Help me understanding the effect of organic acceptor molecules on coinage metals.
|
|
- Owen Barrett
- 5 years ago
- Views:
Transcription
1 Help me understanding the effect of organic acceptor molecules on coinage metals. Gerold M. Rangger, 1 Oliver T. Hofmann, 1 Anna M. Track, 1 Ferdinand Rissner, 1 Lorenz Romaner, 1,2 Georg Heimel, 2 Benjamin Bröker, 3 Ralf-Peter Blum, 3 Norbert Koch 3, and Egbert Zojer 1 1 Inst. für Festkörperphysik, Technische Universität Graz, 8010 Graz, Austria. 2 Dep. of Material Physics, University of Leoben, 8700 Leoben, Austria. 3 Inst. für Physik, Humboldt-Universität zu Berlin, Berlin, Germany. Festkörperphysikseminar WS 2008/09 Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 1
2 Help, just anybody Why does F4 bond? F4TCNQ (2,3,5,6-tetrafluoro-7,7,8,8-tetracyanoquinodimethane) N F F N N F F N on Ag(111), Au(111), Cu(111) ML coverage, loosely packed Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 2
3 OUTLINE F 4 TCNQ on Ag(111) charge transfer work-function modification geometric distortions Comparison: theory versus experiment Ag versus Au (Cu) COOP bond-lenght changes binding energy Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 3
4 Motivation reduction of the hole injection barrier N. Koch, et al Phys. Rev. Lett. 2005, 95, increase in work function charge transfer from metal to molecule (filling of the LUMO) from molecule to metal? adsorption-induced geometry change help our friends the chemists to design new acceptors Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 4
5 Experimental/Theoretical data for F 4 TCNQ Ag(111): ( theoretical, experimental paper to be published) Reduction of hole injection barrier UPS (Ultraviolet photoelectron spectroscopy) XPS (X-ray photoemission spectroscopy) work-function modification Au(111): (N. Koch, et al PRL 2005, 95, ,Jäckel et al. PRL 100, , 2008) UPS XPS low temperature STM (scanning tunneling microscopy) Cu(111): (Romaner et al. PRL 99, , 2007) UPS XSW (X-ray standing wave) Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 5
6 Setup: F 4 TCNQ Monolayer coverage STM Sub-monolayer coverage (3 3 x 5) Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 6
7 Theory details - DFT VASP 1 Plane wave Slab calculations SIESTA 2 LCAO code 1 further details: L. Romaner et al., Phys. Rev. Lett. 99, , further detailes: L. Romaner et al., Small 2006; 2: 1468 Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 7
8 F 4 TCNQ on Ag - UPS spectra and MDOS additional new peak charge transfer metal to molecule =E F UPS signal of bare Ag(111) subtracted from that of a surface covered with ca. one monolayer. MDOS energy scale has not been shifted or expanded Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 8
9 bond-length change (Ag) N F F N N F F N Isolated molecule Adsorbed molecule driving force for electron transfer Quinoidal Adsorption aromatic stabilisation Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 9
10 3D charge rearrangements F4TCNQ on Ag(111) at ML coverage LUMO electrons flow from dark to bright areas Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 10
11 plane integrated charge rearrangements ρ + ( ) ( r ) = ρ( r ) ρ ( r ) ρ ( r ) Δ bond Ag (111) mono Q bond ( z) Δ ρ = z 0 bond ( ' z ) dz ' 2 e E ε Δρ 0 ( r ) = ( r ) bond BD Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 11
12 MODOS of selected orbitals of F4TCNQ o some show strong hybridization Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 12
13 Orbital Occupation of F 4 TCNQ on Ag LUMO largly filled HOMO-(9-12) forward donation from deep lying orbitals LUMO projection method: G. M. Rangger et al., Surf. and Interf. Anal. 40, 371, 2008 Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 13
14 work-function modification 1. metal to molecule charge transfer 2. molecule to metal back charge transfer Ag: Experiment Calculation Difference Φmet 4.5 ev 4.5 ev 0.0 ev ΔΦ 0.70 ev 0.85 ev ev Au: Experiment Calculation Difference Φmet 5.3 ev 5.2 ev -0.1 ev ΔΦ 0.35 ev 0.29 ev ev Cu: Experiment Calculation Difference Φmet 4.9 ev 4.8 ev -0.1 ev ΔΦ 0.55 ev 0.20 ev ev Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 14
