design of new metallic multicomponent alloys [1,2,3]. This specific composition design is compatible with the four core factors of HEAs, namely, high entropy, sluggish diffusion, lattice distortion, and cocktail effect [1,2]. The high mixing entropy enhances the mutual solubility among elements and reduces the tendency of phase separation into ordered phases or intermetallic compounds. The sluggish diffusion decreases the diffusion rate and results in the formation of nanocrystalline or even amorphous structures. The lattice distortion hinders the dislocation motion and results in a significantly strengthened solid solution. Finally, cocktail effects cause a composite effect in HEAs. The interaction and influence of alloy components are reflected in the alloy properties and produce additional effects. With proper alloy designs, the alloy components have shown properties that outperform traditional materials, such as high hardness and superior resistance to temper softening, wear, oxidation, and corrosion.
On the basis of the development of HEAs, HEA films are frequently investigated because of their mechanical and thermal properties. Many researchers have prepared HEA films by using various methods, such as magnetron sputtering [4,5,6,7,8,9,10,11,12], laser cladding [13,14,15], electrochemical deposition [16], arc thermal spraying [17], cold spraying [18], electron beam evaporation deposition [19], and plasma cladding [20]. At present, laser cladding and magnetron sputtering are commonly used by researchers to obtain films with excellent physical properties. The laser cladding technology is used to form coatings by melting metal powder by using high-power and high-speed lasers. This strategy provides many unparalleled advantages in forming refractory HEAs. The rapid solidification velocity enables nonequilibrium solute trapping and avoids component segregation. The coating combined with the metallurgy matrix remarkably improves the bonding strength. However, cracks and pores easily occur during laser cladding [12]. Sputtering deposition occurs due to the ion bombardment on targets by using plasma and knocking the atoms off the target surface. The high kinetic energy of the knockout target atoms allows the formation of compact and smooth films. However, sputtered films produce limited film thickness and poor bonding strength between the film and the substrate. The advantage of the sputtering method is the deposition of HEA nitride (HEAN) films. HEAN films are easily synthesized due to the easy incorporation of the nitrogen during deposition. This feature provides an effective way of exploring the HEAN system.
Additional applications have been expanded recently by producing HEANs in the form of thin films, such as (AlCoCrNi)N [4], (TiZrHfNiCuCo)N [5], (CrTaTiVZr)N [6,7], (TiZrNbAlYCr)N [8], (AlCrNbSiTiV)N [9], (FeCoNiCrCuAl0.5)N [10], (FeCoNiCuVZrAl)N [11], and (TiVCrZrNbMoHfTaWAlSi)N [12]. Almost all HEAN coatings consist of a single face-centered cubic (FCC) solid solution structure. Their mechanical properties strongly depend on the process parameters and constituent elements. Our previous research has investigated the structural evolution and the mechanical and the electro-optical properties of (CrTaTiVZr)N coatings [7]. The target constituents are all refractory, and strong nitride-forming elements are designed to deposit strong nitride coatings. In the past years, sputtered ternary (CrTiV)N coatings have exhibited a hardness of 18.74 GPa [21]. Large and heavy Ta and Zr atoms are incorporated to improve microstructure and mechanical properties, suppress grain growth, increase the energy of sputtered and backscattered atoms reaching the substrate, densify the coating structure, and enhance physical performance [22]. (CrTaTiVZr)N coatings are characterized by hardness and electrical conductivity of 36.4 GPa and 7633 S·cm−1, respectively, with light reflectivity of 74% near 2000 nm. These findings indicate the competitiveness of these coatings in coating applications. Compared with some high-entropy nitrides with non-nitride-forming elements, such as Ni, Cu, and Fe, (CrTaTiVZr)N coatings have better mechanical properties. On the other hand, AlN and Si3N4 are electrically insulating materials, and their incorporation into HEANs results in high electrical resistivity and low infrared reflectivity. These features make their applicability in microelectronic and optical fields questionable. By contrast, (CrTaTiVZr)N coatings exhibit satisfactory electro-optical performance. However, a detailed study on their oxidation resistance and structural changes during the thermal process in air is lacking. The oxidation resistance of coatings has become an important issue because of their widespread application. For instance, infrared-reflective coatings on solar-selective applications are necessary for the concentration of sunlight on heat-collecting elements. However, the high temperature provided by sunlight causes coating instability, resulting in loss in reflectivity. Ideal durable infrared-reflective coatings require high infrared reflectivity and durability in oxidation resistance at high temperatures. Developing high-temperature air-stable solar-selective coatings is urgently needed. In another example, under some machining conditions, the temperature at contact points between the tool and the workpiece becomes high. Machining without the application of coolants has been a common trend in the industry to reduce health and environmental effects but leads to excessive heat. Thus, the oxidation behavior of protective coatings under high temperature in air is becoming critical. Therefore, this study attempted to grow (CrTaTiVZr)N coatings for applications with high temperature in air. The mechanical and electrical properties after annealing at different temperatures in air were evaluated. The crystal phase evolutions and microstructure developments were also investigated.

