2000
DOI: 10.1038/scientificamerican0600-86
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Computing with Molecules

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Cited by 262 publications
(170 citation statements)
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“…41,42 Despite the well-known issue that B3LYP may be inadequate to account for the dispersion interaction which is a significant contribution to the interaction between CBPQT and TTF/ DNP, 16,19 it should still be adequate in describing the difference between the interactions at different oxidation states, since the variation of the dispersion interaction for different oxidation states should be minor compared to the variation of the electrostatic interaction. At the final geometry, the solvation energy in AN (dielectric constant 35.69, density 0.7857 g/cm 3 at 20°C, 43 probe radius 2.18 Å) is also calculated in B3LYP/ 6-31G** (since the solvation energy is not very sensitive to the choice of basis set 42 ) using the Poisson-Boltzmann continuum-solvation model. 44,45 The following atomic radii are used (in Å): 42 H 1.15, C 1.9, N 1.6, O 1.6, F 1.682, P 2.074, and S 1.7 (which has been changed from 1.9 to reproduce the experimental reduction potentials of TTF).…”
Section: Methodsmentioning
confidence: 99%
“…41,42 Despite the well-known issue that B3LYP may be inadequate to account for the dispersion interaction which is a significant contribution to the interaction between CBPQT and TTF/ DNP, 16,19 it should still be adequate in describing the difference between the interactions at different oxidation states, since the variation of the dispersion interaction for different oxidation states should be minor compared to the variation of the electrostatic interaction. At the final geometry, the solvation energy in AN (dielectric constant 35.69, density 0.7857 g/cm 3 at 20°C, 43 probe radius 2.18 Å) is also calculated in B3LYP/ 6-31G** (since the solvation energy is not very sensitive to the choice of basis set 42 ) using the Poisson-Boltzmann continuum-solvation model. 44,45 The following atomic radii are used (in Å): 42 H 1.15, C 1.9, N 1.6, O 1.6, F 1.682, P 2.074, and S 1.7 (which has been changed from 1.9 to reproduce the experimental reduction potentials of TTF).…”
Section: Methodsmentioning
confidence: 99%
“…In addition, oligomeric materials with defined length and constitution have become important subjects of their own [8]. One of the emerging and most challenging areas for monodisperse conjugated oligomers is molecular scale electronics, in which single or small packets of molecules function as the active channels for information transportation, processing, and storage [9,10]. Constructing electronic devices with organic molecules can overcome the fundamental physical restraints in traditional Si-based technologies and can also result in a rapid and low-cost bottom-up manufacturing process for electronic device fabrication.…”
mentioning
confidence: 99%
“…The theoretical analysis suggests that the bias dependence of the polarizability of the molecule feeds back into the current leading to an asymmetric shape of the current-voltage characteristics, similar to the phenomena in a semiconductor diode. molecular electronics ͉ rectification ͉ single-molecule studies T he idea to build an electronic device based on single molecules is today called Molecular Electronics (1)(2)(3)(4). Conceptually and historically, this field starts out from electron transfer physics (5) and chemistry (6,7), where a single electron is transferred within a molecule.…”
mentioning
confidence: 99%