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Article

A Study of the Features of Coating Deposition on a Carbide Substrate Using Preliminary Etching with Glow-Discharge Plasma

1
Department of High-Efficiency Machining Technologies, Moscow State University of Technology “STANKIN”, Vadkovsky Lane 3a, 127055 Moscow, Russia
2
Institute of Design and Technological Informatics of the Russian Academy of Sciences (IDTI RAS), Vadkovsky Lane 18a, 127055 Moscow, Russia
3
Department of Materials Science of Semiconductors and Dielectrics, National University of Science and Technology “MISiS”, Leninsky Prospect 4, 119049 Moscow, Russia
4
Department of Digital and Additive Technologies, Federal State Budget Educational Institution of Higher Education, MIREA—Russian Technological University, Vernadsky Avenue, 78, 119454 Moscow, Russia
*
Author to whom correspondence should be addressed.
Surfaces 2024, 7(4), 920-937; https://doi.org/10.3390/surfaces7040060
Submission received: 23 July 2024 / Revised: 24 August 2024 / Accepted: 29 October 2024 / Published: 2 November 2024

Abstract

:
The properties of coatings obtained using two surface preparation methods were compared: heating and etching by ion bombardment with plasma generation by arc evaporators and heating and etching by a glow discharge. A Ti-TiN-(Ti,Cr,Al)N coating was deposited. The use of a glow discharge provides better resistance of the coating to destruction during the scratch test and wear resistance of metal-cutting tools when turning steel. As the cutting speed increases, the advantage in wear resistance of the coating deposited using a glow discharge increases. During the process of heating and etching by ion bombardment with metal ions, a nanolayer rich in cobalt and tooling elements (iron, molybdenum) is formed in the area of the interface of the coating and the carbide substrate. When heated and etched by a glow discharge, such a layer does not form. When using both methods, there is identical diffusion of tungsten into the coating and diffusion of chromium and possibly titanium into the substrate. Thus, the glow-discharge heating and etching method can be effectively used in the process of PVD coating deposition.

