2019
DOI: 10.1039/c8sc04199g
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Charge transfer complexation boosts molecular conductance through Fermi level pinning

Abstract: Efficient charge transport across long molecular wires enabled by charge-transfer complexation, through Fermi level pinning of interference features.

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Cited by 51 publications
(37 citation statements)
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“…We also note that this resonance in the transmission spectra has a line-shape of the Breit-Wigner distribution. [34][35][36] The transmission for carbocation states at the Fermi level is more than one order of magnitude higher than that for MGOH, which is in good agreement with the experimental observation. Fig.…”
Section: Resultssupporting
confidence: 87%
“…We also note that this resonance in the transmission spectra has a line-shape of the Breit-Wigner distribution. [34][35][36] The transmission for carbocation states at the Fermi level is more than one order of magnitude higher than that for MGOH, which is in good agreement with the experimental observation. Fig.…”
Section: Resultssupporting
confidence: 87%
“…[5] One challenging area in molecular electronics is the achievement of high and controllable conductance in singlemolecule wires. [6] According to Landauer theory, [7] the conductance G 0 of the quantum point contact follows the equation…”
Section: Introductionmentioning
confidence: 99%
“…As a basic research topic in molecular electronics, single‐molecule wires are essential components for molecular devices and can provide a fundamental understanding for electron transport in single molecules or molecular assemblies, which can lead to advancements in chemistry, biology and materials science . One challenging area in molecular electronics is the achievement of high and controllable conductance in single‐molecule wires . According to Landauer theory, the conductance G 0 of the quantum point contact follows the equation trueG0=2eh∑n=1NTn …”
Section: Introductionmentioning
confidence: 99%
“…3 b. The response time [ 38 , 39 ] ( τ ris representing the time gap from the 90% current peak to the 10% current peak) is determined as 1.8 s, while the recovery time ( τ rec defined oppositely) is 2.4 s, which are nearly a constant in the entire temperature range. For 10 K and 20 K, the delay time of the “tail” structure is about 15.7 s, which is surprisingly absent when the illumination of LED current is smaller than 500 ÎŒA.…”
Section: Resultsmentioning
confidence: 99%