15 work-function modification, ΔΦ ΔΦ = ΔE vac + BD ΔE vac BD Def. in analogy to SAMs Heimel et al. Acc. of Chem. Res. 41, 721, 2008 Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 15
16 F 4 TCNQ monolayer ΔE vac... electron potential energy difference of F 4 TCNQ layer proportional to molecular dipole moment ML φ Left ML φ Right geometry induced contribution Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 16
17 Coverage Summary F4TCNQ Ag Metal Area (Ų) Φ (ev / D) E vac (ev / D) BD (ev / D) Q bond (e) E bind (ev) Ag ML / / / Ag subml / / / Ratio / / / slightly sub-linear change maximum of Q bond same stronger bond in ML setup Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 17
18 charge rearrangements peculiar arrangement at ML cov. BUT Δρ bond DIFFERS no metal shown Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 18
19 coverage - experiment work function increase linear relationship at sub-monolayer coverage Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 19
20 coverage - UPS 3 adsorption features appear LUMO HOMO HOMO-1 Does the LUMO peak shift? same subml to ML shift Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 20
21 COOP, a suitable tool? old chemical concept: Hofmann, Rev. Mod. Phys. 60, 1988; Dronskowski, J.Phys.Chem, 97, 1993; Grechnev, J.Phys.:Condens.Matter, 15, 2003 COOP ij ( E) = c l, k * ik c jk Sˆ ijk ( E orbital population weighted DOS positive: bonding negative: antibonding amplitude: number of states in energy intervall magnitude: coupling overlap and size of cs δ ε lk ) Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 21
22 MO diagramm of CO un-occupied occupied Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 22
23 CO as example Integration up to E F ToP=0.83 E F Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 23
24 F4TCNQ Ag(111) ML N Bonding, only due to N atoms? TEST: straight F4 vs. bent Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 24
25 straight vs. bent N s, N pz Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 25
26 COOP isolated versus adsorbed Total overlap population of the molecule Isolated Ag ML Au ML Ag sml Cu sml Cu sml (XSW) Molecule Mol-Met Total xxxxx molecule 2 metal COOP Cu sml Ag ML Au ML (XSW) (sml) 100 (66) % 79 (69) % 34 % Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 26
27 COOP vs. bond-lenght changes Ag sml Ag ML Au ML Cu sml Cu sml 1 difference COOP C1-C C2-C C3-C C7-C C12-N C2-F XSW Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 27
28 total COOP vs. binding energy Binding energy Ag/ML Ag/sML Au ML Cu sml F4TCNQ ( ev) In % Area (A²) (BE/area)* In % COOP F4TCNQ In % Area (BE/area)* In % Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 28
29 Conclusions Experimental results (qualitatively) reproduced Molecule bends upon adsorption (XSW) Work-function increase! Subtle interplay between charge transfer and distortion induced dipole Chemical bonding via charge forward and backward donation Different behavior of F 4 TCNQ Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 29
30 Conclusions bond towards metal increases COOP bent of molecule increases COOP F4TCNQ CN groups strong docking groups N s and N pz orbtials interact with metal d-band agreement: bond-lenght changes and E bind Questions: analysis of docking groups which ones are stronger, why? Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 30
31 Acknoledgements Theory: Oliver T. Hofmann Anna M. Track Ferdinand Rissner Lorenz Romaner Georg Heimel Egbert Zojer Jean-Luc Bredás Experiments: Benjamin Bröker, Ralf-Peter Blum, Steffen Duhm, Norbert Koch For financial support: European commision Strep (EC-STREP ), ISOTEC/SENSPHYS Help me if you can, I m feeling down and I do appreciate you beeing around Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 31
32 MDOS of F 4 TCNQ on Ag (Coverage) Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 32
