Potential-Induced Conformational Changes in an alfa-CN-terthiophene Thiolate Film on GaAs(110)

VALENTINA LAZARESCU, RARES SCURTU, MIHAIL F. LAZARESCU, ANA M. TOADER, ELENA VOLANSCHI, ELIZABETH SANTOS, HAROLD JONES, GÜNTHER GÖTZ, AND PETER BÄUERLE

LANGMUIR

Año: 2009 vol. 25 p. 6522 - 6531

0743-7463

Second harmonic generation (SHG) investigations on R-CN-terthiophene-thiolate-covered GaAs(110) electrodes in 1 N H2SO4 solution revealed significant changes in the rotational anisotropy of the SH response. The enhancement of the 1- and the 3-fold contributions around -250 mV suggests changes in the symmetry properties of the delocalized electron system due to an alteration of the adsorption geometry induced by the applied potentials. The analysis of the EIS data showed that in the potential region where the SH signal exhibits the more important changes the Mott-Schottky plot undergoes a pronounced shift to more negative potentials as a result of the charging of the surface states grouped about 1.06 eV below the conduction band edge. Semiempirical MO calculations suggest that the most energetically favorable interaction implies electron transfer from the semiconductor conduction band to the lowest unoccupied molecular orbital of the organic molecule with εLUMO = -1.707 eV. Such a chemisorption bond bringing the organicmolecule to a quasi-planar position iswell supported by the major changes in theXPS spectra of the electrochemically biased samples with respect to the as-prepared ones. Two distinct N 1s species instead of one and a shift of 1.6 eV to higher BE of the terthiophene S 2s core level are strong evidence for a potential-induced change in the adsorption geometry. Taking into account that the acceptor-like surface state group located close to the semiconductor valence edge (EC,S = -1.06 eV)  may correspond to the LUMO level (shifted downward by the adsorption process), we assume that the organic molecule, initially adsorbed by the thiolate end, undergoes a conformational change from a tilted to an almost flat position when the applied potential brings the semiconductor Fermi level into its neighborhood. This assumption is in a very good agreement with the potential-induced variation in the thiol thickness estimated from the thiol capacitance.