6 research outputs found

    Experimental and Theoretical Analysis of Nanotransport in Oligophenylene Dithiol Junctions as a Function of Molecular Length and Contact Work Function

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    We report the results of an extensive investigation of metal–molecule–metal tunnel junctions based on oligophenylene dithiols (OPDs) bound to several types of electrodes (M<sub>1</sub>–S–(C<sub>6</sub>H<sub>4</sub>)<i><sub>n</sub></i>–S–M<sub>2</sub>, with 1 ≤ <i>n</i> ≤ 4 and M<sub>1,2</sub> = Ag, Au, Pt) to examine the impact of molecular length (<i>n</i>) and metal work function (Φ) on junction properties. Our investigation includes (1) measurements by scanning Kelvin probe microscopy of electrode work function changes (ΔΦ = Φ<sub>SAM</sub> – Φ) caused by chemisorption of OPD self-assembled monolayers (SAMs), (2) measurements of junction current–voltage (<i>I</i>–<i>V</i>) characteristics by conducting probe atomic force microscopy in the linear and nonlinear bias ranges, and (3) direct quantitative analysis of the full <i>I</i>–<i>V</i> curves. Further, we employ transition voltage spectroscopy (TVS) to estimate the energetic alignment ε<sub>h</sub> = <i>E</i><sub>F</sub> – <i>E</i><sub>HOMO</sub> of the dominant molecular orbital (HOMO) relative to the Fermi energy <i>E</i><sub>F</sub> of the junction. Where photoelectron spectroscopy data are available, the ε<sub>h</sub> values agree very well with those determined by TVS. Using a single-level model, which we justify <i>via ab initio</i> quantum chemical calculations at post-density functional theory level and additional UV–visible absorption measurements, we are able to quantitatively reproduce the <i>I</i>–<i>V</i> measurements in the whole bias range investigated (∼1.0–1.5 V) and to understand the behavior of ε<sub>h</sub> and Γ (contact coupling strength) extracted from experiment. We find that Fermi level pinning induced by the strong dipole of the metal–S bond causes a significant shift of the HOMO energy of an adsorbed molecule, resulting in ε<sub>h</sub> exhibiting a weak dependence with the work function Φ. Both of these parameters play a key role in determining the tunneling attenuation factor (β) and junction resistance (<i>R</i>). Correlation among Φ, ΔΦ, <i>R</i>, transition voltage (<i>V</i><sub>t</sub>), and ε<sub>h</sub> and accurate simulation provide a remarkably complete picture of tunneling transport in these prototypical molecular junctions

    Effect of Heteroatom Substitution on Transport in Alkanedithiol-Based Molecular Tunnel Junctions: Evidence for Universal Behavior

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    The transport properties of molecular junctions based on alkanedithiols with three different methylene chain lengths were compared with junctions based on similar chains wherein every third −CH<sub>2</sub>– was replaced with O or S, that is, following the general formula HS­(CH<sub>2</sub>CH<sub>2</sub>X)<sub><i>n</i></sub>CH<sub>2</sub>CH<sub>2</sub>SH, where X = CH<sub>2</sub>, O, or S and <i>n</i> = 1, 2, or 3. Conducting probe atomic force microscopy revealed that the low bias resistance of the chains increased upon substitution in the order CH<sub>2</sub> < O < S. This change in resistance is ascribed to the observed identical trend in contact resistance, <i>R</i><sub>c</sub>, whereas the exponential prefactor β (length sensitivity) was essentially the same for all chains. Using an established, analytical single-level model, we computed the effective energy offset ε<sub>h</sub> (<i>i.e.</i>, Fermi level relative to the effective HOMO level) and the electronic coupling strength Γ from the current–voltage (<i>I–V</i>) data. The ε<sub>h</sub> values were only weakly affected by heteroatom substitution, whereas the interface coupling strength Γ varied by over an order of magnitude. Consequently, we ascribe the strong variation in <i>R</i><sub>c</sub> to the systematic change in Γ. Quantum chemical calculations reveal that the HOMO density shifts from the terminal SH groups for the alkanedithiols to the heteroatoms in the substituted chains, which provides a plausible explanation for the marked decrease in Γ for the dithiols with electron-rich heteroatoms. The results indicate that the electronic coupling and thus the resistance of alkanedithiols can be tuned by substitution of even a single atom in the middle of the molecule. Importantly, when appropriately normalized, the experimental <i>I–V</i> curves were accurately simulated over the full bias range (±1.5 V) using the single-level model with no adjustable parameters. The data could be collapsed to a single universal curve predicted by the model, providing clear evidence that the essential physics is captured by this analytical approach and supporting its utility for molecular electronics