2. Experimental

(CrTaTiVZr)N coatings were deposited on p-Si (100) wafers and fused quartz via the DC magnetron sputtering system by using equimolar CrTaTiVZr targets with a diameter of 75 mm. All elements in the target had the same molar ratios. Prior to deposition, the p-Si (100) wafers were cleaned in an ultrasonic bath and rinsed thoroughly with ethanol and distilled water. These wafers were then placed in the vacuum system. The distance from the target to the substrate was 90 mm, and the deposition angle was 60° relative to the substrate. The substrate stage was rotated at 5 rpm to obtain the quality and thickness of a homogeneous film. The coating thickness was set to approximately 1 μm. The sputtering system consisted of a stainless-steel vacuum chamber and a rotary turbo pump, which provided an ultimate vacuum of 7 × 10−6 Torr before the gases were introduced. (CrTaTiVZr)N coatings were deposited under an Ar + N2 mixed atmosphere at a DC power and working pressure of 400 W and 6.67 × 10−1 Pa, respectively. During deposition, the Ar and the N2 flow rates were 40 and 10 sccm, respectively. The substrate was not subjected to external substrate bias and heating. The as-deposited nitride coatings were annealed at different temperatures (300–700 °C) for 2 h in air by using a furnace to determine their oxidation resistance.
The chemical compositions of (CrTaTiVZr)N coatings were determined via field-emission electron probe microanalyses (FE-EPMA, JEOL JXA-8800 M, JEOL Ltd., Tokyo, Japan), and at least three tests were performed on each sample. The crystal structures were analyzed using a glancing-incidence (1°) X-ray diffractometer (XRD, BRUKER D8 Discover, Bruker, Billerica, MA, USA) with Cu Kα radiation at a scanning speed of 1°·min−1. The scanning step and range were 0.02° and 10°–80°, respectively. Morphological studies were carried out using a field-emission scanning electron microscope (SEM, JEOL JSM-6700F, JEOL Ltd., Tokyo, Japan). The microstructural examinations were conducted using an analytic transmission electron microscope (TEM, FEI E.O. TecnaiF20, Tecnai F20 G2, EFI, Hillsboro, OR, USA). The hardness and elastic modulus of coatings were measured using the TriboLab nanoindenter (Hysitron Inc., Minneapolis, MN, USA) with a Berkovich diamond indenter tip (tip radius of approximately 50 nm). During the tests, a maximum applied load of 5000 μN was set. At least five tests were performed on each sample. The electrical resistivity of coatings was measured using a four-point probe system.

