Low Bias Electron Scattering in Structure ... - Researcher - IBM
Low Bias Electron Scattering in Structure ... - Researcher - IBM
Low Bias Electron Scattering in Structure ... - Researcher - IBM
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Carbon Nanotubes”, Science, 323, p.106 (2009). The region near charge neutrality<br />
po<strong>in</strong>t is more affected by many-body <strong>in</strong>teractions. Whereas, resistivity away from<br />
charge neutrality po<strong>in</strong>t comes primarily from phonon scatter<strong>in</strong>g, hence it’s easier<br />
to ascerta<strong>in</strong> phonon contribution <strong>in</strong> this region.<br />
Chirality dependence of CNT resistivity<br />
The results from numerical simulation predict a very small dependence on tube<br />
chirality. Figure 4b <strong>in</strong> manuscript uses a tube chirality of (28, 0) with a diameter of<br />
2.2 nm. Fig. S3 shows the temperature dependence of the resistivity for (17,15)<br />
and (21,11) and (28,0) CNTs due to tube phonon and SPP modes. These CNTs<br />
have the same diameter but very different chiral angles. It is clear that the SPP<br />
scatter<strong>in</strong>g has very little or no dependence on tube chirality.<br />
2<br />
L m<br />
(μm)<br />
1<br />
(17,15)<br />
(21,11)<br />
(28,00)<br />
0.3<br />
20 100 700<br />
T (K)<br />
Fig. S3. Model results with SPP scatter<strong>in</strong>g for different chirality semiconduct<strong>in</strong>g<br />
CNTs with d=2.2 nm placed over AlN substrate.