Title. I-V curve? e-e interactions? Conductance? Electrical Transport Through Single Molecules. Vibrations? Devices?

Similar documents
Computational Modeling of Molecular Electronics. Chao-Cheng Kaun

Molecular electronics. Lecture 2

Speed-up of ATK compared to

Canadian Journal of Chemistry. Spin-dependent electron transport through a Mnphthalocyanine. Draft

Electronic communication through molecular bridges Supporting Information

Density Functional Theory (DFT) modelling of C60 and

Session Chair: Prof. Haiping Cheng (University of Florida) Dr. Lei Shen. National University of Singapore

Herre van der Zant. interplay between molecular spin and electron transport (molecular spintronics) Gate

arxiv:cond-mat/ v2 [cond-mat.mtrl-sci] 21 Feb 2007

Time-Dependent Electron Localization Function! (TD-ELF)! GOAL! Time-resolved visualization of the breaking and formation of chemical bonds.!

Supporting Information: Local Electronic Structure of a Single-Layer. Porphyrin-Containing Covalent Organic Framework

Introduction to Density Functional Theory with Applications to Graphene Branislav K. Nikolić

First-Principles Modeling of Charge Transport in Molecular Junctions

single-electron electron tunneling (SET)

Impact of collective effects on charge transport through molecular monolayers

Pseudopotentials for hybrid density functionals and SCAN

Electronic level alignment at metal-organic contacts with a GW approach

Electrical conductivity of metal carbon nanotube structures: Effect of length and doping

Kinetic equation approach to the problem of rectification in asymmetric molecular structures

Electronic structure mechanism of spin-polarized electron transport in a Ni C 60 Ni system

2. TranSIESTA 1. SIESTA. DFT In a Nutshell. Introduction to SIESTA. Boundary Conditions: Open systems. Greens functions and charge density

Designing interfaces for Spin Injection into Organic Molecular Solids: A Surface Science Approach

Molecular Electronics 11/17/05

Single-Molecule Junctions: Vibrational and Magnetic Degrees of Freedom, and Novel Experimental Techniques

arxiv:cond-mat/ v1 [cond-mat.mes-hall] 19 Dec 2006

An ab initio approach to electrical transport in molecular devices

Momentum filtering effect in molecular wires

arxiv:cond-mat/ v1 [cond-mat.mtrl-sci] 27 Feb 2007

First-principles study of spin-dependent transport through graphene/bnc/graphene structure

PHYSICAL REVIEW B 70, (2004) (Received 23 November 2003; revised manuscript received 16 March 2004; published 24 August 2004)

Interaction between a single-molecule

Heterostructures and sub-bands

Physics of Semiconductors

Key word: DensityFunctional Theory, Endohedral Energy gap, Electonic properties.

Electron spin transport in Magnetic Multilayers and Carbon Materials. Kurt Stokbro CEO, Founder QuantumWise A/S (Copenhagen, Denmark)

METAL/CARBON-NANOTUBE INTERFACE EFFECT ON ELECTRONIC TRANSPORT

Supporting Information. Charge Transport Across Insulating. Self-Assembled Monolayers: Non-Equilibrium. Approaches and Modeling to Relate Current and

New Volleyballenes: Y 20 C 60, La 20 C 60, and Lu 20 C 60

Electron transport through molecular junctions and FHI-aims

Perfect spin-fillter and spin-valve in carbon atomic chains

2D Materials with Strong Spin-orbit Coupling: Topological and Electronic Transport Properties

Modeling Transport in Heusler-based Spin Devices

Outline. Introduction: graphene. Adsorption on graphene: - Chemisorption - Physisorption. Summary

Do molecular rectifiers exist?

Lecture 4: Band theory

Electron transport through Shiba states induced by magnetic adsorbates on a superconductor

Spin and Charge transport in Ferromagnetic Graphene

arxiv: v1 [cond-mat.mes-hall] 2 Mar 2018

A Single-Level Tunnel Model to Account for Electrical Transport through. Single Molecule- and Self-Assembled Monolayer-based Junctions

Apparent reversal of molecular orbitals reveals entanglement

Transport through Andreev Bound States in a Superconductor-Quantum Dot-Graphene System

Supporting information. Realizing Two-Dimensional Magnetic Semiconductors with. Enhanced Curie Temperature by Antiaromatic Ring Based

arxiv: v1 [cond-mat.mes-hall] 3 Apr 2014

DENSITY FUNCTIONAL THEORY FOR NON-THEORISTS JOHN P. PERDEW DEPARTMENTS OF PHYSICS AND CHEMISTRY TEMPLE UNIVERSITY

Strong Correlation Effects in Fullerene Molecules and Solids

Australian Journal of Basic and Applied Sciences

Saroj P. Dash. Chalmers University of Technology. Göteborg, Sweden. Microtechnology and Nanoscience-MC2

Classification of Solids

Temperature dependence of Andreev spectra in a superconducting carbon nanotube quantum dot

Conductance Calculations for Small Molecules

SPINTRONICS. Waltraud Buchenberg. Faculty of Physics Albert-Ludwigs-University Freiburg