3. Results and Discussion

The coating stability at elevated temperature in air (ambient environment in the majority of applications) is a crucial factor. Figure 1 demonstrates the FE-EPMA results of (CrTaTiVZr)N coatings after annealing at different temperatures in air. The N content of coatings significantly decreased, whereas the O content increased with increased annealing temperatures above 300 °C. After annealing at 600 °C, the O content reached 61.0 at.%, whereas N was undetected in the coating. The absence of N implied that complete oxidation occurred. The extremely larger enthalpies in the formation of metal oxides relative to those of metal nitrides cause the rapid oxidation [23,24]. Notably, the constituent metal content in the coating was almost the same after annealing. Except V2O5, which had a relatively low melting point (690 °C), the oxides of the target constituents had high melting points (over 700 °C). The V2O5 phase formed during annealing may cause a slight loss in the V content. In other words, no V2O5 crystal phase was formed in this study.
Figure 2 shows the XRD patterns of (CrTaTiVZr)N coatings after annealing at different temperatures in air. At 300 °C, no phase transformation was detected. The FCC peaks were sustained at 400 °C, but the FCC (111) peak weakened. The FCC peaks disappeared due to the increased annealing temperature (500 °C), and the rutile TiO2 phase began to form. The increase in annealing temperature to 600 °C caused the appearance of an additional tetragonal phase. The relative integrated intensity of oxide phases increased sharply at 700 °C. This result indicated that rapid oxidation occurred at 500 °C with the formation of a nonprotective oxide layer. The initial crystalline TiO2 phase is usually a metastable anatase due to the faster recrystallization caused by its lower surface free energy compared with that of a rutile phase. The reported crystallization onset temperatures in the anatase phase often appear at around 300 °C. Then, the anatase phase transforms irreversibly to the rutile phase at 600 °C. This phase transformation is sometimes referred to as ART [25,26]. In our study, the rutile TiO2 phase was directly obtained at elevated temperatures. Chou et al. [27] have demonstrated that the kinetics of the anatase to rutile transformation is affected strongly by the O defect levels because O vacancies facilitate the rutile transformation. Reidy et al. [28] have shown that O vacancies provide a low-energy mass transport route and decrease the ART temperature. Thus, high O vacancies result in low ART temperatures. Batzill [29] and Ihara et al. [30] have found that N doping promotes the rutile transition. In this study, the produced oxide via the annealing of nitride may contain a high level of O vacancies and lead to a direct rutile transition [31]. The formed tetragonal phase at temperatures above 600 °C was very similar to the ZrSiO4 phase (a = 0.6604 nm, c = 0.5979, space group = I41/amd). However, no Si signal was detected from the ESCA (not shown). Huang et al. [32] have determined that the sputtered AlCoCrCu0.5NiFe oxide coatings are in the tetragonal HCP solid solution phase because the large mixing entropy at elevated temperatures can stabilize solid solutions in multiprincipal elements. Therefore, the formation of a BCT I41/amd solid solution phase via the CrTaTiVZr oxide coating was relevant to the high entropy effect.
Figure 3 shows the SEM micrographs of (CrTaTiVZr)N coatings after annealing at different temperatures in air. The as-deposited typical columnar structure exhibited a cauliflower-like surface feature. No significant change was observed at 300 °C. However, a very thin and dense oxide layer formed at 400 °C with a thickness of 80 nm on the surface of the nitride. The oxide layer thickened and revealed a nanopore feature when the annealing temperature was increased to 500 °C. The oxide reaction became rapid and nonuniform at 500 °C. The oxide layer thickness ranged from 500 nm to 900 nm. At annealing temperature above 600 °C, the coating was fully oxidized and displayed a granular porous structure.
TEM was further used to clarify the oxidation behaviors of (CrTaTiVZr)N coatings (Figure 4, Figure 5, Figure 6 and Figure 7). Similar to the SEM observation, TEM showed that the as-deposited (CrTaTiVZr)N coating exhibited a very dense and compact columnar structure (Figure 4a). The selected area diffraction (SAD) patterns (Figure 4b,c) of the CrTaTiVZr and the (CrTaTiVZr)N layers demonstrated amorphous and FCC phases, respectively. The combined high-resolution TEM (HRTEM) lattice images (Figure 4d) clearly demonstrated that the nitride layer had high FCC crystallinity. Annealing the coating at 400 °C resulted in the formation of a thin amorphous oxide with a thickness of around 80 nm on the nitride coating (Figure 5a,b). The oxide layer contained numerous visible pores with a diameter of 5–30 nm and developed large cracks that were probably due to the N release and volume expansion during oxidation. The SAD and HRTEM results (Figure 5b,c) revealed the existence of some unoxidized nitride crystallites in the oxide layer, which indicated that the oxidation behavior of coatings was controlled by diffusion [33]. After annealing at 500 °C, severe oxidation occurred, and the porous oxide layer thickened rapidly (Figure 6a). The microstructures of the surface and the inner oxide layers