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In these experiments, a micrometrically driven hanging mercury drop electrode was used. This device allows us to control the Hg drop size by increasing or decreasing the volume of the suspended drop with ca. 1% precision.
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2) Figure 2.
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0347960898
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Equation 8 does not include the image charge effects since they are negligible for the purpose of the argument presented in the subsequent section in the text.
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4+ radius.
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0346700241
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note
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Since the monolayer films used by Miller and co-workers (ref 40) were hydroxy terminated, the difference between our hexadecanethiolate monolayer and their α,ω-hydroxytetradecanethiol monolayers is only one σ-bond. Thus, the correction we applied gives high estimates of the expected values. However, our previous measurements (ref 24) showed that the rates of electron tunneling across the hydroxy-terminated monolayer are actually somewhat higher than those measured at methyl terminated monolayers of the same number of carbon atoms. We also note that since Miller's data were obtained on gold electrode where the alkyl chains are tilted by ca. 30°, they are intrinsically higher than ours obtained on Hg (0° tilt angle), everything else being the same, due to a contribution to the total rate from a tunneling pathway involving chain-to-chain coupling. Thus, overall, the correction we used is reasonably accurate.
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We demonstrated previously that the increase of an electron tunneling rate in case A is due to additional contribution to the tunneling from a pathway involving chain-to-chain coupling (see ref 24).
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