Abstract:In this work, the production of RuN thin films using the reactive direct current magnetron sputtering technique is presented. Samples were grown with varying Ar/N2 ratio with values of 60/40, 80/20, 85/15, 90/10, 95/5, and 100/0. X‐ray photoelectron spectroscopy was employed to determine the presence of RuN before and after a sputtering etching process. According to the high‐resolution of N1s spectra, 3 peaks were identified at 397.4 ± 0.3 eV, 398.3 ± 0.3 eV, and 398.8 ± 0.3 eV binding energies, corresponding … Show more
“…The contribution to the broadening of the metal peaks by oxide formation from an exposure to atmosphere and the nitride formed by the ion exposure experiment are difficult to quantify. The lack of a significant peak shift of the Ru3d peaks indicates that the sample remains mostly metallic, consistent with transition metal nitrides [13]. The O1s peak for air exposed nitrides shares similar difficulties as the contributions from the oxy-nitride and O-H groups from adsorbed water and hydroxides are challenging to deconvolve.…”
Section: Methodssupporting
confidence: 55%
“…The quantification of the nitride and oxynitride is therefore limited to the N1s spectra. Two components of the N1s have been identified, one at 397.3eV corresponding to the nitride and 398.8 eV which is characteristic for an oxynitride for transition metal nitrides exposed to atomsphere [13,30]. The area under the N1s peak corresponded to 18 atomic percent of nitrogen in the measured sample volume, implying implantation of nitrogen within the target.…”
Section: Methodsmentioning
confidence: 92%
“…Ruthenium nitride (RuN x ) is predicted to have a positive enthalpy of formation [11]. The formation energy barrier is overcome by the incidence of energetic nitrogen ions or radicals either by magnetron sputtering [12,13] plasmas or pulsed lasers [14]. The formation of RuN x during sputter measurements would modify the SBE for such combinations involving reactive species leading to larger deviations in model predictions.…”
Ion surface interactions near sputter-threshold are of interest for various plasma facing materials. We report experimental determination of sputter yields for ruthenium films grown on a quartz crystal microbalance and exposed to Ar + and N + 2 ions in the energy range of 50-300 eV. Comparison to semi-empirical models shows agreement to previously reported yields for argon bombardment. In the case of nitrogen, the Yamamura model was modified to account for molecular effects and the yields are found to be between extremes of rigid and non-rigid molecular approximations proposed by Yao. Ex-situ XPS measurements revealed implantation of nitrogen in the ruthenium film after exposure to nitrogen ions. The discrepancy between the models and experimental results for N + 2 bombardment is explained by an increase in the surface binding energy of the target leading to a chemically reduced sputter yield.
“…The contribution to the broadening of the metal peaks by oxide formation from an exposure to atmosphere and the nitride formed by the ion exposure experiment are difficult to quantify. The lack of a significant peak shift of the Ru3d peaks indicates that the sample remains mostly metallic, consistent with transition metal nitrides [13]. The O1s peak for air exposed nitrides shares similar difficulties as the contributions from the oxy-nitride and O-H groups from adsorbed water and hydroxides are challenging to deconvolve.…”
Section: Methodssupporting
confidence: 55%
“…The quantification of the nitride and oxynitride is therefore limited to the N1s spectra. Two components of the N1s have been identified, one at 397.3eV corresponding to the nitride and 398.8 eV which is characteristic for an oxynitride for transition metal nitrides exposed to atomsphere [13,30]. The area under the N1s peak corresponded to 18 atomic percent of nitrogen in the measured sample volume, implying implantation of nitrogen within the target.…”
Section: Methodsmentioning
confidence: 92%
“…Ruthenium nitride (RuN x ) is predicted to have a positive enthalpy of formation [11]. The formation energy barrier is overcome by the incidence of energetic nitrogen ions or radicals either by magnetron sputtering [12,13] plasmas or pulsed lasers [14]. The formation of RuN x during sputter measurements would modify the SBE for such combinations involving reactive species leading to larger deviations in model predictions.…”
Ion surface interactions near sputter-threshold are of interest for various plasma facing materials. We report experimental determination of sputter yields for ruthenium films grown on a quartz crystal microbalance and exposed to Ar + and N + 2 ions in the energy range of 50-300 eV. Comparison to semi-empirical models shows agreement to previously reported yields for argon bombardment. In the case of nitrogen, the Yamamura model was modified to account for molecular effects and the yields are found to be between extremes of rigid and non-rigid molecular approximations proposed by Yao. Ex-situ XPS measurements revealed implantation of nitrogen in the ruthenium film after exposure to nitrogen ions. The discrepancy between the models and experimental results for N + 2 bombardment is explained by an increase in the surface binding energy of the target leading to a chemically reduced sputter yield.
“…In C1s: C, 16 CO, 17 CN, 18 CO 3 . 19 In N1s: MeN (metal nitride), 20,21 CN, 22 CNO, 23 CN and NO, 24,25 to blocking the slip grain border. 47 If the temperature is continuously increasing, the presence of the CO 2 would accelerate the corrosion on the surface and increase the roughness such that the hardness falls abruptly 8 ; besides, the displacement produced by O atoms would have a decisive effect on the oxidation behavior.…”
Section: Results and Analysismentioning
confidence: 99%
“…In C1s: C, 16 CO, 17 CN, 18 CO 3 19 . In N1s: MeN (metal nitride), 20,21 CN, 22 CNO, 23 CN and NO, 24,25 NO, 26 N 2 , 27 NO 2 26 . In O1s: O 2 , 28 C x O y , 29 TiO 2 and ZrO 2 , 30 TiNO x , 31 TiO, 18 CNO, 23 NO x , 32 CO 33 .…”
Currently, studies about the CO 2 gas injection improve the production efficiency of crude oil. The surface interaction between CO 2 and thin films is a large area of research in the scientific community. In this work, we are showing that The TiZrN (coating) + Si (substrate) system immersed on environments of fully CO 2 can interact to below 400 C temperature, because the TiZrN (coating) + Si (substrate) system is broken to temperatures above of the 400 C. The Ti2p, Zr3d, N1s, O1s, and C1s narrow spectra are shown, which illustrate the evolution of TiZrN to TiN x , TiO x , and TiON x compounds and afterwards to TiO 2 and ZrO 2 phases. TiN x , TiO x , and TiON x compounds are responsible for the increase of the micro-hardness (measured through Vickers Hardness Testing) of the system (TiZrN [coating] + Si [substrate]) due to that are found at 400 C thermal treatment. Topographical images obtained by atomic force microscopy showed an increase of the surface roughness due to the thermal treatment. Scanning electron microscopy demonstrated that sample submit to 600 C temperature suffered fracture with small indentations.
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