1. Introduction

Modifying coatings deposited by the Physical Vapor Deposition (PVD) method is actively used to improve the performance properties of various modern industrial objects. Among the areas of the application of coatings are cutting and stamping tools, medicine, engine building, energy, and a few other applications. The preparation of the substrate surface before coating deposition is a key operation that ensures the strength of adhesion of the coating to the substrate and, accordingly, the durability and reliability of the coated part [1,2,3,4,5,6,7,8]. Among the main tasks of surface preparation is its cleaning from residual microcontaminants (including chemical, for example, oxide films), as well as thermal activation. The main method of such preparation is ion bombardment, although in some cases, chemical desorption is also used [2,4,9]. Ion bombardment (cleaning, etching) involves bombarding a surface with accelerated ions. Various schemes of ion bombardment are used, among which we can highlight etching with a beam of gas ions (usually argon ions), which is formed during the operation of a special source [10,11,12,13].
Treatment with ions accelerated by the negative potential of the substrate from plasma created by a vacuum discharge is also used [6,14,15,16,17,18,19,20,21]. This method is based on the ability to regulate ion energy by changing the negative bias potential on the substrate [17,19].
An alternative method is etching in a glow-discharge plasma [22,23,24]. This method consists in accelerating gas plasma ions (usually argon is also used) on the surface of the product, which is either the cathode of the glow discharge itself or an additional electrode negative relative to the plasma [1,3,25,26,27,28]. If nitrogen is used instead of argon, using this method, it is possible to ensure the nitriding of the surface layer of parts [29,30,31]. Other gas media are also used (acetylene, nitrogen, argon, hydrogen, and their mixtures) [32]. This method is used less frequently due to the fact that the etching rate in this case is quite low due to the low plasma density. An additional disadvantage of this method, also associated with the relatively low speed of the process, is the possibility of introducing insoluble atoms of an inert gas into the surface layer and thereby reducing the properties of this layer [28,33]. To eliminate these disadvantages of etching in gas discharge plasma, various methods are used. For example, a mesh cylinder is placed inside a rotating fixture, to which a negative voltage is applied to increase the density of the gas plasma [34]. Other ways to increase the intensity of the etching process with glow-discharge plasma include etching with dual-capacitive coupled radio-frequency (CCRF) glow-discharge plasma (CCRF) [35], atmosphere-pressure glow discharges (APGDs) [36], high-pressure glow discharges (HPGs) [37], and Arc-enhanced glow discharges (AEGDs) [24,38,39]. Glow-discharge plasma etching affects the surface layer of carbide substrates (for example, cutting tools). It was found that such etching has a greater effect on the surface layer of WC and a much smaller effect on the surface layer of TiC [40]. Pre-treatment in glow-discharge plasma can significantly increase the adhesion of the coating and substrate, as well as improve the properties of the coating itself [23,24,38,39].
All ion etching (cleaning) methods discussed above are associated with the removal of surface layers of the substrate due to the sputtering of atoms under the influence of bombardment with ions of gasses or metals accelerated to high energy. During the ion etching process, various chemical and physical processes take place on the surface of the substrate, including interdependent processes of condensation, penetration, and sputtering. When ions crash into the surface of a substrate, they transfer their kinetic energy to surface atoms [1,41]. As a result, those atoms that have acquired kinetic energy exceeding the chemical bond energy in the crystal lattice can be knocked out (emitted) from the surface of the substrate. First, those atoms that have the lowest binding energy with the surface are sputtered (for example, atoms of contaminants or chemical films).
Ion etching helps to reduce the number of macro- and microdefects, residual internal stresses, create a favorable microrelief, clean up to the atomic level (obtaining an almost juvenile clean surface), and enhance diffusion processes and surface activation by increasing the surface bond energy [5,9,40,42]. This treatment creates favorable conditions for the subsequent deposition of coatings with high adhesive bonds [6,7,15].
The efficiency of ion etching depends on the placement of samples in a vacuum chamber [26,27,28,43]. Under certain placement conditions, there may be a high likelihood of repeated cross-contamination of substrates. In areas where the intensity of ion bombardment is low, contaminants can accumulate due to the repeated redeposition of sputtered material from areas where the intensity is high.
A recently published paper [44] examines the arc-enhanced glow-discharge ion etching of ultrafine-grained WC-Co cemented carbide. The authors claim that the proposed technique allows for a significant increase in the etching rate, as well as an increase in the substrate surface roughness, which ensures better coating adhesion.
This work compares two methods of cleaning and heating samples before coating deposition:
  • Ion bombardment with the generation of metal plasma by arc evaporators.
  • Ion bombardment with the generation of gas plasma by a glow discharge.
The deposited coatings include an adhesive layer (metallic titanium, 30–50 nm thick), a transition layer of TiN with a thickness of 500–700 nm, and a wear-resistant layer (Ti, Cr, Al)N with a thickness of about 3 µm.

2. Materials and Methods

To deposit coatings on the samples, a special research installation VIT-2 was used (IDTI RAS—MSUT “STANKIN”, Russia) [45,46,47,48,49,50] (Figure 1). At the same time, two types of evaporators were installed: one filtered cathodic vacuum arc deposition (FCVAD) system [50], which allows for an up to 98% phase separation of microparticles in combination with providing a high degree of focusing of the plasma flow. Two Controlled Accelerated Arc (CAA-PVD) system evaporators were also installed [18,51,52], which are characterized by a high energy efficiency and a reduced number of microparticles compared to traditional arc-type evaporators. The Al cathode (99.8%) was installed on the FCVAD evaporator, since the Al cathode under normal conditions forms many microparticles during evaporation, which reduce the quality of the coating. Ti (99.6%) and Cr (99.9%) cathodes were installed on evaporators of the CAA-PVD system.
The method of glow-discharge plasma etching with a partial hollow cathode effect developed by Yuri Bublikov was used. Some technical details of this method are considered know-how and, since the patenting process is not yet completed, cannot be fully disclosed.
Before installation on specialized equipment and placement in the chamber, the samples underwent a preparation procedure. This procedure included washing in a special solution at high temperature with ultrasonic stimulation, washing in specially purified water, and drying in a stream of purified air. After loading the samples into the chamber, the installation is pumped down to a pressure of 6.6 × 10−3 Pa.
The working gas pressure in the chamber was maintained at different stages within the range of 1–10 Pa. The voltage on the substrate is from 300 to 1500 V.
In this work, we compare the properties of coatings using two different methods of surface cleaning and thermal activation: ion bombardment with an ion flow (hereinafter denoted as IB) and ion etching with a glow discharge (hereinafter denoted as GD).