33 MODOS of LUMO and HOMO-10 most DOS of LUMO below Fermi energy Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 33
34 electron density: F 4 TCNQ on Cu vs. Ag metallic character extended Graz, Professor 11/19/2008 Horst Cerjak, Help me understanding the effect of organic acceptor molecules on coinage metals 34
Metal/Organic Interfaces
Metal/Organic Interfaces from first-principles Georg Heimel Institut für f r Physik, Humboldt-Universit Universität t zu Berlin Dresden, 12.02.2009 Outline Investigated Systems / Motivation Methods Overview
More informationFunctional interfaces with conjugated organic materials: energy level tuning and "soft" metallic contacts
unctional interfaces with conjugated organic materials: energy level tuning and "soft" metallic contacts Norbert Koch Emmy Noether-Nachwuchsgruppe "Supramolecular Systems" Institut für Physik Humboldt-Universität
More informationElectronic Supporting Information for
Electronic Supplementary Material (ESI) for Materials Horizons. This journal is The Royal Society of Chemistry 2015 Electronic Supporting Information for Probing the Energy Levels in Hole-doped Molecular
More informationA Momentum Space View of the Surface Chemical Bond - Supplementary Information
A Momentum Space View of the Surface Chemical Bond - Supplementary Information Stephen Berkebile, a Thomas Ules, a Peter Puschnig, b Lorenz Romaner, b Georg Koller, a Alexander J. Fleming, a Konstantin
More informationSubstrate-mediated band-dispersion of adsorbate molecular states - Supplementary Information
Substrate-mediated band-dispersion of adsorbate molecular states - Supplementary Information M. Wießner, 1, 2 J. Ziroff, 1, 2 F. Forster, 1, 2 M. Arita, 3 K. Shimada, 3 P. Puschnig, 4 A. Schöll*, 1, 2,
More informationX-ray diffraction and Crystal Structure Solutions from Thin Films
X-ray diffraction and Crystal Structure Solutions from Thin Films Ingo Salzmann Humboldt-Universität zu Berlin Institut für Physik Overview Experimental technique X-ray diffraction The principal phenomenon
More informationImpact of collective effects on charge transport through molecular monolayers
Impact of collective effects on charge transport through molecular monolayers Obersteiner Veronika Institute of Solid State Physics 11.12.2013 Outline Introduction Motivation Investigated Systems Methodology
More informationTable S2. Pseudopotentials PBE 5.2 applied in the calculations using VASP
Supporting Information for Understanding the Adsorption of CuPc and ZnPc on Noble Metal Surfaces by Combining Quantum-Mechanical Modelling and Photoelectron Spectroscopy 1. Used vdw Coefficients PBE-vdW
More informationOrbital Tomography: A Method to Obtain the Orbital-Projected DOS from ARPES
Orbital Tomography: A Method to Obtain the Orbital-Projected DOS from ARPES Motivation ARPES data from Stephen Berkebile et al. (2007) hν (21eV) ARPES Intensity e- (20-3) Uniaxially ordered para-sexiphenyl
More informationPOST-ADSORPTION WORK FUNCTION TUNING
Supporting Information POST-ADSORPTION WORK FUNCTION TUNING VIA HYDROGEN PRESSURE CONTROL Hermann Edlbauer, Egbert Zojer, and Oliver T. Hofmann* Institute for Solid State Physics, NAWI Graz, Graz University
More informationDithiocarbamate Self-Assembled Monolayers as Efficient Surface Modifiers for Low Work Function Noble Metals
Dithiocarbamate Self-Assembled Monolayers as Efficient Surface Modifiers for Low Work Function Noble Metals Dominik Meyer*,1, Tobias Schäfer 1, Philip Schulz 1,2,3, Sebastian Jung 1, Daniel Mokros 1, Ingolf
More informationSpectroscopies for Unoccupied States = Electrons
Spectroscopies for Unoccupied States = Electrons Photoemission 1 Hole Inverse Photoemission 1 Electron Tunneling Spectroscopy 1 Electron/Hole Emission 1 Hole Absorption Will be discussed with core levels
More informationIn the field of organic electronics, controlling the work
Work-Function Modification beyond Pinning: When Do Molecular Dipoles Count? Oliver T. Hofmann, David A. Egger, and Egbert Zojer* Institut für Festkörperphysik, Technische Universität Graz, Petersgasse
