1998
DOI: 10.1016/s0257-8972(97)00147-3
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Characterizing the remote plasma polymerization of octafluorocyclobutane induced by RF-driven hollow-cathode discharge

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Cited by 13 publications
(12 citation statements)
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“…Similarly, adding Ar gas into the deposition chamber was not found to have a significant effect on roughness or water contact angle behaviour. In all cases the water contact angle was found to be 111 , which is in good agreement with previously reported results [10]. Upon production of a Zisman plot, the critical solid surface tension of the CF x O y films was estimated as 9.3 mN/m, and it was generally found that the higher the surface tension of the liquid investigated, the higher the contact angle with the CF x O y film; although interestingly, polar molecules such as ethanol (35 ) and propan-2-ol (33 ) display remarkably low contact angles.…”
Section: Methodssupporting
confidence: 92%
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“…Similarly, adding Ar gas into the deposition chamber was not found to have a significant effect on roughness or water contact angle behaviour. In all cases the water contact angle was found to be 111 , which is in good agreement with previously reported results [10]. Upon production of a Zisman plot, the critical solid surface tension of the CF x O y films was estimated as 9.3 mN/m, and it was generally found that the higher the surface tension of the liquid investigated, the higher the contact angle with the CF x O y film; although interestingly, polar molecules such as ethanol (35 ) and propan-2-ol (33 ) display remarkably low contact angles.…”
Section: Methodssupporting
confidence: 92%
“…Argyrakis et al [7] employed CF x O y thin films as an anti-adhesion and structure release aide. Grant et al [8,9] examined the growth and structure of CF x O y thin films as a function of the C 4 F 8 gas inlet feed position relative to the plasma zone, while Ningel et al [10] characterised CF x O y thin films deposited onto substrates up to 250 mm in length, reporting that the films exhibited excellent surface homogeneity.…”
Section: Introductionmentioning
confidence: 99%
“…The corresponding peaks in the spectrum of PP-OFCB fall in a comparatively broad band at the region of 1100 to 1400 cm -1 , which is due to a convolution of CF x ( x = 1,2, or 3) stretching modes. The individual CF x peaks located within this broad convoluted band are difficult to assign unambiguously. Two small broad peaks located at 740 and 1740 cm -1 can also be seen in the PP-OFCB spectrum. The former is caused by the vibrations from amorphous fluoro-materials, ,, CF−CF 3 vibration, and zone center CF 2 system stretching, , which implies a traditional polymer chain structure .…”
Section: Resultsmentioning
confidence: 99%
“…The individual CF x peaks located within this broad convoluted band are difficult to assign unambiguously. Two small broad peaks located at 740 and 1740 cm -1 can also be seen in the PP-OFCB spectrum. The former is caused by the vibrations from amorphous fluoro-materials, ,, CF−CF 3 vibration, and zone center CF 2 system stretching, , which implies a traditional polymer chain structure . The latter is due to the vibrations of CCF 2 , −CCF 2 , and −CFCF 2 groups, , which signifies the existence of cross-linking structure in the film .…”
Section: Resultsmentioning
confidence: 99%
“…The presence of these vibrations implies the existence of crosslinking. [38,39] A few small absorption bands emerge at 2850 and 2950 cm…”
mentioning
confidence: 99%