were significantly different. On the basis of the SAD and the nanobeam diffraction (NBD) patterns (Figure 6b,c), the phase structure in the inner oxide layer remained unchanged. However, the surface amorphous oxide layer further transformed into the rutile TiO2 crystalline phase. The HRTEM image (Figure 6d) also clarified that the amorphous phase transformed into the rutile TiO2 phase. The TEM observations demonstrated that the formed oxide layer annealed at 500 °C in air contained rutile TiO2 and amorphous phases. This finding indicated the preferred crystallization of TiO2 in this work. Notably, the behavior of the complex multicomponent (CrTaTiVZr)N alloy was difficult to examine because the alloy contained elements characterized by different oxidation mechanisms. Hence, the tendency toward selective oxidation can be anticipated from the difference in free energy for oxidation per mole of O2. The values are listed in Table 1 [24]. The extent to which this phenomenon happens or the sensitivity of selective oxidation to the difference in thermodynamic stability is assumed to be high. According to Table 1, the high thermodynamic driving forces in TiO2 and ZrO2 results in the predominant formation of TiO2 and ZrO2. However, the phase presentation strongly depends on the crystallization temperature of amorphous materials. Tominaga et al. [34] have determined that the crystallization temperatures are 445, 740, and 480 °C for Cr2O3, Ta2O5, and TiO2, respectively. Abadias et al. [22] have confirmed that crystalline oxide phases are detected in ZrN, TiN, and TaN after annealing at 500, 550, and 800 °C, respectively. Zou et al. [35] have found that annealing at 500 °C triggers the crystallization of amorphous V2O5. Therefore, except Ta2O5, the binary oxide phase of other target constituents should be observed after annealing at 700 °C. However, the oxidation behavior of the multiprincipal elements is very complex. The intense incorporation of elements with different atomic sizes in coatings results in crystallization retardation. Moreover, the ternary oxide phase instead of the individual binary oxide may form during high-temperature oxidation. Müller et al. [36] have reported that TaMoCrTiAl yields the crystal phases of TiO2, Al2O3, Cr2O3, and CrTaO4 after annealing at 1000 °C. Tsai et al. [37] have oxidized (TiVCrZrHf)N at 600 °C to form the (Zr, Hf)TiO4 crystal phase. Ren et al. [38] have detected that Ni-based superalloys consists of Cr2O3, TiO2, NiCr2O4, Al2O3, and CrTaO4 crystal phases after annealing at 850 °C. In general, the ternary oxide has higher crystallization temperatures than binary oxide, thereby expanding the amorphous temperature. In oxidized (CrTaTiVZr)N coatings, TiO2 and ZrO2 should be the preferred phases of formation due to their low free energies of formation and low crystallization temperature. However, in this study, the ZrO2 phase was undetected. On the basis of the ZrO2–V2O5 phase diagram, ZrO2 and V2O5 had extremely high affinity and tended to form the ZrV2O7 phase at relatively low temperatures [39]. Xing et al. [40] have revealed that the phase transition temperature of ZrV2O7 is 771 °C. Jantschner et al. [41] have discovered that the crystallization of amorphous ZrV2O7 occurs after annealing above 600 °C. This finding indicates that V2O5 significantly retards the formation of ZrO2 phase. By contrast, TiO2 and V2O5 have extremely low mutual solubilities [42,43]. As a result, the rutile TiO2 crystal phase formed preferentially. By further increasing the annealing temperature to 600 °C, the coating achieved complete oxidation and developed a granular porous structure (Figure 7a). The SAD observations (Figure 7b) demonstrated that high temperatures promoted the growth of rutile TiO2 phase and produced a minor BCT solid solution phase. The NBD and the HRTEM images (Figure 7c,d) also verified the growth of a highly rutile TiO2 phase. These results showed that oxidation occurred primarily through the inward diffusion of O. This finding suggested that the formation of oxide phases may have resulted in the escape of N and large volume expansion during annealing and subsequently led to porosity with many voids. These conditions implied that O can diffuse freely inward through the voids, intensify oxidation, and adversely affect the coating.
Figure 8 shows the variations in the hardness and elastic modulus of the (CrTaTiVZr)N coatings after annealing at different temperatures in air. The hardness of the as-deposited (CrTaTiVZr)N coatings was about 34.3 GPa. Hardness was almost constant during annealing at 300 °C. However, increasing the annealing temperature to 700 °C significantly reduced the hardness to 1.52 GPa.
The electrical resistivity of coatings also presented a similar trend with annealing temperature, as shown in Figure 9. The electrical resistivity of the as-deposited coatings was 142 μΩ·cm and remained constant when the annealing temperature was increased to 300 °C. Beyond this temperature, the electrical resistivity of the coatings revealed a very sharp reduction from 155 Ω·cm to 17.5 Ω·cm. Oxides typically yielded smaller hardness and higher electrical resistivity than nitrides. Therefore, poor hardness and electrical conductivity were due to the oxidized coating surface. Moreover, the increased coating porosity at high annealing temperatures considerably decreases hardness and electrical conductivity [44,45].

