We report on the interfacial structure, the current−voltage (I−V) characteristics, and contact resistance of
metal electrode−carbon nanotube contacts for five metals, Ti, Pd, Pt, Cu, and Au, based on first-principles
quantum mechanical density functional and matrix Green's function methods. We find that Ti leads to the
lowest contact resistance followed by Pd, Pt, Cu, and Au. The sequence, Ti ≫ Pd > Pt > Cu > Au, correlates
well with the predicted cohesive strength of the electrode−carbon interface. In addition Ti leads to linear
I−V characteristics up to ∼1 V, suggesting an Ohmic contact for both metallic and semiconductor nanotubes.
However, the high reactivity of the Ti electrode at the contact to the nanotube distorts the nanotube structure.
The microphase structure of noncrystalline poly(ethylene-co-13.3 mol % methacrylic acid)
(E-0.133MAA) ionomers was investigated by using infrared (IR) spectroscopic, X-ray scattering, differential
scanning calorimetric (DSC), and dielectric measurements. The noncrystallinity was confirmed by small-angle X-ray scattering (SAXS) and DSC studies, which has enabled a quantitative analysis of the SAXS
ionic peak associated with ionic aggregates without being perturbed by the polyethylene lamellae peak.
In 60% neutralized Na ionomer, it was revealed that almost 100% of MAA side groups including
unneutralized COOH are incorporated into the ionic aggregates with an average ionic core radius (R
1) of
∼6 Å. The dielectric relaxation studies showed that the ionic aggregates form a microphase-separated
ionic cluster. Analysis of dielectric strengths indicated the most (∼90%) of the COONa groups are present
in the ionic cluster. On the other hand, in the 60% neutralized Zn ionomer, both SAXS and dielectric
studies indicated that the ionic aggregates with R
1 ∼ 4 Å are almost isolated and dispersed in the matrix;
the formation of ionic cluster was not recognized. Similarly to partly crystalline E-MAA ionomers, all
noncrystalline E-0.133MAA ionomers exhibited an endothermic peak at 320−330 K (labeled T
i) on the
first heating, depending on the aging time at room temperature. Several factors that would be critical
for the DSC T
i peak were discussed. It was concluded that the DSC T
i peak is certainly associated with
changes of the state of ionic aggregate region.
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