2015
DOI: 10.1002/ppap.201400220
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Structural Characterization of γ‐Terpinene Thin Films Using Mass Spectroscopy and X‐Ray Photoelectron Spectroscopy

Abstract: Understanding the polymerization mechanism of a precursor is indispensable to enhance the requisite material properties. In situ mass spectroscopy and X‐ray photoelectron spectroscopy is used in this study to understand the RF plasma polymerization of γ‐terpinene. High‐resolution mass spectra positive ion mass spectrometry data of the plasma phase demonstrates the presence of oligomeric species of the type [M+H]+ and [2M+H]+, where M represents a unit of the starting material. In addition, there is abundant fr… Show more

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Cited by 26 publications
(31 citation statements)
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“…The reduction in E g as a result of power deposition was attributed to dangling bonds that formed in the polymer structure during the fabrication process. At low input power density, a low concentration of dangling bonds are created due to their saturation with hydrogen atoms, whereas higher input power enhances the fragmentation rate in the plasma field [41], which highly accelerates the formation of chains with unsaturated bonds [42]. The relatively high energy gap for geranium plasma polymer films is in good agreement with the low conductivity values acquired in this study.…”
Section: Resultssupporting
confidence: 86%
“…The reduction in E g as a result of power deposition was attributed to dangling bonds that formed in the polymer structure during the fabrication process. At low input power density, a low concentration of dangling bonds are created due to their saturation with hydrogen atoms, whereas higher input power enhances the fragmentation rate in the plasma field [41], which highly accelerates the formation of chains with unsaturated bonds [42]. The relatively high energy gap for geranium plasma polymer films is in good agreement with the low conductivity values acquired in this study.…”
Section: Resultssupporting
confidence: 86%
“…3(a) displays the presence of strong carbon and oxygen at peaks at 282 and 531 eV, respectively. The C 1 s peaks for geranium polymers were fitted with four peaks, which can be ascribed to major hydrocarbon C–C/C–H (BE = 284.9 eV), and other functional groups, such as ether C–O (BE = 286.2 eV), carbonyl C = O (BE = 287.5 eV), and ester O–C = O (BE = 288.9 eV) 29 , as seen in Fig. 3(c).
Figure 3Full scan XPS spectrum of pristine polymer ( a ) and composite ( b ) thin films.
…”
Section: Resultsmentioning
confidence: 99%
“…The reduction in the peak intensities and disappearance of some peaks in the polymer can be interpreted as the precursor molecules being partially dissociated as a result of being subjected to the RF plasma field [ 33 ]. However, the absorption band of C=O asymmetric stretching observed in the 1800−1600 cm −1 region was possibly due to the post oxidation of the trapped free radicals, confined during film formation [ 34 ].…”
Section: Resultsmentioning
confidence: 99%