2.1. Metal Ion Etching of Plasma Generated by Vacuum Evaporators (IB)

Upon the completion of loading, the vacuum chamber was evacuated. The ion cleaning and heating of products was carried out at a pressure of no higher than 1.0 × 10−2 Pa in plasma generated by arc evaporators with titanium and chromium cathodes installed on them. At the beginning of the process, in order to avoid the appearance of micro-arcs, a negative potential of 100 V was applied to the turntable. As the parts were cleaned and heated to achieve the required temperature of 650–700 °C, the negative potential gradually increased to 1000 V or more. When the specified temperature of the parts was reached, an adhesive titanium sublayer was deposited by an arc evaporator within 3 min. The arc current of the titanium cathode was 80 A, and the negative voltage on the parts decreased to 160 V. Then, process gas (nitrogen) was supplied to the vacuum chamber to a pressure of 0.6 Pa and a layer of titanium nitride was applied for 15 min. For the subsequent deposition of the (Ti,Cr,Al)N layer, arc evaporators with a chromium cathode and an aluminum cathode located in the separator were additionally turned on. The arc current of the evaporator with a chromium cathode was 80 A, and that of the evaporator with an aluminum cathode was 160 A. Precipitation was carried out for 30 min at a temperature of about 480 °C. The temperature of the products was regulated by the value of the reference voltage of the turntable.

2.2. Etching by Gas Ions of a Self-Sustained Glow-Discharge Plasma (GD)

This technological process differs from the one described above in that the ion cleaning and heating of products was carried out by ion bombardment only with gas ions of a glow-discharge plasma. All other stages and parameters of both technological cycles were identical. The stage of the ion cleaning of products was carried out in a glow discharge in an argon environment at a pressure of 2.5 Pa. The process began with applying a negative bias potential of −100 V to the sprayed parts; then, the potential gradually rose to −1500 V, the pressure in the chamber increased to 8 Pa, the negative bias potential on the products was fixed at −1500 V, and the parts were heated to a temperature of 650 °C.
To study the hardness, an automated mechanical tester SV-500 (Nanovea, Irvine, CA, USA) was used with a nanomodule equipped with a precision piezo drive and a highly sensitive, drive-independent load sensor. The measurement method is instrumental indentation using a Berkovich pyramidal indenter, with a load of 200 mN.
To study micro- and nanostructures, a transmission electron microscope (TEM) JEM 2100 (JEOL, Tokyo, Japan) at an accelerating voltage of 200 kV was used. To analyze the composition of the coatings, a TEM with the EDX system INCA Energy (OXFORD Instruments, Abingdon, UK) was used. Lamellas were manufactured using a Strata focused ion beam (FIB) 205 (FEI Company, Hillsboro, OR, USA). A comparison of the wear resistance of samples with coatings was carried out when turning 1045 steel on an ACU 500 MRD lathe (Sliven) with a ZMM CU500MRD variable-speed drive, without the use of cutting fluid (dry cutting) tool (carbide inserts SNUN ISO 1832:2012 (WC + 15% TiC + 6% Co)) with the studied coatings. The following cutting geometry and conditions were used: γ = −7°, α = 7°, λ = 0, r = 0.4 mm; feed f = 0.1 rpm, cutting depth ap = 0.5 mm, and cutting speed vc = 300 and 350 m/min. The maximum applicable rational cutting speed was selected, ensuring maximum productivity while maintaining sufficient tool life. In accordance with the ANSI/ASME B94.55M-1985 standard [53], the average width of the flank wear land VB = 0.3 mm, and the maximum width of the flank wear land VBmax = 0.6 mm. An analysis of the recommended VBB values for the turning conditions of 1045 steel under the specified cutting conditions, taking into account the reliability criterion, in this work the wear criterion VBmax = 0.35 mm, was adopted. Five experiments were carried out for the tool with every coating.