More informationQuantum wells and Dots on surfaces
Lecture in the course Surface Physics and Nano Physics 2008 Quantum wells and Dots on surfaces Bo Hellsing Department of Physics, Göteborg University, Göteborg, S Collaborators: QW Johan Carlsson, Göteborg
More informationThe symmetry properties & relative energies of atomic orbitals determine how they react to form molecular orbitals. These molecular orbitals are then
1 The symmetry properties & relative energies of atomic orbitals determine how they react to form molecular orbitals. These molecular orbitals are then filled with the available electrons according to
More informationGrowth and Electronic Structure of Organic Molecular Layers Studied by Density Functional Theory
Growth and Electronic Structure of Organic Molecular Layers Studied by Density Functional Theory Slide 1 Motivation OLED para-sexiphenyl (6P) (C36H26) OFET Pentacene (5A) (C22H14) Slide 2 Outline 1. Density
More informationContrasting Pentacene on Cu(110) and Ag(110): interactions revealed by valence band tomography
Contrasting Pentacene on Cu(110) and Ag(110): interactions revealed by valence band tomography Ules Thomas Surface Science Group, KFUni Graz Outline Angle Resolved UPS; Orbital Tomography Influence of
More informationSupplementary Figure 1: Change of scanning tunneling microscopy (STM) tip state. a, STM tip transited from blurred (the top dark zone) to orbital
Supplementary Figure 1: Change of scanning tunneling microscopy (STM) tip state. a, STM tip transited from blurred (the top dark zone) to orbital resolvable (the bright zone). b, Zoomedin tip-state changing
More informationValence bond theory accounts, at least qualitatively, for the stability of the covalent bond in terms of overlapping atomic orbitals.
Molecular Orbital Theory Valence bond theory accounts, at least qualitatively, for the stability of the covalent bond in terms of overlapping atomic orbitals. Using the concept of hybridization, valence
More information1s atomic orbital 2s atomic orbital 2s atomic orbital (with node) 2px orbital 2py orbital 2pz orbital
Atomic Orbitals 1s atomic orbital 2s atomic orbital 2s atomic orbital (with node) 2px orbital 2py orbital 2pz orbital Valence Bond Theory and ybridized Atomic Orbitals Bonding in 2 1s 1s Atomic Orbital
More informationIn order to determine the energy level alignment of the interface between cobalt and
SUPPLEMENTARY INFORMATION Energy level alignment of the CuPc/Co interface In order to determine the energy level alignment of the interface between cobalt and CuPc, we have performed one-photon photoemission
More informationSupplementary Figures
Supplementary Figures Supplementary Figure 1 Measured versus calculated optical transitions in the CPX. The UV/Vis/NIR spectrum obtained experimentally for the 1:1 blend of 4T and F4TCNQ (red curve) is
More informationA high-pressure-induced dense CO overlayer on Pt(111) surface: A chemical analysis using in-situ near ambient pressure XPS
Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics. This journal is the Owner Societies 2014 Electronic Supplementary Information for A high-pressure-induced dense CO overlayer
More informationSfb 658 Colloquium 11 May Part II. Introduction to Two-Photon-Photoemission (2PPE) Spectroscopy. Martin Wolf
Sfb 658 Colloquium 11 May 2006 Part II Introduction to Two-Photon-Photoemission (2PPE) Spectroscopy Martin Wolf Motivation: Electron transfer across interfaces key step for interfacial and surface dynamics
More informationPart III: Theoretical Surface Science Adsorption at Surfaces
Technische Universität München Part III: Theoretical Surface Science Adsorption at Surfaces Karsten Reuter Lecture course: Solid State Theory Adsorption at surfaces (T,p) Phase II Phase I Corrosion Growth
More informationProbing Matter: Diffraction, Spectroscopy and Photoemission