    Exceptionally Small Statistical Variations in the Transport Properties of Metal–Molecule–Metal Junctions Composed of 80 Oligo­phenylene Dithiol Molecules

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    Strong stochastic fluctuations witnessed as very broad resistance (<i>R</i>) histograms with widths comparable to or even larger than the most probable values characterize many measurements in the field of molecular electronics, particularly those measurements based on single molecule junctions at room temperature. Here we show that molecular junctions containing 80 oligophenylene dithiol molecules (OPDn, 1 ≤ <i>n</i> ≤ 4) connected in parallel display small relative statistical deviationsδ<i>R</i>/<i>R</i> ≈ 25% after only ∼200 independent measurementsand we analyze the sources of these deviations quantitatively. The junctions are made by conducting probe atomic force microscopy (CP-AFM) in which an Au-coated tip contacts a self-assembled monolayer (SAM) of OPDs on Au. Using contact mechanics and direct measurements of the molecular surface coverage, the tip radius, tip-SAM adhesion force (<i>F</i>), and sample elastic modulus (<i>E</i>), we find that the tip-SAM contact area is approximately 25 nm<sup>2</sup>, corresponding to about 80 molecules in the junction. Supplementing this information with <i>I–V</i> data and an analytic transport model, we are able to quantitatively describe the sources of deviations <i>δR</i> in <i>R</i>: namely, <i>δN</i> (deviations in the number of molecules in the junction), <i>δε</i> (deviations in energetic position of the dominant molecular orbital), and <i>δΓ</i> (deviations in molecule-electrode coupling). Our main results are (1) direct determination of <i>N</i>; (2) demonstration that <i>δN</i>/<i>N</i> for CP-AFM junctions is remarkably small (≤2%) and that the largest contributions to <i>δR</i> are <i>δε</i> and <i>δΓ</i>; (3) demonstration that δ<i>R</i>/<i>R</i> after only ∼200 measurements is substantially smaller than most reports based on >1000 measurements for single molecule break junctions. Overall, these results highlight the excellent reproducibility of junctions composed of tens of parallel molecules, which may be important for continued efforts to build robust molecular devices

    Table S4 from Snake fungal disease: an emerging threat to wild snakes

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    Additional samples analyzed by fungal culture to assess the known host range and geographic distribution of Ophidiomyces. Location data is displayed only to the county level due to concerns with disclosing specific locations of rare or sensitive snake populations. The type of growth medium upon which the fungus culture was performed is listed in the last column (DTM = dermatophyte test medium; IMA = inhibitory mold agar; PFA = potato flake agar; SD = Sabouraud's dextrose agar

    Table S2 from Snake fungal disease: an emerging threat to wild snakes

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    Fungal operational taxonomic units (OTUs) recovered from the skin of snakes. Each unique internal transcribed spacer (ITS) region DNA sequence variant (i.e., 100% identity) was assigned a numerical code and a presumptive taxon identification. The NWHC case number (see table S1) of the host(s) from which each variant was recovered is specified. A representative DNA sequence for each variant has been deposited in GenBank; bolded case numbers depict the snakes from which these deposited fungal DNA sequences originated. The assignment of each ITS variant to an OTU based on cut-offs of 99.5%, 99%, 98%, and 97% sequence identities is shown, with each OTU given an alpha-numeric cod

    Table S1 from Snake fungal disease: an emerging threat to wild snakes

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    Samples used to determine the types of fungi associated with dermatitis in wild snakes. Location data are displayed only to the county (or sometimes state) level due to concerns with disclosing specific locations of rare or sensitive snake populations. Fungal infection was assessed by examining histologic sections of skin lesions. The number of gross lesions consistent with dermatitis were categorized as "none" (no gross skin lesions observed), "single" (one lesion), "multiple" (more than one discrete lesion), or "not assessed" (no information was available on the number of skin lesions present). The type of fungal growth medium upon which samples were cultured is listed as "DTM" (dermatophyte test medium) or "SD" (Sabouraud dextrose medium containing chloramphenicol and gentamycin). The number of unique internal transcribed spacer region DNA sequences identified per snake (or operational taxonomic units [OTUs] at 100% sequence identity) is listed. Samples originating from snakes cited in previous literature are specifie
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