2008
DOI: 10.1016/j.surfcoat.2008.06.057
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Microstructure and mechanical properties of SiCN hard films deposited by an arc enhanced magnetic sputtering hybrid system

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Cited by 41 publications
(21 citation statements)
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“…They are promising coating materials in advanced technology. Most recent reports [1][2][3][4][5][6] revealed many unique features of SiCN films which may be used as hard, dense, and high temperatureand corrosion-resistant coatings for metals (giving excellent tribological behavior), as well as highly selective gas separation membranes. [7] Of the various methods based on the gas-phase processes which are used for the formation of SiCN films, remote microwave plasma (RP)CVD from organosilicon precursors, developed in our laboratory, appeared to be a very useful technique, offering wellcontrolled deposition conditions free of film-damaging effects.…”
mentioning
confidence: 99%
“…They are promising coating materials in advanced technology. Most recent reports [1][2][3][4][5][6] revealed many unique features of SiCN films which may be used as hard, dense, and high temperatureand corrosion-resistant coatings for metals (giving excellent tribological behavior), as well as highly selective gas separation membranes. [7] Of the various methods based on the gas-phase processes which are used for the formation of SiCN films, remote microwave plasma (RP)CVD from organosilicon precursors, developed in our laboratory, appeared to be a very useful technique, offering wellcontrolled deposition conditions free of film-damaging effects.…”
mentioning
confidence: 99%
“…In addition, the diffraction peaks (2 0 0) shifted to higher angles with the increasing of TMS flows, which corresponds to a progressive reduction of the lattice parameter, suggests the incorporation of Si into the cubic CrN structure [48,52,53]. In addition, the diffraction peaks (1 1 1) and (2 2 0) disappeared as a result of amorphous structure and lower residual stress [56], which is due to the substitution of smaller Si atoms for Cr sites in the CrN lattice [54], and then leads to the distortion of the CrN lattices [53]. According to the Scherrer's equation expressed as: D = 0.9 /(ˇ cos Â), where D is the mean crystallite size, is the X-ray wavelength, ␤ is the peak width at half the maximum intensity (FWHM), and  is the Bragg's angle.…”
Section: Resultsmentioning
confidence: 93%
“…The Si 2p spectra of samples have been deconvoluted into the five possible oxidation states (Si 0 , Si 1+ , Si 2+ , Si 3+ and Si 4+ ). The energy [25][26][27][28]. When the thin films annealed at RT -400 • C, the peaks of Si 4+ and O 2− were weak, whereas the peaks of Si 0 and O 4/x− were intensive, which indicated that most of the Si Si x O 4−x (1 < x < 3) clusters were in the thin films.…”
Section: Resultsmentioning
confidence: 99%