Probing Matter: Diffraction, Spectroscopy and Photoemission Anders Nilsson Stanford Synchrotron Radiation Laboratory Why X-rays? VUV? What can we hope to learn? 1 Photon Interaction Incident photon interacts
More informationSite- and orbital-dependent charge donation and spin manipulation in electron-doped metal phthalocyanines
Site- and orbital-dependent charge donation and spin manipulation in electron-doped metal phthalocyanines Cornelius Krull 1, Roberto Robles 2, Aitor Mugarza 1, Pietro Gambardella 1,3 1 Catalan Institute
More informationSurface Transfer Doping of Diamond by Organic Molecules
Surface Transfer Doping of Diamond by Organic Molecules Qi Dongchen Department of Physics National University of Singapore Supervisor: Prof. Andrew T. S. Wee Dr. Gao Xingyu Scope of presentation Overview
More informationBe H. Delocalized Bonding. Localized Bonding. σ 2. σ 1. Two (sp-1s) Be-H σ bonds. The two σ bonding MO s in BeH 2. MO diagram for BeH 2
The Delocalized Approach to Bonding: The localized models for bonding we have examined (Lewis and VBT) assume that all electrons are restricted to specific bonds between atoms or in lone pairs. In contrast,
More informationCurriculum Vitae December 2006
Appendix: (A brief description of some representative results) (1) Electronic states of Pb adatom and Pb adatom chains on Pb(111) have been investigated by spatially scanning tunneling spectroscopy (STS)
More informationMolecular Orbital Theory. Molecular Orbital Theory: Electrons are located in the molecule, not held in discrete regions between two bonded atoms
Molecular Orbital Theory Valence Bond Theory: Electrons are located in discrete pairs between specific atoms Molecular Orbital Theory: Electrons are located in the molecule, not held in discrete regions
More informationAdsorption, desorption, and diffusion on surfaces. Joachim Schnadt Divsion of Synchrotron Radiation Research Department of Physics
Adsorption, desorption, and diffusion on surfaces Joachim Schnadt Divsion of Synchrotron Radiation Research Department of Physics Adsorption and desorption Adsorption Desorption Chemisorption: formation
More informationPhoton Interaction. Spectroscopy
Photon Interaction Incident photon interacts with electrons Core and Valence Cross Sections Photon is Adsorbed Elastic Scattered Inelastic Scattered Electron is Emitted Excitated Dexcitated Stöhr, NEXAPS
More informationElectronic Structure of Surfaces
Electronic Structure of Surfaces When solids made of an infinite number of atoms are formed, it is a common misconception to consider each atom individually. Rather, we must consider the structure of the
More informationSurface Characte i r i zat on LEED Photoemission Phot Linear optics
Surface Characterization i LEED Photoemission Linear optics Surface characterization with electrons MPS M.P. Seah, WA W.A. Dench, Surf. Interf. Anal. 1 (1979) 2 LEED low energy electron diffraction De
More informationSupplementary Figure 1 Irregular arrangement of E,E-8-mer on TMA. STM height images formed when
Supplementary Figure 1 Irregular arrangement of E,E-8-mer on TMA. STM height images formed when a 5 µl heptanoic acid solution of E,E-8-mer is applied on: (a) a TMA templated HOPG substrate, U s = +1.00
More informationSpectroscopy of Nanostructures. Angle-resolved Photoemission (ARPES, UPS)
Spectroscopy of Nanostructures Angle-resolved Photoemission (ARPES, UPS) Measures all quantum numbers of an electron in a solid. E, k x,y, z, point group, spin E kin, ϑ,ϕ, hν, polarization, spin Electron
More informationMolecular Orbital Theory
Molecular Orbital Theory 1. MO theory suggests that atomic orbitals of different atoms combine to create MOLECULAR ORBITALS 2. Electrons in these MOLECULAR ORBITALS belong to the molecule as whole 3. This
More informationOutline. Introduction: graphene. Adsorption on graphene: - Chemisorption - Physisorption. Summary
Outline Introduction: graphene Adsorption on graphene: - Chemisorption - Physisorption Summary 1 Electronic band structure: Electronic properties K Γ M v F = 10 6 ms -1 = c/300 massless Dirac particles!
