Fine structure in the off-resonance conductance of small Coulomb blockade systems
arXiv:cond-mat/9612068 · doi:10.1103/PhysRevB.55.15735
Abstract
We show how a fine, multiple-peak structure can arise in the off-resonance, zero-bias conductance of Coulomb blockade systems. In order to understand how this effect comes about one must abandon the orthodox, mean-field understanding of the Coulomb blockade phenomenon and consider quantum fluctuations in the occupation of the single-particle electronic levels. We illustrate such an effect with a spinless Anderson-like model for multi-level systems and an equation-of-motion method for calculating Green's functions that combines two simple decoupling schemes.
5 pages, 3 figures, postscript file also available at http://www.pa.uky.edu/~palacios/papers/eom.ps One figure added. Discussion of results extended
References in corpus (5)
- Low Temperature Transport through a Quantum Dot: The Anderson Model out of Equilibrium
- Electron correlation resonances in the transport through a single quantum level
- Capacitance spectroscopy in quantum dots: Addition spectra and decrease of tunneling rates
- Coherent tunnelling through two quantum dots with Coulomb interaction
- Low-lying excitations of Quantum Hall Droplets
Cited by in corpus (8)
- Transport in multilevel quantum dots: from the Kondo effect to the Coulomb blockade regime
- Kondo effect in quantum dots coupled to ferromagnetic leads with noncollinear magnetizations
- Green function techniques in the treatment of quantum transport at the molecular scale
- Magnetoresistance of a quantum dot with spin-active interfaces
- Molecular junctions in the Coulomb blockade regime: rectification and nesting
- Spin polarized current and shot noise in carbon nanotube quantum dot in the Kondo regime
- Spin-polarized transport through a single-level quantum dot in the Kondo regime
- Bistability in the Tunnelling Current through a Ring of Coupled Quantum Dots