No data available.
Please log in to see this content.
You have no subscription access to this content.
No metrics data to plot.
The attempt to load metrics for this article has failed.
The attempt to plot a graph for these metrics has failed.
Quantum transport with two interacting conduction channels
3. M. Galperin
, A. Nitzan
, and M. A. Ratner
, preprint arXiv:0909.0915
9.It should be emphasized that the theory addresses only locally stable states that will not persist beyond some finite lifetime, and do not imply multistability in the thermodynamic sense.
12. L. M. K. Vandersypen, J. M. Elzerman, R. N. Schouten, L. H. W. v. Beveren, R. Hanson, and L. P. Kouwenhoven, Appl. Phys. Lett. 85, 4394 (2004).
15. S. Gustavsson, R. Leturcq, B. Simovic, R. Schleser, T. Ihn, P. Studerus, K. Ensslin, D. C. Driscoll, and A. C. Gossard, Phys. Rev. Lett. 96, 076605 (2006).
22.The “fast” channel carries all the current if the “slow” channel is coupled only to one of the leads.
27. A. Migliore and A. Nitzan, “Irreversibility and hysteresis in redox molecular junctions” (unpublished).
38.Note that while in quantum mechanics damping rates and level widths are synonymous, it is exactly the energetic consequence of the finite lifetime, that is, the level broadening, which is disregarded in the kinetic approximation.
39. S. Datta, Electric Transport in Mesoscopic Systems (Cambridge University Press, Cambridge, 1995).
40. H. Haug and A.-P. Jauho, Quantum Kinetics in Transport and Optics of Semiconductors (Springer, 2008).
Article metrics loading...
Full text loading...
Most read this month