More informationSupporting Information. for. Angew. Chem. Int. Ed. Z Wiley-VCH 2003
Supporting Information for Angew. Chem. Int. Ed. Z52074 Wiley-VCH 2003 69451 Weinheim, Germany Kinetic and Thermodynamic Control via Chemical Bond Rearrangement on Si(001) Surface Chiho Hamai, Akihiko
More informationOrganic semiconductor heterointerfaces containing bathocuproine
JOURNAL OF APPLIED PHYSICS VOLUME 86, NUMBER 8 15 OCTOBER 1999 Organic semiconductor heterointerfaces containing bathocuproine I. G. Hill a) and A. Kahn Department of Electrical Engineering, Princeton
More informationFunctional Group Adsorption on Calcite: I. Oxygen Containing and Nonpolar Organic Molecules
SUPPORTING INFORMATION Functional Group Adsorption on Calcite: I. Oxygen Containing and Nonpolar Organic Molecules E. Ataman*, M. P. Andersson, M. Ceccato, N. Bovet, S. L. S. Stipp Nano-Science Center,
More informationUltraviolet Photoelectron Spectroscopy (UPS)
Ultraviolet Photoelectron Spectroscopy (UPS) Louis Scudiero http://www.wsu.edu/~scudiero www.wsu.edu/~scudiero; ; 5-26695 scudiero@wsu.edu Photoemission from Valence Bands Photoelectron spectroscopy is
More informationNH 3 H 2 O N 2. Why do they make chemical bonds? Molecular Orbitals
N 2 NH 3 H 2 O Why do they make chemical bonds? 5 Molecular Orbitals Why do they make chemical bonds? Stabilization Bond energy Types of Chemical Bonds Metallic Bond Ionic Bond Covalent Bond Covalent Bond
More informationSupplementary Figure 1 Experimental setup for crystal growth. Schematic drawing of the experimental setup for C 8 -BTBT crystal growth.
Supplementary Figure 1 Experimental setup for crystal growth. Schematic drawing of the experimental setup for C 8 -BTBT crystal growth. Supplementary Figure 2 AFM study of the C 8 -BTBT crystal growth
More informationTheory of doping graphene
H. Pinto, R. Jones School of Physics, University of Exeter, EX4 4QL, Exeter United Kingdom May 25, 2010 Graphene Graphene is made by a single atomic layer of carbon atoms arranged in a honeycomb lattice.
More informationSpectroscopy at nanometer scale
Spectroscopy at nanometer scale 1. Physics of the spectroscopies 2. Spectroscopies for the bulk materials 3. Experimental setups for the spectroscopies 4. Physics and Chemistry of nanomaterials Various
More informationX-ray Spectroscopy. Interaction of X-rays with matter XANES and EXAFS XANES analysis Pre-edge analysis EXAFS analysis
X-ray Spectroscopy Interaction of X-rays with matter XANES and EXAFS XANES analysis Pre-edge analysis EXAFS analysis Element specific Sensitive to low concentrations (0.01-0.1 %) Why XAS? Applicable under
More informationSupporting Information for. Employing X-ray Photoelectron Spectroscopy for Determining Layer Homogeneity in Mixed Polar Self-Assembled Monolayers
Supporting Information for Employing X-ray Photoelectron Spectroscopy for Determining Layer Homogeneity in Mixed Polar Self-Assembled Monolayers Iris Hehn, 1& Swen Schuster, 2& Tobias Wächter, 2 Tarek
More informationScanning Tunneling Microscopy. how does STM work? the quantum mechanical picture example of images how can we understand what we see?
Scanning Tunneling Microscopy how does STM work? the quantum mechanical picture example of images how can we understand what we see? Observation of adatom diffusion with a field ion microscope Scanning
More information5.80 Small-Molecule Spectroscopy and Dynamics
MIT OpenCourseWare http://ocw.mit.edu 5.80 Small-Molecule Spectroscopy and Dynamics Fall 2008 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms. 5.80 Lecture
More informationChemical Bonding. Lewis Theory-VSEPR Valence Bond Theory Molecular Orbital Theory
Chemical Bonding Lewis Theory-VSEPR Valence Bond Theory Molecular Orbital Theory Problems with Valence Bond Theory VB theory predicts properties better than Lewis theory bonding schemes, bond strengths,
More informationSupplementary Information. Spin coupling and relaxation inside molecule-metal contacts
Supplementary Information Spin coupling and relaxation inside molecule-metal contacts Aitor Mugarza 1,2*, Cornelius Krull 1,2, Roberto Robles 2, Sebastian Stepanow 1,2, Gustavo Ceballos 1,2, Pietro Gambardella
More informationMicroscopy and Spectroscopy with Tunneling Electrons STM. Sfb Kolloquium 23rd October 2007
Microscopy and Spectroscopy with Tunneling Electrons STM Sfb Kolloquium 23rd October 2007 The Tunnel effect T ( E) exp( S Φ E ) Barrier width s Barrier heigth Development: The Inventors 1981 Development:
More informationCatalytic Activity of IrO 2 (110) Surface: A DFT study
Catalytic Activity of IrO 2 (110) Surface: A DFT study Jyh-Chiang Jiang Department of Chemical Engineering, National Taiwan University of Science and Technology (NTUST) NCTS-NCKU 9/7, 2010 Computational
More informationBonds to Bands. An introduction to basic concepts in solid state and surface bonding and electronic structure.