4. Conclusions

In this study, (CrTaTiVZr)N coatings were deposited on the Si substrate through the reactive magnetron sputtering process to evaluate their crystal phases, microstructure, and mechanical and electrical properties after oxidation at high temperatures in the air environment. The FCC structure of the as-deposited coating partially changed to amorphous phases on the surface after oxidation at 400 °C in air for 2 h. The amorphous oxide layer of the coating thickened rapidly along the thickness direction and started to transform into the crystal rutile TiO2 phase near the coating surface. A minor BCT I41/amd solid solution phase appeared at annealing temperatures above 600 °C. The as-deposited coating had a columnar structure, whereas the oxide layer obtained a granular porous structure at temperatures above 500 °C. The average grain size increased with increasing annealing temperature. The mechanical and electrical performance of the oxide layer with porous structure clearly worsened. The hardness and the electrical resistivity of (CrTaTiVZr)N coatings decreased to 1.52 GPa and increased to 17.5 Ω·cm, respectively.

Author Contributions

Formal analysis, J.-Y.L.; investigation, J.-Y.L.; data curation, Z.-C.C.; writing—original draft preparation, Z.-C.C.; writing—review and editing, Z.-C.C. All authors have read and agreed to the published version of the manuscript.

Funding

This research was funded by the Ministry of Science and Technology of Taiwan under Grant No. NSC 106-2622-E-167-013-CC3.

Acknowledgments

The present work was supported in part by the Center for Micro/Nano Science and Technology of the National Cheng Kung University.

Conflicts of Interest

The authors declare no conflict of interest.

