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Luttinger-liquid behaviour in carbon nanotubes
Electron transport in conductors is usually well described by Fermi-liquid theory, which assumes that the energy states of the electrons near the Fermi level EF are not qualitatively altered by Coulomb interactions. In one-dimensional systems, however, even weak Coulomb interactions cause strong per...
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Published in: | Nature (London) 1999-02, Vol.397 (6720), p.598-601 |
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Main Authors: | , , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | Electron transport in conductors is usually well described by Fermi-liquid
theory, which assumes that the energy states of the electrons near the Fermi
level EF are not qualitatively altered by Coulomb interactions.
In one-dimensional systems, however, even weak Coulomb interactions cause
strong perturbations. The resulting system, known as a Luttinger liquid, is
predicted to be distinctly different from its two- and three-dimensional counterparts. For example, tunnelling into a Luttinger liquid at energies near
the Fermi level is predicted to be strongly suppressed, unlike in two- and
three-dimensional metals. Experiments on one-dimensional semiconductor wires, have been interpreted by using Luttinger-liquid
theory, but an unequivocal verification of the theoretical predictions has
not yet been obtained. Similarly, the edge excitations seen in fractional
quantum Hall conductors are consistent with Luttinger-liquid behaviour, , but recent experiments failed to confirm the predicted
relationship between the electrical properties of the bulk state and those
of the edge states. Electrically conducting single-walled carbon
nanotubes (SWNTs) represent quantum wires that may
exhibit Luttinger-liquid behaviour, . Here
we present measurements of the conductance of bundles ('ropes')
of SWNTs as a function of temperature and voltage that agree with predictions
for tunnelling into a Luttinger liquid. In particular, we find that the conductance
and differential conductance scale as power laws with respect to temperature
and bias voltage, respectively, and that the functional forms and the exponents
are in good agreement with theoretical predictions. |
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ISSN: | 0028-0836 1476-4687 |
DOI: | 10.1038/17569 |