3. Results

3.1. Scratch Test Hardness

The coatings have identical hardness (28.3 ± 1.2 and 29.7 ± 0.9 GPa, respectively, for IB and GD). The content of elements in the wear-resistant coating layer is as follows: Al—8.2 ± 4.3 at.%, Ti—42.5 ± 3.7 at.%, Cr—44.8 ± 2.7 at.%.
The surface morphology of the coatings is almost identical; the presence of titanium and chromium microparticles is observed (Figure 2a,b).
Coating IB begins to fail (peeling of coating fragments, critical failure load LC1) at 36 N (Figure 2c). When the maximum load of 40 N is reached, no signs of the destruction of the GD coating (visual or acoustic emission) are observed (Figure 2d).

3.2. Cutting Test When Using Turning Steel 1045 (Cutting Speed vc = 300 and 350 m/min)

The results of the cutting test when using turning steel 1045 show that at a cutting speed vc = 300 m/min, a tool with a GD coating shows slightly less active wear dynamics compared to a tool with an IB coating; however, these differences are insignificant and can partly be offset by scatter values (Figure 3). When the cutting speed increases to vc = 350 m/min, the difference in wear dynamics becomes more noticeable and obvious. After 7 min of cutting, the tool coated with IB technology reached the wear limit criterion (VBmax = 350 μm), while the tool coated with GD technology remains operational and has not reached the wear limit. Since the temperature increases first when the cutting speed increases, it can be assumed that the GD coating has better heat resistance compared to the IB coating. But since the deposition parameters of the coatings are completely identical, except for the stage of cleaning and thermal activation, it can be assumed that the coating better maintains adhesion to the substrate under high-temperature conditions.
To test this assumption, the nature of the wear and the destruction of samples with the resulting coatings was studied in more detail. For further study, coated tool samples worn after cutting 1045 steel at vc = 350 m/min were selected.

3.3. Character of Wear of Cutting Tools with Studied Coatings

The worn rake face of an IB-coated tool shows signs of delamination of the coating from the substrate (this can be seen, in particular, based on the distribution of tungsten). In tools coated with GD, signs of delamination from the substrate are also present, but to a slightly lesser extent, appearing in several small areas of delamination. To study the reasons for this kind of coating destruction, we will study transverse sections (lamellae) cut from the wear boundary of the coatings (indicated by red lines in Figure 4).
Figure 5 shows the general appearance of the lamellae, the locations of which are shown in Figure 4. SAED phase analysis showed the presence of the dominant cubic phase (Ti,Al,Cr)n Fm3m in both coatings, while in the IB coating there is also an insignificant presence of the hexagonal phase AlN P6.3mc. Given that the aluminum content in the IB and GD coatings is almost identical, the presence/absence of this phase can rather be associated with the accuracy limits of the SAED method. The coating thickness is about 3 microns.