References

  1. Murty, B.S.; Yeh, J.W.; Ranganathan, S. High-Entropy Alloys; Elsevier Inc.: Amsterdam, The Netherlands, 2014. [Google Scholar]
  2. Gao, M.C.; Yeh, J.W.; Liaw, P.K.; Zhang, Y. High-Entropy Alloys Fundamentals and Applications; Springer International Publishing: Cham, Switzerland, 2016. [Google Scholar]
  3. Miracle, D.B.; Senkov, O.N. A critical review of high entropy alloys and related concepts. Acta Mater. 2017, 122, 448–511. [Google Scholar] [CrossRef] [Green Version]
  4. Kim, Y.S.; Park, H.J.; Lim, K.S.; Hong, S.H.; Kim, K.B. Structural and Mechanical Properties of AlCoCrNi High Entropy Nitride Films: Influence of Process Pressure. Coatings 2020, 10, 10. [Google Scholar] [CrossRef] [Green Version]
  5. Kim, Y.S.; Park, H.J.; Mun, S.C.; Jumaev, E.; Hong, S.H.; Song, G.; Kim, J.T.; Park, Y.K.; Kim, K.S.; Jeong, S.I.; et al. Investigation of structure and mechanical properties of TiZrHfNiCuCo high entropy alloy thin films synthesized by magnetron sputtering. J. Alloys Compd. 2019, 797, 834–841. [Google Scholar] [CrossRef]
  6. Chang, Z.-C.; Tsai, D.-C.; Chen, E.-C. Effect of N2 flow on the structure and mechanical properties of (CrTaTiVZr)Nx coatings processed by reactive magnetron sputtering. J. Mater. Res. 2015, 30, 924–934. [Google Scholar] [CrossRef]
  7. Chang, Z.-C.; Tsai, D.-C.; Chen, E.-C. Structure and characteristics of reactive magnetron sputtered (CrTaTiVZr)N coatings. Mater. Sci. Semicond. Process. 2015, 39, 30–39. [Google Scholar] [CrossRef]
  8. Pogrebnjak, A.D.; Beresnev, V.M.; Smyrnova, K.V.; Kravchenko, Y.; Zukowski, P.V.; Bondarenko, G.G. The influence of nitrogen pressure on the fabrication of the two-phase superhard nanocomposite (TiZrNbAlYCr)N coatings. Mater. Lett. 2018, 211, 316–318. [Google Scholar] [CrossRef] [Green Version]
  9. Chang, C.H.; Li, P.W.; Wu, Q.Q.; Wang, M.H.; Sung, C.C.; Hsu, C.-Y. Nanostructured and mechanical properties of high-entropy alloy nitride films prepared by magnetron sputtering at different substrate temperatures. Mater. Technol. 2018, 34, 343–349. [Google Scholar] [CrossRef]
  10. Chen, T.K.; Shun, T.T.; Yeh, J.W.; Wong, M.S. Nanostructured nitride films of multi-element high-entropy alloys by reactive DC sputtering. Surf. Coat. Technol. 2004, 188–189, 193–200. [Google Scholar] [CrossRef]
  11. Liu, L.; Zhu, J.B.; Hou, C.; Li, J.C.; Jiang, Q. Dense and smooth amorphous films of multicomponent FeCoNiCuVZrAl high-entropy alloy deposited by direct current magnetron sputtering. Mater. Des. 2013, 46, 675–679. [Google Scholar] [CrossRef]
  12. Chang, Z.-C. Structure and properties of duodenary (TiVCrZrNbMoHfTaWAlSi)N coatings by reactive magnetron sputtering. Mater. Chem. Phys. 2018, 220, 98–110. [Google Scholar] [CrossRef]
  13. Shu, F.Y.; Liu, S.; Zhao, H.Y.; He, W.X.; Sui, S.H.; Zhang, J.; He, P.; Xu, B.S. Structure and high-temperature property of amorphous composite coating synthesized by laser cladding FeCrCoNiSiB high-entropy alloy powder. J. Alloys Compd. 2018, 731, 662–666. [Google Scholar] [CrossRef]
  14. Jin, G.; Cai, Z.; Guan, Y.; Cui, X.; Liu, Z.; Li, Y.; Dong, M.; Zhang, D. High temperature wear performance of laser-cladded FeNiCoAlCu high-entropy alloy coating. Appl. Surf. Sci. 2018, 445, 113–122. [Google Scholar] [CrossRef]
  15. Chen, S.; Chen, X.; Wang, L.; Liang, J.; Liu, C. Laser cladding FeCrCoNiTiAl high entropy alloy coatings reinforced with self-generated TiC particles. J. Laser Appl. 2016, 29, 012004. [Google Scholar] [CrossRef]
  16. Yao, C.; Wei, B.; Zhang, P.; Lu, X.; Liu, P.; Tong, Y. Facile preparation and magnetic study of amorphous Tm-Fe-Co-Ni-Mn multicomponent alloy nanofilm. J. Rare Earths 2011, 29, 133–137. [Google Scholar] [CrossRef]
  17. Li, Q.; Yue, T.; Guo, Z. Electro-spark Deposition of Multi-Element High Entropy Alloy Coating; ASM International: Almere, The Netherlands, 2010. [Google Scholar]
  18. Yin, S.; Li, W.; Song, B.; Yan, X.; Kuang, M.; Xu, Y.; Wen, K.; Lupoi, R. Deposition of FeCoNiCrMn high entropy alloy (HEA) coating via cold spraying. J. Mater. Sci. Technol. 2019, 35, 1003–1007. [Google Scholar] [CrossRef]
  19. Popov, V.V.; Katz-Demyanetz, A.; Koptyug, A.; Bamberger, M. Selective electron beam melting of Al0.5CrMoNbTa0.5 high entropy alloys using elemental powder blend. Heliyon 2019, 5, e01188. [Google Scholar] [CrossRef] [Green Version]
  20. Cai, Z.; Wang, Y.; Cui, X.; Jin, G.; Li, Y.; Liu, Z.; Dong, M. Design and microstructure characterization of FeCoNiAlCu high-entropy alloy coating by plasma cladding: In comparison with thermodynamic calculation. Surf. Coat. Technol. 2017, 330, 163–169. [Google Scholar] [CrossRef]
  21. Tsai, D.-C.; Huang, Y.-L.; Lin, S.-R.; Jung, D.-R.; Chang, S.-Y.; Shieu, F.-S. Structure and mechanical properties of (TiVCr)N coatings prepared by energetic bombardment sputtering with different nitrogen flow ratios. J. Alloys Compd. 2011, 509, 3141–3147. [Google Scholar] [CrossRef]