Electron tunneling through alkanedithiol molecules

Lecture 12. Electron Transport in Molecular Wires Possible Mechanisms

Theory of doping graphene

Site- and orbital-dependent charge donation and spin manipulation in electron-doped metal phthalocyanines

TRANSVERSE SPIN TRANSPORT IN GRAPHENE

Spin injection. concept and technology

Surface Transfer Doping of Diamond by Organic Molecules

Single- molecule conductance of pyridine- terminated dithienylethene switch molecules

CME 300 Properties of Materials. ANSWERS: Homework 9 November 26, As atoms approach each other in the solid state the quantized energy states:

Effective masses in semiconductors

Electrical Conductance of Molecular Wires

CITY UNIVERSITY OF HONG KONG. Theoretical Study of Electronic and Electrical Properties of Silicon Nanowires

1+2 on GHD (5 µl) Volume 1+2 (µl) 1 on GHD 1+2 on GHD


Many-body correlations in a Cu-phthalocyanine STM single molecule junction

In order to determine the energy level alignment of the interface between cobalt and

Branislav K. Nikolić

DFT EXERCISES. FELIPE CERVANTES SODI January 2006

Intro to ab initio methods

LUMO + 1 LUMO. Tómas Arnar Guðmundsson Report 2 Reikniefnafræði G

J 12 J 23 J 34. Driving forces in the nano-magnetism world. Intra-atomic exchange, electron correlation effects: Inter-atomic exchange: MAGNETIC ORDER

Measuring charge transport through molecules

Many-body transitions in a single molecule visualized by scanning tunnelling microscopy

Electronic properties of aluminium and silicon doped (2, 2) graphyne nanotube

V + XOR AND. Architectures HS for molecular electronic computers: molecular electronic diodes MITRE. James C. Ellenbogen J.

Chapter 6. Electronic spectra and HOMO-LUMO studies on Nickel, copper substituted Phthalocyanine for solar cell applications

Molecules and Condensed Matter

The Gutzwiller Density Functional Theory

Ferromagnetism and Electronic Transport. Ordinary magnetoresistance (OMR)

Formation and characterization of a. molecule-metal-molecule bridge in real space SUPPORTING INFORMATION

Structural, electronic and magnetic properties of vacancies in single-walled carbon nanotubes

Mn in GaAs: from a single impurity to ferromagnetic layers

Ab-initio Molecular Electronics: are we reaching the limit? Yamila.García Applied Physics Department, Alicante University, Spain

Supporting Information for Ultra-narrow metallic armchair graphene nanoribbons

The Electronic Structure of Dye- Sensitized TiO 2 Clusters from Many- Body Perturbation Theory

Molecular electronics and single electron transistors. Molecular electronics: definition

Single Electron Tunneling Examples

Electron Emission from Diamondoids: a DMC Study. Neil D. Drummond Andrew J. Williamson Richard J. Needs and Giulia Galli

Quantum Chemistry. NC State University. Lecture 5. The electronic structure of molecules Absorption spectroscopy Fluorescence spectroscopy

Transcription:

Electrical Transport Through Single Molecules Harold U. Baranger, Duke University Title with Rui Liu, San-Huang Ke, and Weitao Yang Thanks to S. Getty, M. Fuhrer and L. Sita, U. Maryland Conductance? I-V curve? e-e interactions? Vibrations? Devices? role of contact atomic structure agreement between experiment and theory metal atoms are good for conduction!

How to contact a molecule?? How to contact?? self-assembled alkanethiol monolayers-prb 48, 1711 (1993) mechanically controllable break junction Science 278,252 (1997) electromigration junction APL 75, 301 (1999)

Examples: Experiments on Conjugated Molecules Expt. Examples Reed & Tour groups, Science 278, 252 (97) Reichert, et al. (Karlsruhe) APL 82, 4137 (03) Rawlett, et al. APL 81, 3043 (02) Organic molecules: gap of order 1 V

Theoretical Approach: Two Main Ingredients 1. Transmission of incident flux: Single-particle electron states Energy of relevant states are in window determined by ev about Fermi energy Consider flux impinging on molecule from lead 1 How much gets transmitted? Method (1) µ 1 µ 2 I lead 1 molecule lead 2 V 2. Electronic structure from Density Functional Theory in local approx. Use Kohn-Sham theory to get self-consistent equilibrium density & structure Reliable! lots of experience in quantum chemistry Use Kohn-Sham single-particle states for transmission NOT JUSTIFIED! For non-equilibrium, get self-consistent density matrix by filling states coming from lead 1 to µ 1 and states coming from lead 2 to µ 2

Computational Methods molecule lead 1 lead 2 Method (2) extended molecule Semi-infinite leads at constant µ (no voltagle drop); no spin polarization Extended molecule: include large amount of leads in the molecule First-principles DFT theory using SIESTA program (Double-zeta plus polarization Comp. basis set, Tech. optimized Troullier-Martins pseudopotentials, PBE version of GGA functional for exchange-correlation) Transmission from Green function built from Kohn-Sham orbitals San-Huang Ke, H.U.Baranger, and W. Yang, PRB (2004) Datta group, PRB (2001); Ratner group, Chem. Phys. (2002); Guo group, PRB (2003)