3.3.1. Heating by Ion Bombardment with Plasma Generation by Arc Evaporators (IB)

The interface between the coating and the substrate has a rather complex layered structure (Figure 6a). A study of the distribution of elements in these layers shows that the layer, dark in contrast (point 3 in Figure 6b), with a thickness of about 20 nm, has a high cobalt content. This layer also contains the presence of iron and a high content of chromium and aluminum, with a lower titanium content relative to neighboring layers. Directly adjacent to the substrate is a light-colored layer with a high titanium content, also containing cobalt, chromium, and aluminum. The examination of another interface region (Figure 6c) also shows alternating layers with high cobalt and titanium content, but in this case, they are less differentiated. In the layer adjacent to the substrate (point 3 in Figure 6c), noticeable diffusion of tungsten is also observed. In both cases under consideration, chromium diffuses into the substrate to a depth of up to 200 nm.
To confirm the discovered patterns, we analyze a lamella cut from another sample (Figure 7). The general pattern shows the presence of a layer with a high cobalt content (in some cases, above 40 at.%, see Figure 7d). In most cases, there is a layer directly adjacent to the surface of the substrate with a high titanium content (80–98 at.%, see Figure 7a,d,e). In two cases (Figure 7b,c), such a layer is not observed; a layer with a high cobalt content is directly adjacent to the substrate. In one case (Figure 7d), between layers with a high titanium and cobalt content, a layer with a high (up to 19 at.%) chromium content is formed. This layer also contains a high content of aluminum and molybdenum. The presence of iron in minor quantities in the cobalt-rich layer is observed in Figure 7d (point 6) and Figure 7e (point 5).

3.3.2. The Heating of the Substrate Surface by a Glow Discharge (GD)

Let us consider the structure and composition of the layer formed when the substrate surface is heated by the GD method. The coating–substrate interface also has a layered structure (Figure 8a). In this case, there is no layer with a high cobalt content; in some areas, the presence of cobalt is observed in extremely small quantities. There is also a slight presence of iron and molybdenum, their content being significantly lower than that observed in the study of IB coatings. In some cases (Figure 8b,d), tungsten diffuses into the titanium-rich layer adjacent to the substrate.

4. Discussion

The formation of a layered structure, including a layer of almost pure titanium and a layer with a high cobalt content and the possible inclusion of some additional elements (for example, iron), which are absent both in the composition of the coating and in the composition of the substrate, requires some discussion. It was previously established [5] that ion etching with an inert gas leads to faster removal of carbides than of the cobalt matrix. On the contrary, etching with metal ions provides the effect of active sputtering of the cobalt binder. Thus, we can propose the following hypothesis for the formation of a layered structure including a cobalt layer. Titanium ions, when cutting into the surface of a substrate due to collisions, transfer their kinetic energy to surface atoms [1,41]. Since the atomic mass of cobalt (58.93) is comparable to the mass of titanium (47.86) and significantly less than the mass of tungsten (183.84), cobalt atoms are more likely to be knocked out from the surface of the substrate (Figure 9a). Thus, a rarefied cloud of cobalt atoms knocked out from the surface is formed, and titanium atoms form a layer of nanometric thickness on the surface of the substrate (Figure 9b). In this case, cobalt atoms are attracted to the surface of the substrate and at some point, they are re-deposited to form a corresponding layer saturated with cobalt (Figure 9c). Regarding the content of iron and some other elements in the nanolayer under consideration, it can be assumed that during the process of ion etching, the flow of ions can also knock out atoms of iron and some other elements from the fastening equipment elements (made of stainless steel). Similar to cobalt atoms, atoms of these elements (in particular, iron) can settle on the surface of the substrate during the process of thermal activation before the deposition of the adhesive sublayer.
Thus, in the process of ion bombardment with plasma generation by arc evaporators, a layer with a complex structure and composition is formed at the boundary of the coating and substrate, which may include the following:
  • A diffusion layer in the substrate (up to 200 nm thick). The diffusion of chromium and, possibly, titanium is observed (identification of titanium diffusion is difficult due to its also being present in the composition of the substrate—TiC).
  • A layer with a dominant titanium content (30–50 nm thick).
  • A layer with a high cobalt content and the possible presence of elements from the equipment (in particular, iron and molybdenum). The composition of this layer is almost impossible to control.