  22. Abadias, G.; Koutsokeras, L.E.; Siozios, A.; Patsalas, P. Stress, phase stability and oxidation resistance of ternary Ti–Me–N (Me=Zr, Ta) hard coatings. Thin Solid Films 2013, 538, 56–70. [Google Scholar] [CrossRef]
  23. Pierson, H.O. Handbook of Refractory Carbides and Nitrides; Noyes Publications: Westwood, NJ, USA, 1996. [Google Scholar]
  24. Dean, J.A. Lange’s Handbook of Chemistry; McGraw-Hill: New York, NY, USA, 1999. [Google Scholar]
  25. Rath, C.; Mohanty, P.; Pandey, A.C.; Mishra, N.C. Oxygen vacancy induced structural phase transformation in TiO2 nanoparticles. J. Phys. D Appl. Phys. 2009, 42, 205101. [Google Scholar] [CrossRef]
  26. Ghosh, T.B.; Dhabal, S.; Datta, A.K. Erratum: On crystalline size dependence of phase stability of nanocrystalline TiO2. Appl. Phys. 94, 4577 (2003). J. Appl. Phys. 2003, 95, 408. [Google Scholar] [CrossRef] [Green Version]
  27. Chou, P.-W.; Wang, Y.-S.; Lin, C.-C.; Chen, Y.-J.; Cheng, C.-L.; Wong, M.-S. Effect of carbon and oxygen on phase transformation of titania films during annealing. Surf. Coat. Technol. 2009, 204, 834–839. [Google Scholar] [CrossRef]
  28. Reidy, D.J.; Holmes, J.D.; Morris, M.A. The critical size mechanism for the anatase to rutile transformation in TiO2 and doped-TiO2. J. Eur. Ceram. Soc. 2006, 26, 1527–1534. [Google Scholar] [CrossRef]
  29. Batzill, M.; Morales, E.H.; Diebold, U. Influence of Nitrogen Doping on the Defect Formation and Surface Properties of TiO2 Rutile and Anatase. Phys. Rev. Lett. 2006, 96, 026103. [Google Scholar] [CrossRef]
  30. Ihara, T.; Miyoshi, M.; Iriyama, Y.; Matsumoto, O.; Sugihara, S. Visible-light-active titanium oxide photocatalyst realized by an oxygen-deficient structure and by nitrogen doping. Appl. Catal. B Environ. 2003, 42, 403–409. [Google Scholar] [CrossRef]
  31. Chen, H.-Y.; Lu, F.-H. Oxidation behavior of titanium nitride films. J. Vac. Sci. Technol. A 2005, 23, 1006–1009. [Google Scholar] [CrossRef] [Green Version]
  32. Huang, Y.-S.; Chen, L.; Lui, H.-W.; Cai, M.-H.; Yeh, J.-W. Microstructure, hardness, resistivity and thermal stability of sputtered oxide films of AlCoCrCu0.5NiFe high-entropy alloy. Mater. Sci. Eng. A 2007, 457, 77–83. [Google Scholar] [CrossRef]
  33. Unutulmazsoy, Y.; Merkle, R.; Fischer, D.; Mannhart, J.; Maier, J. The oxidation kinetics of thin nickel films between 250 and 500 °C. Phys. Chem. Chem. Phys. 2017, 19, 9045–9052. [Google Scholar] [CrossRef] [Green Version]
  34. Tominaga, K.; Adachi, H.; Wasa, K. 6—Functional Thin Films. In Handbook of Sputtering Technology, 2nd ed.; Wasa, K., Kanno, I., Kotera, H., Eds.; William Andrew Publishing: Oxford, UK, 2012; p. 495. ISBN 978-1-4377-3483-6. [Google Scholar]
  35. Zou, C.W.; Yan, X.D.; Patterson, D.; Emanuelsson, E.A.C.; Bian, J.M.; Gao, W. Temperature sensitive crystallization of V2O5: From amorphous film to β-V2O5nanorods. CrystEngComm 2010, 12, 691–693. [Google Scholar] [CrossRef]
  36. Müller, F.; Gorr, B.; Christ, H.-J.; Müller, J.; Butz, B.; Chen, H.; Kauffmann, A.; Heilmaier, M. On the oxidation mechanism of refractory high entropy alloys. Corros. Sci. 2019, 159, 108161. [Google Scholar] [CrossRef]
  37. Tsai, D.-C.; Chang, Z.-C.; Kuo, L.-Y.; Lin, T.-J.; Lin, T.-N.; Shiao, M.-H.; Shieu, F.-S. Oxidation resistance and structural evolution of (TiVCrZrHf)N coatings. Thin Solid Films 2013, 544, 580–587. [Google Scholar] [CrossRef]
  38. Ren, W.; Ouyang, F.; Ding, B.; Zhong, Y.; Yu, J.; Ren, Z.; Zhou, L. The influence of CrTaO4 layer on the oxidation behavior of a directionally-solidified nickel-based superalloy at 850–900 °C. J. Alloys Compd. 2017, 724, 565–574. [Google Scholar] [CrossRef]
  39. Ondik, H.; McMurdie, H.F. Phase Diagrams for Zirconium and Zirconia Systems; American Ceramic Society: Columbus, DC, USA, 2017. [Google Scholar]
  40. Xing, X.; Zhu, Z.; Qiu, X.; Liu, G. Zero-Thermal Expansion and Heat Capacity of Zirconium Pyrovanadate Doped with Zirconia and Vanadium (V) Oxide. Rare Met. 2001, 20, 1–4. [Google Scholar]
  41. Jantschner, O. Investigation on Vanadium Containing Zirconia Coatings for High Temperature Sliding Interfaces; University of Leoben: Leoben, Austria, 2011. [Google Scholar]
  42. Habel, D.; Stelzer, J.B.; Feike, E.; Schröder, C.; Hösch, A.; Hess, C.; Knop-Gericke, A.; Caro, J.; Schubert, H. Phase development in the catalytic system V2O5/TiO2 under oxidising conditions. J. Eur. Ceram. Soc. 2006, 26, 3287–3294. [Google Scholar] [CrossRef]
  43. Malan, W.D.; Akdogan, G.; Taskinen, P.; Hamuyuni, J.; Zietsman, J. Phase equilibria and thermodynamic evaluation of the Ti-V-O system in air. Calphad 2018, 63, 220–228. [Google Scholar] [CrossRef] [Green Version]
  44. Tsai, D.-C.; Chang, Z.-C.; Kuo, B.-H.; Tsao, C.-T.; Chen, E.-C.; Shieu, F.-S. Influence of discharge power on the structural, electro-optical, and mechanical properties of (TiZrHf)N coatings. J. Alloys Compd. 2015, 622, 446–457. [Google Scholar] [CrossRef]