Vary surface [(111) or (100)], adsorption site, linking atom (S, Se, or Te), type of lead (thin, infinite surface, surface+protrusion) Benzene: structures [San-Huang Ke] Simple case: 1 Carbon ring + S to bond to Au

Transmission for benzenedithiol+au: Surface+protrusion Benzene: T [San-Huang Ke]

Additional Au makes a difference: T(E) resonance and NDR! Benzene: I-V transmission resonance at Fermi energy negative differential resistance [San-Huang Ke]

Image resonant state Benzene: ldos Surface of constant local density of states: (ie. one contour of a 3d contour plot) ρ ( r, ) = E F constant [San-Huang Ke]

Carbon nanotube Metal electrode contact How good NT-met can the electrical struc contact be? Does it depend on the metal? Try to make an ideal contact, to set a bound: assume metal wets tube, many strong bonds are formed! 3 terminal transmission [San-Huang Ke]

Au Pd (5,5) Tube 7 layers of Au or Pd 5x5, 3Term, 7L excellent contact!! [San-Huang Ke]

(5,5) Tube: Evolution with width of metal electrode 5x4, 3Term, 3/5L [San-Huang Ke]

(10,0) Tube Doped and undoped 2 Terminal 10x0, 2Term [San-Huang Ke]

(10,0) Tube: 3 Terminal Transmission 10x0, 3Term Again, Pd make a better contact than Au [San-Huang Ke]

Metallocenes: Organometallic Sandwich Complexes Metallocenes M=Fe: ferrocene 6 electrons in levels in box S=0 M=Co: cobaltocene 7 electrons in levels in box S=1/2 [Rob Toreki, Organometallic HyperTextBook]

Experiment: I-V of a phenyl-ethynyl-ferrocene complex Fcene: data 1!!! [Getty, Engtrakul, Wang, Fuhrer, and Sita; U. Maryland; PRB `05]

Experiment: I-V of Ferrocene-OPE compared to OPE Fcene: data 2!!!!!! [Getty, Engtrakul, Wang, Fuhrer, and Sita; U. Maryland]

Conductance of Ferrocene-OPE: Calculation Fcene: calc resonance at the Fermi energy [Rui Liu]

But what about the OPE control? It ALSO conducts Fcene: control This embarassing result is an example of a long-standing problem in the theory of transport through molecules: theory says fully conjugated molecules should conduct, while experiment shows that they do not. Not clear why: because of using the Kohn- Sham wave-functions to find the transmission? local exchange-correlation? (ie. self-interaction?) failure to include interactions in transport calculation? The fact that the Fc molecule avoids this embarassment is an important clue

Cobaltocene: One more electron in a nice place lowest energy bonding state: Cobaltocene increasing energy e 2g e 2g a 1g e 1u

Cobaltocene Rectifier Rectifier: Conducts Rectifier: under forward bias, I-V but not under reverse bias [Rui Liu]

Transmission Resonances in Cobaltocene Rectifier Density of states projected Rectifier: on molecule T, ldos Transmission (E,V) Resonance A (HOMO at V=0): Resonance B (LUMO at V=0): [Rui Liu]

Potential Drop in Rectifier Rectifier: potential [Rui Liu]

Spin active molecule Use Cobaltocene s Spin: Molecular Spintronics Goal: Move spin active parts from leads into molecules Spin active molecule Cobaltocene spin filter: Apply B field to align spin of cobaltocene; Current is spin polarized

Spintronic Switch using Ferromagnetic Metals Spintronic switch Density of states at E F for Majority (minority) spin state Also works if N is an insulator: Tunneling Magneto-Resistance (TMR)

Spintronic Switch in a Molecule with 2 Cobaltocenes dico: energetics dico dico-2c Energetics of the singlet-triplet splitting Molecule E(S=1) E(S=0) Inverting B field (g=2) DiCo 12 mev 120 T DiCo-2C 2 mev 20 T DiCo-4C ~0.1 mev ~1 T Ground state => S=0 (super-exchange*). The more insulating the spacer, the smaller the energy difference. B field needed to excite molecule from S=0 to S=1 depends on spacer *The term used for the indirect exchange coupling of unpaired spins via orbitals having paired spins.

Transmission of di-cobaltocene Molecules: A Good Switch and Spin-Valve! dico: T dico dico-2c [Rui Liu]

Conclusions Though the methods Conclusion used are, in general, not quantitative, we have learned some general lessons: Contact atomic structure does matter! additional Au caused a dramatic increase of conductance Excellent Pd/Nanotube contact; even ideal Au is good Ferrocene containing molecule has good conductance! Cobaltocene has a very nice additional electron: * resonance near the Comp. Fermi energy Tech. of Au * unpaired spin to use for spintronics Credits: Rui Liu, San-Huang Ke, Weitao Yang, and HUB Expt: Stephanie Getty, Michael Fuhrer, Larry Sita, and team