Strong Electron Tunneling through a Small Metallic Grain
arXiv:cond-mat/9605133 · doi:10.1134/1.567117
Abstract
Electron tunneling through mesoscopic metallic grains can be treated perturbatively only provided the tunnel junction conductances are sufficiently small. If it is not the case, fluctuations of the grain charge become strong. As a result (i) contributions of all -- including high energy -- charge states become important and (ii) excited charge states become broadened and essentially overlap. At the same time the grain charge remains discrete and the system conductance -periodically depends on the gate charge. We develop a nonperturbative approach which accounts for all these features and calculate the temperature dependent conductance of the system in the strong tunneling regime at different values of the gate charge.
revtex, 8 pages, 2 .ps figures
References in corpus (1)
Cited by in corpus (16)
- Superconductivity in one dimension
- Coulomb Interaction and Quantum Transport through a Coherent Scatterer
- Nonequilibrium theory of Coulomb blockade in open quantum dots
- Cotunneling and renormalization effects for the single-electron transistor
- Strong Electron Tunneling through Mesoscopic Metallic Grains
- Strong Charge Fluctuations in the Single-Electron Box: A Quantum Monte Carlo Analysis
- Strong Tunneling and Coulomb Blockade in a Single-Electron Transistor
- Electron Transport in Granular Metals
- Effect of the Tunneling Conductance on the Coulomb Staircase
- Conductance of the single-electron transistor: A comparison of experimental data with Monte Carlo calculations
- Coulomb blockade in one-dimensional arrays of high conductance tunnel junctions
- Conductance of the Single Electron Transistor for Arbitrary Tunneling Strength
- Charge Fluctuations in the Single Electron Box
- Persistent current noise and electron-electron interactions
- Transport in metallic multi-island Coulomb blockade systems: A systematic perturbative expansion in the junction transparency
- Persistent current noise in normal and superconducting nanorings