Field-induced conformational changes in bimetallic oligoaniline junctions Juan C. Sotelo, 1 Liuming Yan, Michael Wang, 1 and Jorge M. Seminario 1,2 1 Department of Chemical Engineering, Texas A&M University, College Station, Texas 77843, USA 2 Department of Electrical and Computer Engineering, Texas A&M University, College Station, Texas 77843, USA Received 26 August 2006; revised manuscript received 23 October 2006; published 21 February 2007 We report three types of nonplanar conformations, , , and , for a neutral isolated oligoaniline molecule as well as for an oligoaniline with Au and Pd atoms attached at its ends. Each type of conformation has several conformers of nearly equal energies. An applied external voltage can be used to switch between conformations, producing in the process a sharp decrease of their energies. These bias voltage-induced conformational changes are a potential switching mechanism for two terminal molecular devices at the nanoscale domain. They cause the conductivity of the molecule to alternate between high and low states, compensating for the behavior of typical three-terminal devices, needed for the development of a gate-less electronics. DOI: 10.1103/PhysRevA.75.022511 PACS numbers: 31.15.Ew, 33.15.Bh, 31.70.Ks, 31.15.Ar I. INTRODUCTION Molecular switches are essential components in molecular electronics devices as they constitute the building blocks in logic architectures. Lately, much effort has been devoted to the identification of these switches, and to the understanding of the intrinsic mechanisms governing their switching prop- erties. Many types of switching mechanisms have been iden- tified, among them, photon-induced 1, change of redox state 24, and electrically induced switching 58to name a few. A typical electrically driven molecular switch consists of a single molecule, or many of them, e.g., self-assembled monolayer SAM, adsorbed on metal electrodes, which can be electrically toggled between a high conductance ON state and a low conductance OFFstate, with the ON and OFF states being stable enough for a large number of switch- ing cycles. Recently, it has been shown experimentally that for a wide range of temperatures oligoaniline molecular junctions can exhibit electrical bistability and switch be- tween a high and low conducting states in response to an applied external bias voltage 7. It was suggested this be- havior might be due to a redistribution of charges in the molecule coupled with a shift in molecular conformations 7. In this paper we show that there are three main types of conformations for the standalone and for the extended with electrode atoms of Au or Pdoligoaniline molecule, called , , and , which undergo conformational changes under the influence of an external longitudinal electric field. In an Au- oligoaniline-Pd junction, when equilibrium is reached at room temperature, has the highest probability to be present in the junction, has the smallest. Furthermore, when the junction is subjected to an external bias voltage there is an interconversion between the and conformations leading to a switching behavior between high and low current states in the junction, as observed in experiments 7. We deal with the conformational changes by considering first an extended oligoaniline molecule as a protojunction where a sought after property of a molecular switch, such as conformational changes, can be probed more easily 9,10. Although by considering just the extended molecule, the in- teraction with the leads of both the extending metal atoms and the molecule is missing, and the dielectric effect of the leads on the field is not considered, nevertheless, it can still help elucidate the field-induced changes in molecular confor- mation and electronic structure for the following reasons. First, on a first approximation the interaction metal-molecule may be considered local, with metal atoms in direct contact with the molecule or in the near neighborhood contributing the most. This is, in fact, just a restatement of the rationale behind treating a molecular junction as a metal-extended- molecule-metal system 1114. Second, the molecular and electronic structures of the extended molecule are those ob- tained directly from ab initio calculations, which should al- low for a detailed analysis at the atomic level of structural e.g., bond length, torsional anglesand electronic properties e.g., polarization, charge distributionchanges taken place within a molecule exposed to an external field. Such a fine level of resolution is lost when bulk electrodes are brought into consideration because of the coarse approximations that have to be made to treat them in present electron transport models. Ultimately, to take full advantage of molecular de- vices one would like to interconnect them, at most, through small metal clusters rather than through bulk metal solids 8. Once the key properties of the extended molecule have been established, they can be included within an appropriate framework, such as the Green function method introduced below, to study the current through the junction. This paper is organized as follows. Section II introduces the computational methods for dealing with the electronic properties of finite clusters and bulk electrodes, and the current-voltage I-Vcharacterization of the junctions. Sec- tion III presents the DOS and transmission spectra for all conformations, as well as their I-V characteristics at fixed geometries. The section ends with a discussion of conforma- tional changes under applied electric fields. Finally, Sec. IV summarizes the results of this work. II. METHODOLOGY AND PROCEDURE Density functional theory DFTand Green’s function GFtheory are used to study the electrical properties of conformations of the standalone oligoaniline and oligoa- niline junctions. Basically, three different types of calcula- PHYSICAL REVIEW A 75, 022511 2007 1050-2947/2007/752/02251113©2007 The American Physical Society 022511-1