Langmuir, Vol.26, No.3, 1688-1699, 2010
Elastic, Adhesive, and Charge Transport Properties of a Metal-Molecule-Metal Junction: The Role of Molecular Orientation, Order, and Coverage
The elastic, adhesive, and charge transport properties of a metal-molecule-metal junction were studied via conducting-probe atomic force microscopy (AFM) and correlated with molecular structure by near-edge X-ray absorption fine structure (NEXAFS) spectroscopy. The junctions consisted of Co-Cr-coated AFM tips in contact with methyl-terminated alkanethiols (CH3(CH2)(n-1)SH, denoted by C-n, where n is the number of carbons in the molecular chain) on Au substrates. AFM contact data were analyzed with the Derjaguin-Muller-Toporov contact model, modified by a first-order elastic perturbation method to account for substrate effects, and a parabolic tunneling model, appropriate for a metal-insulator-metal junction in which the thickness of the insulator is comparable to the Fermi wavelength of the conducting electrons. NEXAFS carbon K-edge spectra were used to compute the dichroic ratio R-1 for each Film, which provided a quantitative measure of the molecular structure as a function of n. As it decreased from IS to 5, there was a change in the molecular phase from crystalline to amorphous (R-t -> 0)and loss of surface coverage, and as a result, the work of adhesion w increased from 82.8 mJ m(-2) to 168.3 mJ m(-2), the Young's modulus of the film E-film decreased from 1.0 to 0.15 GPa. and the tunneling barrier height phi(0) - E-F decreased from 2.4 to 2.1 eV. For all n, the harrier thickness t decreased for small applied loads F and remained constant at similar to 2.2 run for large F The change in behavior was explained by the presence of two insulating layers: an oxide layer on the Co-Cr tip, and the alkanethiol monolayer on the Au surface. X-ray photoelectron spectroscopy confirmed the presence of an oxide layer on the Co-Cr tip, and by performing high-resolution region scans through the film, the thickness of the oxide layer t(oxide) was found to be between 1.9 and 3.9 nm. Finally, it was shown that phi(0) - E-F is strain-dependent, and the strain at which the film is completely displaced from under the tip is -0.17 for all values of n.