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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.

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