Conduction mechanisms in biphenyl dithiol single-molecule junctions

M. Bürkle, J. K. Viljas, D. Vonlanthen, A. Mishchenko, G. Schön, M. Mayor, T. Wandlowski, and F. Pauly
Phys. Rev. B 85, 075417 – Published 21 February 2012

Abstract

Based on density-functional theory calculations, we report a detailed study of the single-molecule charge-transport properties for a series of recently synthesized biphenyl-dithiol molecules [D. Vonlanthen et al., Angew. Chem., Int. Ed. 48, 8886 (2009); A. Mishchenko et al., Nano Lett. 10, 156 (2010)]. The torsion angle ϕ between the two phenyl rings, and hence the degree of π conjugation, is controlled by alkyl chains and methyl side groups. We consider three different coordination geometries, namely, top-top, bridge-bridge, and hollow-hollow, with the terminal sulfur atoms bound to one, two, and three gold surface atoms, respectively. Our calculations show that different coordination geometries give rise to conductances that vary by one order of magnitude for the same molecule. Irrespective of the coordination geometries, the charge transport calculations predict a cos2ϕ dependence of the conductance, which is confirmed by our experimental measurements. We demonstrate that the calculated transmission through biphenyl dithiols is typically dominated by a single transmission eigenchannel formed from π electrons. For perpendicular orientation of the rings a residual conductance arises from σ-π couplings. But only for a single molecule with a completely broken conjugation we find a nearly perfect degeneracy of the σ-π eigenchannels for the hollow-hollow-type contact in our theory.

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  • Received 1 September 2011

DOI:https://doi.org/10.1103/PhysRevB.85.075417

©2012 American Physical Society

Authors & Affiliations

M. Bürkle1,2, J. K. Viljas3,4, D. Vonlanthen5, A. Mishchenko6, G. Schön1,2,7, M. Mayor2,5,7,*, T. Wandlowski6,†, and F. Pauly1,2,8,‡

  • 1Institute of Theoretical Solid State Physics, Karlsruhe Institute of Technology, D-76131 Karlsruhe, Germany
  • 2Center for Functional Nanostructures, Karlsruhe Institute of Technology, D-76131 Karlsruhe, Germany
  • 3Low Temperature Laboratory, Aalto University, P.O. Box 15100, FIN-00076 AALTO, Finland
  • 4Department of Physics, P.O. Box 3000, FIN-90014 University of Oulu, Finland
  • 5Department of Chemistry, University of Basel, CH-4003 Basel, Switzerland
  • 6Department of Chemistry and Biochemistry, University of Bern, CH-3012 Bern, Switzerland
  • 7Institute of Nanotechnology, Karlsruhe Institute of Technology, D-76344 Eggenstein-Leopoldshafen, Germany
  • 8Molecular Foundry, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA

  • *marcel.mayor@unibas.ch
  • thomas.wandlowski@dcb.unibe.ch
  • fabian.pauly@kit.edu

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Issue

Vol. 85, Iss. 7 — 15 February 2012

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