5. Conclusions

The properties of coatings obtained using two surface preparation methods were compared: heating and etching by ion bombardment with plasma generation by arc evaporators (IB) and heating and etching by a glow discharge (GD). A Ti-TiN-(Ti,Cr,Al)N coating was deposited. We had the following findings:
  • The use of heating when exposed to gas ions of a glow discharge provides a smaller spread in the temperature of the samples throughout the chamber volume compared to heating by ion bombardment with plasma generation by arc evaporators;
  • The IB coating begins to fail at 36 N. When the maximum load of 40 N is reached, there are no signs of failure of the GD coating;
  • The cutting test results for turning 1045 steel show that at the cutting speed vc = 300 m/min, the GD-coated tool shows slightly less active wear dynamics compared to the IB-coated tool. When the cutting speed increases to vc = 350 m/min, the difference in wear dynamics becomes more noticeable and obvious. After 7 min of cutting, the IB-coated tool reached the wear limit criterion (VBmax = 350 μm), while the GD-coated tool remained functional and had not reached the wear limit value;
  • In the process of ion bombardment, a layer of complex structure and composition is formed at the boundary of the coating and substrate, which may include the following:
    o
    A diffusion layer in the substrate (up to 200 nm thick). The diffusion of chromium and possibly titanium is observed;
    o
    A layer with a dominant titanium content (30–50 nm thick);
    o
    A layer with a high cobalt content and the possible presence of elements of other elements (in particular iron and molybdenum). This layer is formed only when using heating and etching by ion bombardment with plasma generation by arc evaporators.
  • The formation of a layer with a high molybdenum content may be associated with sputtering of cobalt atoms from the substrate by a flow of metal ions, followed by the reverse deposition of cobalt;
  • A layer with a high cobalt content and the presence of other (contaminant) elements can negatively affect the overall adhesion strength of the coating and the substrate. This issue requires additional study.
Thus, the method of heating and etching by a glow discharge (GD) can be effectively used in the process of the deposition of coatings using the PVD method.

Author Contributions

Conceptualization, Y.B. and A.V.; methodology, Y.B., A.V., C.S., A.S. and F.M.; resources, S.G.; data curation, C.S. and I.S.; investigation, C.S., A.S. and I.S.; supervision, S.G. and A.V.; writing—original draft preparation, A.V. and Y.B.; writing—review and editing, A.V., C.S. and M.V.; project administration, C.S. and M.V. All authors have read and agreed to the published version of the manuscript.

Funding

This work was funded by the state assignment of the Ministry of Science and Higher Education of the Russian Federation, Project No. FSFS-2023-0003.

Data Availability Statement

Data are contained within the article.

Acknowledgments

The study used the equipment from the Center for Collective Use of Moscow State Technological University STANKIN (agreement no. 075-15-2021-695, 26/07/2021).

Conflicts of Interest

The authors declare no conflicts of interest.

