The Electrical Resistance of AgTS-S(CH2)n-1CH3//Ga2O3/EGaIn Tunneling Junctions

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Cademartiri, Ludovico
Thuo, Martin M.
Nijhuis, Christian A.
Reus, William F.
Tricard, Simon
Sodhi, Rana N. S.
Brodersen, Peter
Kim, Choongik
Chiechi, Ryan C.
Note: Order does not necessarily reflect citation order of authors.
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https://doi.org/10.1021/jp212501sMetadata
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Cademartiri, Ludovico, Martin M. Thuo, Christian A. Nijhuis, William F. Reus, Simon Tricard, Jabulani R. Barber, Rana N. S. Sodhi, et al. 2012. The Electrical Resistance of AgTS-S(CH2)n-1CH3//Ga2O3/EGaIn Tunneling Junctions. Journal of Physical Chemistry C 116, no. 20: 10848–10860. doi:10.1021/jp212501sAbstract
Tunneling junctions having the structure AgTS–S(CH2)n−1CH3//Ga2O3/EGaIn allow physical–organic studies of charge transport across self-assembled monolayers (SAMs). In ambient conditions, the surface of the liquid metal electrode (EGaIn, 75.5 wt % Ga, 24.5 wt % In, mp 15.7 °C) oxidizes and adsorbs―like other high-energy surfaces―adventitious contaminants. The interface between the EGaIn and the SAM thus includes a film of metal oxide, and probably also organic material adsorbed on this film; this interface will influence the properties and operation of the junctions. A combination of structural, chemical, and electrical characterizations leads to four conclusions about AgTS–S(CH2)n−1CH3//Ga2O3/EGaIn junctions. (i) The oxide is ∼0.7 nm thick on average, is composed mostly of Ga2O3, and appears to be self-limiting in its growth. (ii) The structure and composition (but not necessarily the contact area) of the junctions are conserved from junction to junction. (iii) The transport of charge through the junctions is dominated by the alkanethiolate SAM and not by the oxide or by the contaminants. (iv) The interface between the oxide and the eutectic alloy is rough at the micrometer scale.Terms of Use
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