SU(12) Kondo Effect in Carbon Nanotube Quantum Dot
arXiv:1310.6563 · doi:10.1103/PhysRevB.89.195110
Abstract
We study the Kondo effect in a CNT(left lead)-CNT(QD)-CNT(right lead) structure. Here CNT is a single-wall metallic carbon nanotube, for which 1) the valence and conduction bands of electrons with zero orbital angular momentum () coalesc at the two valley points and of the first Brillouin zone and 2) the energy spectrum of electrons with has a gap whose size is proportional to . Following adsorption of hydrogen atoms and application of an appropriately designed gate potential, electron energy levels in the CNT(QD) are tunable to have: 1) two-fold spin degeneracy; 2) two-fold isospin (valley) degeneracy; 3) three-fold orbital degeneracy . As a result, an SU(12) Kondo effect is realized with remarkably high Kondo temperature. Unlike the SU(2) case, the low temperature conductance and magnetic susceptibility have a peak at finite temperature. Moreover, the magnetic susceptibilities for parallel and perpendicular magnetic fields (WRT the tube axis) display anisotropy with a universal ratio that depends only on the electron's orbital and spin factors.
18 pages, 11 figures, discussions expanded, Appendix extended, references added
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- Effects of strong electron interactions and resonance scattering on power output of nano-devices
- Poor man's scaling: Coqblin--Schrieffer model revisited
- Thermoelectric transport and current noise through a multilevel Anderson impurity: Three-body Fermi-liquid corrections in quantum dots and magnetic alloys
- The role of spin-flip assisted or orbital mixing tunneling on transport through strongly correlated multilevel quantum dot
- Fractional shot noise of an SU(N) Kondo system