677 research outputs found

    A versatile experimental approach for understanding electron transport through organic materials

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    This paper describes an experimentally simple method for assembling junctions with nanometer-scale, structured organic films positioned between two metal electrodes. These junctions comprise two metal electrodes that sandwich two self-assembled monolayers (SAMs) - that is, metal (mercury)-SAM//SAM-metal (mercury, gold or silver) junctions. The junctions are easy to assemble (because the mercury electrode is compliant) and they are compatible with SAMs incorporating organic groups having a range of structures. This paper describes three different variations on this type of Hg-based junction. The first junction, formed by two contacting mercury drops covered by the same type of SAM, is a prototype system that provided useful information on the structure and electrical properties of the Hg-based junctions. The second junction consists of a Hg drop covered by one SAM (Hg-SAM(1)) in contact with a second SAM supported on a silver film (Ag-SAM(2)) - that is, a Hg-SAM(1)//SAM(2)-Ag junction. This junction allowed systematic measurements of the current that flowed across SAM(2), as a function of structure (for example, using aliphatic or aromatic thiols of different length), and a common SAM(1) of hexadecane thiol. The current density follows the relation I = I0e-βdAg,Hg, where dAg,Hg is the distance between the electrodes, and β is the structure-dependent attenuation factor for the molecules making up SAM(2): β was 0.87 ± 0.1 Å-1 for alkanethiols, 0.61 ± 0.1 Å-1 for oligophenylene thiols, and 0.67 ± 0.1 Å-1 for benzylic derivatives of oligophenylene thiols, in general agreement with the values calculated by other approaches. The same type of junction, but using SAM(1) and SAM(2) carrying suitable chemical groups, X and Y, was used to measure the rate of electron transfer across different types of functional groups and bonds: van der Waal interactions, H bonds, and covalent bonds. The third type of junction, Hg-SAM//R//SAM-Hg, is an electrochemical junction that can (i) trap redox-active molecules (R) in the interfacial region between the SAMs, and (ii) control the potential of the electrodes with respect to the redox potential of R using an external reference electrode. This system shows I-V curves with steps that can be interpreted in terms of redox cycling mechanism. © 2002 Elsevier Science B.V. All rights reserved

    Electron Transfer in a Hg‐SAM//SAM‐Hg Junction Mediated by Redox Centers

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    Current affairs: The electron-transport properties of a metal-molecule-metal junction based on two contacting redoxactive self-assembled monolayers of [Ru(NH3)5(NC5H 4-4-CH2NHCO(CH2)10-SH](PF 6)2 (see picture) is described. The junction becomes conductive when the electrode potentials are adjusted to the formal potential of the redox centers and shows diode- and transistor-like characteristics analogous to those of solid-state devices

    Whitesides' Group: Writing a Paper

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    Electron exchange between two electrodes mediated by two electroactive adsorbates

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    Electrochemical junctions are used to incorporate and study teh electtron transport mediated by redox centres. Theoretical model interpret the data of the molecular transistor behavior

    The study of charge transport through organic thin films: mechanism, tools and applications

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    In this paper, we discuss the current state of organic and molecular-scale electronics, some experimental methods used to characterize charge transport through molecular junctions and some theoretical models (superexchange and barrier tunnelling models) used to explain experimental results. Junctions incorporating self-assembled monolayers of organic molecules - and, in particular, junctions with mercury-drop electrodes - are described in detail, as are the issues of irreproducibility associated with such junctions (due, in part, to defects at the metal-molecule interface). © 2007 The Royal Society

    Mesoscale Self-Assembly:  Capillary Interactions When Positive and Negative Menisci Have Similar Amplitudes

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    This paper describes the two-dimensional self-assembly of hexagonal plates at the interface between perfluorodecalin and water. The plates were prepared with five different permutations of hydrophobic and hydrophilic faces. The shapes and amplitudes of the menisci that form on the faces of the plates determine the magnitude of the lateral capillary forces through which they interact. The amplitudes of the menisci also influencethrough their out-of-plane componentsthe position and orientation of the plate relative to the plane of the liquid−liquid interface. In these experiments, the plates were made of poly(dimethylsiloxane) (PDMS) (ρ = 1.05 g/cm3) containing aluminum oxide (ρ = 4.00 g/cm3); this dopant adjusted the density of the plates, the extent to which they sank into the liquid−liquid interface, and thus the structure of their menisci. The plates studied had densities of 1.05 to 1.86 g/cm3. This work complements previous papers (Bowden, N.; Choi I. S.; Grzybowski, B. A.; Whitesides, G. M. J. Am. Chem. Soc. 1999, 121, 5373. Bowden, N.; Oliver, S. R. J.; Whitesides, G. M. J. Phys. Chem. B 2000, 104, 2714.) that examined the assembly of hexagonal plates with densities at the extremes of the range studied. By following the structures of the aggregates formed at intermediate densities, it is possible to observe the way in which the self-assembling system transitions from an aggregate of one structure to that of another. The results from these studies are relevant to the design of micrometer-sized plates capable of self-assembly

    Electron transport through thin organic films in metal-insulator-metal junctions based on self-assembled monolayers

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    This paper describes an experimentally simple system for measuring rates of electron transport across organic thin films having a range of molecular structures. The system uses a metal-insulator-metal junction based on self-assembled monolayers (SAMs); it is particularly easy to assemble. The junction consists of a SAM supported on a silver film (Ag-SAM(1)) in contact with a second SAM supported on the surface of a drop of mercury (Hg-SAM(2))-that is, a Ag-SAM(1)SAM(2)-Hg junction. SAM(1) and SAM(2) can be derived from the same or different thiols. The current that flowed across junctions with SAMs of aliphatic thiols or aromatic thiols on Ag and a SAM of hexadecane thiol on Hg depended both on the molecular structure and on the thickness of the SAM on Ag: the current density at a bias of 0.5 V ranged from 2 × 10-10 A/cm2 for HS(CH2)15CH3 on Ag to 1 × 10-6 A/cm2 for HS(CH2)15H3 on Ag, and from 3 x 10-6 A/cm2 for HS(Ph)3H (Ph = 1,4-C6H4) on Ag to 7 × 10-4 A/cm2 for HSPhH on Ag. The curr..
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