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Chiral effects in normal and superconducting carbon nanotube-based nanostructures
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10.1063/1.3518334
/content/aip/journal/ltp/36/10/10.1063/1.3518334
http://aip.metastore.ingenta.com/content/aip/journal/ltp/36/10/10.1063/1.3518334
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

Transmission coefficient (a) and backward scattering phase (b) as a function of chiral angle at different values of potential strength U0: the solid curve corresponds to , the dashed curve, to .

Image of FIG. 2.
FIG. 2.

Persistent current as a function of magnetic flux for different values of the chiral angle near the off-resonance point ; and results in (this integer represents the 20-th off-resonance point counted from in ): the solid curve corresponds to , the dashed curve to .

Image of FIG. 3.
FIG. 3.

The Josephson current (in units of ) in a long junction, ; the solid curves correspond to the chiral resonance and two off-resonance cases and (symmetric junction); the corresponding currents in an asymmetric junction are represented by the dashed curves.

Image of FIG. 4.
FIG. 4.

The distribution of the number of energy levels over the level spacing (normalized by ) for and different chiral angles: to (a), (b), (c), and (d). For the armchair nanotube we have two sets of equidistant energy levels: and 0.36. The distribution for and is shown here.

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/content/aip/journal/ltp/36/10/10.1063/1.3518334
2010-12-10
2014-04-19
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Chiral effects in normal and superconducting carbon nanotube-based nanostructures
http://aip.metastore.ingenta.com/content/aip/journal/ltp/36/10/10.1063/1.3518334
10.1063/1.3518334
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