2008
DOI: 10.1134/s1995078008070124
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Scaling analysis of the morphology of nanostructured poly(p-xylylene) films synthesized by vapor deposition polymerization

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Cited by 8 publications
(4 citation statements)
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“…However, the average surface roughness of <1 nm for the 8 nm thick films and the uniformity of the granules make it implausible that DM particles would nucleate and grow in the solution and only deposit in a packed monolayer after reaching a certain size. Thus, DM appears to exhibit three-dimensional island growth similar to that observed, for example, in phthalocyanine 45 or poly(pxylylene) 46 films in contrast to pentacene, 47 p-hexaphenyl, 48 or polyethylene 49 films.…”
Section: ■ Materials and Methodssupporting
confidence: 64%
“…However, the average surface roughness of <1 nm for the 8 nm thick films and the uniformity of the granules make it implausible that DM particles would nucleate and grow in the solution and only deposit in a packed monolayer after reaching a certain size. Thus, DM appears to exhibit three-dimensional island growth similar to that observed, for example, in phthalocyanine 45 or poly(pxylylene) 46 films in contrast to pentacene, 47 p-hexaphenyl, 48 or polyethylene 49 films.…”
Section: ■ Materials and Methodssupporting
confidence: 64%
“…The global scaling exponents were found to follow the dynamic scaling hypothesis with z g = α g /β for various G. With an increase in G from 10 to 10 4 , the average local roughness exponent α l remained close to 0.46 with α l = α g , this observation is unlike the ones obtained in self-affine surfaces [15,35]. The anomalous growth exponent β * was also found to decrease from 0.23(4) to 0.18 (8) with an increase in G. Even though our model is in 1+1D as compared to the 2+1D experiments, our estimates of α l and β * are close to the experimental findings of α ≈ 0.5 to 0.7 and β = 0.25 ± 0.03 obtained from the AFM studies of linear PA-N films grown by VDP [21,51]. The similarity between the experimental and simulational estimates appears to be a coincidence since the dimension of the two systems are totally different.…”
Section: Discussionsupporting
confidence: 83%
“…It is evident from AFM studies that the variations in the molecular size and p-bridge length can cause changes in the microstructure of blended lms. Quantitative investigation of the surface morphology based on the analysis of height correlation functions [35][36][37] (see Fig. S35-S38 †) revealed that N(Ph-2T-DCN-Me) 3 :PC 71 BM, and N(Ph-2T-DCNHex) 3 :PC 71 BM blends are heterogeneous lms.…”
Section: Film Morphologymentioning
confidence: 99%
“…It is evident from AFM studies that the variations in the molecular size and p-bridge length can cause changes in the microstructure of blended lms. Quantitative investigation of the surface morphology based on the analysis of height correlation functions [35][36][37] This journal is © The Royal Society of Chemistry 2014 N(Ph-1T-DCN-Me) 3 :PC 71 BM and N(Ph-3T-DCN-Hex) 3 :PC 71 BM are more homogeneous and can be described by only one correlation length. These nanoscale aggregated domains are benecial to the exciton charge separation, charge transportation and in turn enhance performance of the OSCs.…”
Section: Film Morphologymentioning
confidence: 99%