2003
DOI: 10.1016/j.spmi.2004.03.038
|View full text |Cite
|
Sign up to set email alerts
|

Controlling currents through molecular wires

Abstract: We investigate the possibility of controlling by means of external laser fields both the current through molecular wires and the corresponding noise properties. It is found that an appropriate off-resonant driving field reduces the coherent transport across the molecule resulting in a strong current suppression. The relative level of transport noise, characterized by a Fano factor, exhibits characteristic maxima and minima near regimes of current suppression. In a three-terminal configuration, the field allows… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
9
0

Year Published

2005
2005
2020
2020

Publication Types

Select...
6

Relationship

0
6

Authors

Journals

citations
Cited by 9 publications
(9 citation statements)
references
References 26 publications
0
9
0
Order By: Relevance
“…1 can be analyzed in terms of two competing Rabi oscillations: The field driven oscillations between the HOMO and LUMO of the donor (m = 0, 1) induced by the external laser field and the bridge mediated tunneling (superexchange) oscillations between the LUMOs of the donor and acceptor. The field driven frequency is defined by the detuning of the field from the donor resonance and the field intensity, 1 = (ε 1 − ε 0 − ω E ) 2 + (2 μE 0 ) 2 /¯, while the intra-molecular frequency is defined by the donor-acceptor level mismatch and the effective electronic coupling, 43 Figure 3 shows numerical simulations of current induced by CW laser for the model (2)-(5) treated within the mapping to a stationary problem (10). Current is shown as a function of the external field parameters: intensity ( Fig.…”
Section: Resultsmentioning
confidence: 99%
See 2 more Smart Citations
“…1 can be analyzed in terms of two competing Rabi oscillations: The field driven oscillations between the HOMO and LUMO of the donor (m = 0, 1) induced by the external laser field and the bridge mediated tunneling (superexchange) oscillations between the LUMOs of the donor and acceptor. The field driven frequency is defined by the detuning of the field from the donor resonance and the field intensity, 1 = (ε 1 − ε 0 − ω E ) 2 + (2 μE 0 ) 2 /¯, while the intra-molecular frequency is defined by the donor-acceptor level mismatch and the effective electronic coupling, 43 Figure 3 shows numerical simulations of current induced by CW laser for the model (2)-(5) treated within the mapping to a stationary problem (10). Current is shown as a function of the external field parameters: intensity ( Fig.…”
Section: Resultsmentioning
confidence: 99%
“…Here we seek not only charge pumping but also path selectivity during pumping, controlled by the external excitation. We start our consideration from the effective steady-state model (defined by the transformation (10) and the rotating wave approximation) applied to the Hamiltonian (11)- (14). The "standard" parameters as in the charge pump calculations with the donor-acceptor coupling are used here, where the electronic coupling between the donor LUMO and sites 3 and 4 (see Fig.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…(9) and (10). The starting points are expressions for charge and energy (phononassisted) fluxes within the nonequilibrium Green functions (NEGF) technique.…”
Section: Appendix B: Charge and Energy Fluxes In The Nca Within Pp-negfmentioning
confidence: 99%
“…7,8 Coherent control of transport in molecular junctions is one of the focuses of research in this field. [9][10][11][12][13][14] Another focus is the dynamics of energy transfer between plasmonic and molecular excitations. [15][16][17][18][19] The importance of quantum coherence in energy transfer was demonstrated recently in studies of the initial stages of photosynthesis.…”
Section: Introductionmentioning
confidence: 99%