  45. Tsai, D.-C.; Chang, Z.-C.; Kuo, B.-H.; Chen, B.-C.; Chen, E.-C.; Shieu, F.-S. Wide variation in the structure and physical properties of reactively sputtered (TiZrHf)N coatings under different working pressures. J. Alloys Compd. 2018, 750, 350–359. [Google Scholar] [CrossRef]
Coatings 10 00415 g001 550
Figure 1. FE-EPMA results of (CrTaTiVZr)N after annealing at different temperatures in air.
Figure 1. FE-EPMA results of (CrTaTiVZr)N after annealing at different temperatures in air.
Coatings 10 00415 g001
Coatings 10 00415 g002 550
Figure 2. X-ray diffraction patterns of (CrTaTiVZr)N coatings after annealing at different temperatures in air.
Figure 2. X-ray diffraction patterns of (CrTaTiVZr)N coatings after annealing at different temperatures in air.
Coatings 10 00415 g002
Coatings 10 00415 g003 550
Figure 3. Plan-view and cross-sectional SEM micrographs of the (CrTaTiVZr)N coatings after annealing at different temperatures in air. (a) as-deposited, (b) 300 °C, (c) 400 °C, (d) 500 °C, (e) 600 °C, (f) 700 °C.
Figure 3. Plan-view and cross-sectional SEM micrographs of the (CrTaTiVZr)N coatings after annealing at different temperatures in air. (a) as-deposited, (b) 300 °C, (c) 400 °C, (d) 500 °C, (e) 600 °C, (f) 700 °C.
Coatings 10 00415 g003
Coatings 10 00415 g004 550
Figure 4. Cross-sectional TEM micrographs of the as-deposited (CrTaTiVZr)N coatings. (a) bright-field image, (b) SAD pattern of the metal interlayer, (c) SAD pattern of nitride layer, (d) HRTEM lattice image.
Figure 4. Cross-sectional TEM micrographs of the as-deposited (CrTaTiVZr)N coatings. (a) bright-field image, (b) SAD pattern of the metal interlayer, (c) SAD pattern of nitride layer, (d) HRTEM lattice image.
Coatings 10 00415 g004
Coatings 10 00415 g005 550
Figure 5. Cross-sectional TEM micrographs of the as-deposited (CrTaTiVZr)N coatings after annealing at 400 °C in air. (a) bright-field image, (b) SAD pattern of the oxide layer, (c) HRTEM lattice image.
Figure 5. Cross-sectional TEM micrographs of the as-deposited (CrTaTiVZr)N coatings after annealing at 400 °C in air. (a) bright-field image, (b) SAD pattern of the oxide layer, (c) HRTEM lattice image.
Coatings 10 00415 g005
Coatings 10 00415 g006 550
Figure 6. Cross-sectional TEM micrographs of the as-deposited (CrTaTiVZr)N coatings after annealing at 500 °C in air. (a) bright-field image, (b) SAD pattern of the oxide bulk layer, (c) NBD pattern of the oxide surface layer, (d) HRTEM lattice image.
Figure 6. Cross-sectional TEM micrographs of the as-deposited (CrTaTiVZr)N coatings after annealing at 500 °C in air. (a) bright-field image, (b) SAD pattern of the oxide bulk layer, (c) NBD pattern of the oxide surface layer, (d) HRTEM lattice image.
Coatings 10 00415 g006
Coatings 10 00415 g007 550
Figure 7. Cross-sectional TEM micrographs of the as-deposited (CrTaTiVZr)N coatings after annealing at 600 °C in air. (a) bright-field image, (b) SAD pattern of the oxide layer, (c) NBD pattern of the oxide layer, (d) HRTEM lattice image.
Figure 7. Cross-sectional TEM micrographs of the as-deposited (CrTaTiVZr)N coatings after annealing at 600 °C in air. (a) bright-field image, (b) SAD pattern of the oxide layer, (c) NBD pattern of the oxide layer, (d) HRTEM lattice image.
Coatings 10 00415 g007
Coatings 10 00415 g008 550
Figure 8. Hardness and elastic modulus of (CrTaTiVZr)N coatings after annealing at different temperatures in air.
Figure 8. Hardness and elastic modulus of (CrTaTiVZr)N coatings after annealing at different temperatures in air.
Coatings 10 00415 g008
Coatings 10 00415 g009 550
Figure 9. Electrical resistivity of (CrTaTiVZr)N coatings after annealing at different temperatures in air.
Figure 9. Electrical resistivity of (CrTaTiVZr)N coatings after annealing at different temperatures in air.
Coatings 10 00415 g009
Table
Table 1. Standard free energies of formation of oxides based on the target elements.
Table 1. Standard free energies of formation of oxides based on the target elements.
OxideCr2O3Ta2O5TiO2V2O5ZrO2
ΔG (kJ·mol−1 O2)352.7382.2444.4283.86521.4

Share and Cite

MDPI and ACS Style

Chang, Z.-C.; Liang, J.-Y. Oxidation Behavior and Structural Transformation of (CrTaTiVZr)N Coatings. Coatings 2020, 10, 415. https://doi.org/10.3390/coatings10040415

AMA Style

Chang Z-C, Liang J-Y. Oxidation Behavior and Structural Transformation of (CrTaTiVZr)N Coatings. Coatings. 2020; 10(4):415. https://doi.org/10.3390/coatings10040415

Chicago/Turabian Style

Chang, Zue-Chin, and Jun-Yang Liang. 2020. "Oxidation Behavior and Structural Transformation of (CrTaTiVZr)N Coatings" Coatings 10, no. 4: 415. https://doi.org/10.3390/coatings10040415

APA Style

Chang, Z.-C., & Liang, J.-Y. (2020). Oxidation Behavior and Structural Transformation of (CrTaTiVZr)N Coatings. Coatings, 10(4), 415. https://doi.org/10.3390/coatings10040415

Note that from the first issue of 2016, this journal uses article numbers instead of page numbers. See further details here.

Article Metrics

Back to TopTop