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To measure the contact resistance of the deposited films, transfer length method (TLM) was used.
These highly conductive and transparent films transfer electrons by the carbon nanotube networks with a slightly deformed tube-to-tube junction feature.
GPC and NMR data for a-PF-1-12; analysisSEM analysis of the SWNT thin films; Raman spectra of SWNT thin films; transfer curves at high source-drain bias and width-normalized on-currents and on-conductances; transconductance data; capacitance; and contact resistance calculations.
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Fig. 1 a Raman spectra for graphene films transferred to silicon substrate.
However, whilst the LB films transferred at lower pressure (12 mN m−1) displayed reasonable emission, the films transferred at higher pressure (30 mN m−1) resulted in significant quenching of emission.
Additionally, we observed that Au/Ti films transferred with OrmoStamp®; working stamps have significantly lower surface roughness (∼ 1 nm) as compared to identical films transferred with PDMS working stamps (∼3 6 nm).
Raman spectroscopy indicates that graphene films transferred to insulating substrates are of high quality.
One such example consists of few-layer CVD grown graphene films transferred onto elastic substrates, as shown in the left panel of Figure 12b [240].
Cyclic voltammetry on those Co-hcf films, transferred on gold coated glass, indicates the presence of a surface couple corresponding to Fe CN 63−/Fe CN 64− system.
Grazing-incidence X-ray diffraction (in situ) and scanning electron microscopy (of films transferred to substrates) reveal that oriented growth occurs via two distinct mechanisms.
Wafers containing cross-linked multilayers were exposed to pH = 8 for 24 h to remove poly N-vinylpyrrolidone) from cross-linked poly N-vinylpyrrolidoneransfromed to pH = 4 to deswell the films, and dried.
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