2007
DOI: 10.1021/nl071228o
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Electronic Transport in Single Molecule Junctions:  Control of the Molecule-Electrode Coupling through Intramolecular Tunneling Barriers

Abstract: We report on single molecule electron transport measurements of two oligophenylenevinylene (OPV3) derivatives placed in a nanogap between gold (Au) or lead (Pb) electrodes in a field effect transistor device. Both derivatives contain thiol end groups that allow chemical binding to the electrodes. One derivative has additional methylene groups separating the thiols from the delocalized pi-electron system. The insertion of methylene groups changes the open state conductance by 3-4 orders of magnitude and changes… Show more

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Cited by 157 publications
(137 citation statements)
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References 36 publications
(73 reference statements)
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“…Additionally, the methyl substitution increases the dipole moment per repeat unit und, thus, boosts the net effect of the dipoles. To anchor the SAMs to a Au substrate, we used methylene thiolate, where the methylene serves to decouple the π‐system of the SAM from the extended electronic states in the Au substrate (cf., Figure 3a) 44. For the present proof of principles simulations, we assembled the molecules in a comparatively large unit cell (3 × 2√3) in an upright‐standing position (for further details see Section 4; note that a significant tilt of the molecule would reduce the net effect as for the above‐discussed collective effects only the dipole moment perpendicular to the substrate surface counts).…”
Section: Resultsmentioning
confidence: 99%
“…Additionally, the methyl substitution increases the dipole moment per repeat unit und, thus, boosts the net effect of the dipoles. To anchor the SAMs to a Au substrate, we used methylene thiolate, where the methylene serves to decouple the π‐system of the SAM from the extended electronic states in the Au substrate (cf., Figure 3a) 44. For the present proof of principles simulations, we assembled the molecules in a comparatively large unit cell (3 × 2√3) in an upright‐standing position (for further details see Section 4; note that a significant tilt of the molecule would reduce the net effect as for the above‐discussed collective effects only the dipole moment perpendicular to the substrate surface counts).…”
Section: Resultsmentioning
confidence: 99%
“…Óñïåõè ïîñëåäíåãî äåñÿòèëåòèÿ â îáëàñòè ìîëåêóëÿðíîé ýëåêòðîíèêè, â ïåðâóþ î÷åðåäü, ýêñïåðèìåíòàëüíûå, çàâåðøèëèñü, â ÷àñòíîñ-òè, ñîçäàíèåì îäíîìîëåêóëÿðíîãî îäíîýëåêò-ðîííîãî ïîëåâîãî òðàíçèñòîðà (Single-Molecule Single-Electron Transistor, SM-SET) [1][2][3][4][5][6][7][8][9], ñõå-ìàòè÷åñêè ïîêàçàííîãî íà ðèñ. 1.…”
Section: ââåäåíèåmentioning
confidence: 99%
“…For further reading on the physics of molecule/electrode contacts, on the influence of the contact on molecular energetics and how it impacts electron transport phenomenon in molecular devices, the interested reader can found more in recent review papers [97][98][99]. However, this chemical link acts also as a tunnel barrier for electron transfer between the electrode and the molecule [101]. As a consequence, the conductance of a molecular junction is usually small (typically below 10 -2 G 0 , where G 0 =2e 2 /h=77.5µS is the conductance quantum) [49,51,95,[102][103][104].…”
Section: B At the "Device-like" Levelmentioning
confidence: 99%