Molecular Electronics WHY ORGANIC MOLECULES? • Small (nanosize) • Tailor-made properties by synthesis of new molecules • large number of exact copies: control over properties (e.g. exactly the same energy levels) • low-cost • complex structures built up by self-assembly • and more… Nanoscience II spring 2009 1 Nanoscience II spring 2009 2 Classification, examples • Bulk molecular electronics: organic compounds, e.g. Polymer films, liquid crystal displays, organic lightemitting diode (OLED) displays, plastic transistors • Single molecular systems: Hybrid molecular electronics (HME): devices made of single molecules attached to inorganic electrodes (hot research topic) Mono-molecular electronic devices (MME): complex device structures built up by individual molecules (vision) Nanoscience II spring 2009 3 Covalent Carbon bonds p-orbitals • 4 valence electrons, ground state 1s22s22p2 • hybridization: promotion to 2s2p3 , formation of linear combinations of the sorbital and the px- , py- , pz-orbitals, to form -bonds -bonds: • Very flexible bonding, basis of all organic molecules Hybridization and ability to bond”sideways” • sp3: one s-, three p-orbitals. Tetrahedral makes carbon bonds very flexible, allows formation of complex structures geometry (3-dim), example: diamond Conjugated molecules: delocalized 2 • sp : one s-, two p-orbitals. Planar, orbitals hexagonal structure, example: graphite. One p-orbital makes -bond • sp: one s- and one p-orbital: linear bond. Two p-orbitals make two -bonds Nanoscience II spring 2009 4 Other bonds • Van der Waals bonding: weak bonds, important for selfassembly • Hydrogen bonds: ex. C - H - C , O - H - C Contacts to electrodes: • The molecule-electrode bonds determine charge transport properties • covalent bonds, strong wave function overlap => low resistance. Example: S - Au, (thiol) used for many selfassembled monolayers • weak van der Waals-bond => tunneling transport, high resistance Nanoscience II spring 2009 5 Single-molecule: HME and MME Building block issues: conduction, mechanical rigidity Polyene Alkanes Polythiophene Adamantyl Polyphenylenevinylene Biphenyl Polyphenyleneethynylene Thiophenylsubstituted benzene Nanoscience II spring 2009 Trans-acetyleneplatinum (II) Thiophenylsubstituted benzene 6 Diodes Aviram and Ratner 1974: Experimentally realised diodes, in ordered molecular films Suggested a theoretical molecular diode Nanoscience II spring 2009 7 Switches and storage elements Switches can be classified by: - the stimulus that triggers the switch - the property or function that is switched Light-triggered switch (M. Irie) Nanoscience II spring 2009 8 Catenate: supramolecular device consisting of two interlocked rings Nanoscience II spring 2009 9 Three-terminal devices Molecules with 3 terminals? Unlikely Instead two terminals and isolated gate Model of potential from buried gate Different approach: third terminal by ”squeezing” the C60 with the tip Nanoscience II spring 2009 10 Example from Chalmers: Kubatkin et al. Nature, 2003 Nanoscience II spring 2009 11 STM studies of single molecules Stabilizing a single molecular wire by embedding in alkanethiol SAM Nanoscience II spring 2009 12 Monomolecular devices: STM lithography (Reed and Tour) Nanoscience II spring 2009 13 Monomolecular nanopore device: example Nanoscience II spring 2009 14 Monomolecular films with crossbar arrays: Connecting storage elements, logic structures Optical microscope SEM image of a crossbar array SEM AFM Nanoscience II spring 2009 15 Break junctions Mechanically controlled breakage of thin conductor, gap controlled by piezoelectric rod Advantages: same contact at both ends Figure 10.5. (a) I-V characteristics for Benzene-1,4-dithiol between gold electrodes. (b) Schematic of the molecule in contact with gold electrodes, represented here as three gold atoms. Nanoscience II spring 2009 16 Example of break junction experiments: Nanoscience II spring 2009 17 Current transport • • • • • Delocalized -system => Intramolecular ballistic transport Strongly varying electronic levels depends upon molecular structure, bias Quantized conductance G = 2e2/h for each current mode, for ideal contacts (rarely observed) Discrete HOMO and LUMO levels => resonant tunneling => negative dfferential resistance (NDR) Poor overlap of -orbitals with electrode wave functions lead to high tunneling barrier, high resistance Nanoscience II spring 2009 18
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