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Figure 1. A schematic diagram of the VIT-2 installation for coating deposition. 1—gas leak; 2—vacuum system; 3—pyrometer; 4—CAA-PVD system evaporators; 5—vacuum chamber; 6—rotary table; 7—planetary rotating equipment.
Figure 1. A schematic diagram of the VIT-2 installation for coating deposition. 1—gas leak; 2—vacuum system; 3—pyrometer; 4—CAA-PVD system evaporators; 5—vacuum chamber; 6—rotary table; 7—planetary rotating equipment.
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Figure 2. Surface morphology of coatings IB (a) and GD (b). View of scribing furrow and its characteristic areas for IB coating (c) and GD coating (d).
Figure 2. Surface morphology of coatings IB (a) and GD (b). View of scribing furrow and its characteristic areas for IB coating (c) and GD coating (d).
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Figure 3. The dependence of wear on the flank surface of a cutting tool on cutting time. The wear criterion VBmax = 0.35 mm (the dotted line indicates the value of permissible (maximum) wear of the cutting tool).
Figure 3. The dependence of wear on the flank surface of a cutting tool on cutting time. The wear criterion VBmax = 0.35 mm (the dotted line indicates the value of permissible (maximum) wear of the cutting tool).
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Figure 4. A general view of the front surface of the tool, mapping the distribution of elements and the location of the lamella cutting (red line).
Figure 4. A general view of the front surface of the tool, mapping the distribution of elements and the location of the lamella cutting (red line).
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Figure 5. A general view of the lamella and the results of the SAED phase analysis of the IB coating (a) and GD coating (b).
Figure 5. A general view of the lamella and the results of the SAED phase analysis of the IB coating (a) and GD coating (b).
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Figure 6. A study of the interface region between the substrate and the coating during IB: (a) the layered structure of the interface region; (b,c) an analysis of the content of chemical elements.
Figure 6. A study of the interface region between the substrate and the coating during IB: (a) the layered structure of the interface region; (b,c) an analysis of the content of chemical elements.
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Figure 7. (ae) An analysis of the content of chemical elements in the interface region between the coating and the substrate during IB use.
Figure 7. (ae) An analysis of the content of chemical elements in the interface region between the coating and the substrate during IB use.
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Figure 8. A study of the interface region between the substrate and the coating using a GD: (a) the layered structure of the interface region; (bg) the analysis of the content of chemical elements.
Figure 8. A study of the interface region between the substrate and the coating using a GD: (a) the layered structure of the interface region; (bg) the analysis of the content of chemical elements.
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Figure 9. A hypothetical diagram of the formation of a layered structure in the area of the substrate-coating interface: (a) titanium ions knock out cobalt atoms from the surface of the substrate, (b) a titanium layer is formed, while the cobalt atoms knocked out from the surface drift, gradually losing energy and beginning to re-deposit on the surface of the substrate, (c) a layer rich in cobalt is formed above the titanium layer.
Figure 9. A hypothetical diagram of the formation of a layered structure in the area of the substrate-coating interface: (a) titanium ions knock out cobalt atoms from the surface of the substrate, (b) a titanium layer is formed, while the cobalt atoms knocked out from the surface drift, gradually losing energy and beginning to re-deposit on the surface of the substrate, (c) a layer rich in cobalt is formed above the titanium layer.
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MDPI and ACS Style

Grigoriev, S.; Volosova, M.; Bublikov, Y.; Sotova, C.; Milovich, F.; Seleznev, A.; Shmakov, I.; Vereschaka, A. A Study of the Features of Coating Deposition on a Carbide Substrate Using Preliminary Etching with Glow-Discharge Plasma. Surfaces 2024, 7, 920-937. https://doi.org/10.3390/surfaces7040060

AMA Style

Grigoriev S, Volosova M, Bublikov Y, Sotova C, Milovich F, Seleznev A, Shmakov I, Vereschaka A. A Study of the Features of Coating Deposition on a Carbide Substrate Using Preliminary Etching with Glow-Discharge Plasma. Surfaces. 2024; 7(4):920-937. https://doi.org/10.3390/surfaces7040060

Chicago/Turabian Style

Grigoriev, Sergey, Marina Volosova, Yuri Bublikov, Catherine Sotova, Filipp Milovich, Anton Seleznev, Ilya Shmakov, and Alexey Vereschaka. 2024. "A Study of the Features of Coating Deposition on a Carbide Substrate Using Preliminary Etching with Glow-Discharge Plasma" Surfaces 7, no. 4: 920-937. https://doi.org/10.3390/surfaces7040060

APA Style

Grigoriev, S., Volosova, M., Bublikov, Y., Sotova, C., Milovich, F., Seleznev, A., Shmakov, I., & Vereschaka, A. (2024). A Study of the Features of Coating Deposition on a Carbide Substrate Using Preliminary Etching with Glow-Discharge Plasma. Surfaces, 7(4), 920-937. https://doi.org/10.3390/surfaces7040060

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