Bonds to Bands An introduction to basic concepts in solid state and surface bonding and electronic structure. Basic classes of bonding Basic concepts in quantum chemistry LCAO and molecular orbital theory
More informationAdsorption: Physisorption and chemisorption
Adsorption: Physisorption and chemisorption Molecules interact with surfaces with forces originating either from the physical Van der Waals interaction or from the chemical hybridization of their orbitals
More informationThe,electronic structure of adsorbed aromatic molecules: Perylene and PTCDA on Si( 111) and Ag( 111)
Journal of Molecular Structure, 293 (1993) 239-244 Elsevier Science Publishers B.V., Amsterdam 239 The,electronic structure of adsorbed aromatic molecules: Perylene and PTCDA on Si( 111) and Ag( 111) M.
More informationPolaron Transport in Organic Crystals: Theory and Modelling
Polaron Transport in Organic Crystals: Theory and Modelling Karsten Hannewald Institut für Physik & IRIS Adlershof Humboldt-Universität zu Berlin (Germany) Karsten Hannewald (HU Berlin/Germany) www.ifto.uni-jena.de/~hannewald/
More informationX-ray Spectroscopy Theory Lectures
TIMES Lecture Series SIMES-SLAC-Stanford Winter, 2017 X-ray Spectroscopy Theory Lectures J. J. Rehr I. Introduction to the Theory of X-ray spectra II. Real-space Green's function Theory and FEFF III. Inelastic
More informationdesorption (ESD) of the O,/Si( 111) surface K. Sakamoto *, K. Nakatsuji, H. Daimon, T. Yonezawa, S. Suga
-!!!I c%sj ELSEVIER Surface Science 306 (1994) 93-98.:.:.j:::~:::~~~::::::~:~::~~:~~,:~.~...,.. ~. :...:E.:.:: :.:.::::::~.:.:.:.:.:.:.,:.:,:,:. ~.~:+::.:.::::::j:::~::::.:...( ~ :.:.::.:.:.:,:..:,: :,,...
More informationSelf-assembly of molecules on surfaces. Manuel Alcamí Departamento de Química Universidad Autónoma de Madrid
Self-assembly of molecules on surfaces Manuel Alcamí Departamento de Química Universidad Autónoma de Madrid Outline Outline Motivation Examples of molecules deposited on surfaces Graphene/Ru(0001) TQ /
More informationPCCP PERSPECTIVE. The interplay between interface structure, energy level alignment and chemical bonding strength at organic metal interfaces
PERSPECTIVE View Article Online View Journal View Issue Cite this: Phys. Chem. Chem. Phys., 2015, 17, 1530 Received 10th October 2014, Accepted 19th November 2014 DOI: 10.1039/c4cp04595e www.rsc.org/pccp
More informationMolybdenum compound MoP as an efficient. electrocatalyst for hydrogen evolution reaction
Electronic Supplementary Material (ESI) for Energy & Environmental Science. This journal is The Royal Society of Chemistry 2014 Molybdenum compound MoP as an efficient electrocatalyst for hydrogen evolution
More informationELEMENTARY BAND THEORY
ELEMENTARY BAND THEORY PHYSICIST Solid state band Valence band, VB Conduction band, CB Fermi energy, E F Bloch orbital, delocalized n-doping p-doping Band gap, E g Direct band gap Indirect band gap Phonon
More informationEnergy level alignment and two-dimensional structure of pentacene on Au 111 surfaces
JOURNAL OF APPLIED PHYSICS VOLUME 91, NUMBER 5 1 MARCH 2002 Energy level alignment and two-dimensional structure of pentacene on Au 111 surfaces P. G. Schroeder, C. B. France, J. B. Park, and B. A. Parkinson
More informationModeling Ultrafast Deactivation in Oligothiophenes via Nonadiabatic Dynamics
Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics. This journal is the Owner Societies 2015 Supplementary Data for Modeling Ultrafast Deactivation in Oligothiophenes via Nonadiabatic
More informationElectron transport through Shiba states induced by magnetic adsorbates on a superconductor
Electron transport through Shiba states induced by magnetic adsorbates on a superconductor Michael Ruby, Nino Hatter, Benjamin Heinrich Falko Pientka, Yang Peng, Felix von Oppen, Nacho Pascual, Katharina
More informationSUPPLEMENTARY INFORMATION
Simultaneous and coordinated rotational switching of all molecular rotors in a network Y. Zhang, H. Kersell, R. Stefak, J. Echeverria, V. Iancu, U. G. E. Perera, Y. Li, A. Deshpande, K.-F. Braun, C. Joachim,
More informationSUPPLEMENTARY INFORMATION
SUPPLEMENTARY INFORMATION Conductance Measurements The conductance measurements were performed at the University of Aarhus. The Ag/Si surface was prepared using well-established procedures [1, 2]. After
More informationFormation of Halogen Bond-Based 2D Supramolecular Assemblies by Electric Manipulation
Formation of Halogen Bond-Based 2D Supramolecular Assemblies by Electric Manipulation Qing-Na Zheng, a,b Xuan-He Liu, a,b Ting Chen, a Hui-Juan Yan, a Timothy Cook, c Dong Wang* a, Peter J. Stang, c Li-Jun
More information2) Atom manipulation. Xe / Ni(110) Model: Experiment:
2) Atom manipulation D. Eigler & E. Schweizer, Nature 344, 524 (1990) Xe / Ni(110) Model: Experiment: G.Meyer, et al. Applied Physics A 68, 125 (1999) First the tip is approached close to the adsorbate
More informationModellierung molekularer Prozesse beim Wachstum organischer Schichten
Modellierung molekularer Prozesse beim Wachstum organischer Schichten Slide 1 Motivation OLED para Sexiphenyl (6P) (C36H26) OFET Pentacene (5A) (C22H14) Slide 2 Outline Methods and Materials Cohesive,
More informationInteraction between a single-molecule
Interaction between a single-molecule magnet Mn 12 monolayer and a gold surface 12 Kyungwha Park Department of Physics, Virginia Tech Salvador Barraza-Lopez (postdoc) Michael C. Avery (undergraduate) Supported
More informationScanning Tunneling Microscopy (STM)
Page 1 of 8 Scanning Tunneling Microscopy (STM) This is the fastest growing surface analytical technique, which is replacing LEED as the surface imaging tool (certainly in UHV, air and liquid). STM has
More informationSupporting information for Chemical and Electrochemical. Surfaces: Insights into the Mechanism and Selectivity from DFT.
Electronic Supplementary Material (ESI) for RSC Advances. This journal is The Royal Society of Chemistry 2015 Supporting information for Chemical and Electrochemical Hydrogenation of CO 2 to hydrocarbons
More informationLUMO + 1 LUMO. Tómas Arnar Guðmundsson Report 2 Reikniefnafræði G
Q1: Display all the MOs for N2 in your report and classify each one of them as bonding, antibonding or non-bonding, and say whether the symmetry of the orbital is σ or π. Sketch a molecular orbital diagram
More informationScanning tunneling microscopy on unpinned GaN(11 00) surfaces: Invisibility of valence-band states
Scanning tunneling microscopy on unpinned GaN(11 00) surfaces: Invisibility of valence-band states Ph. Ebert, 1, * L. Ivanova, 2 and H. Eisele 2 1 Institut für Festkörperforschung, Forschungszentrum Jülich
More informationStudying Metal to Insulator Transitions in Solids using Synchrotron Radiation-based Spectroscopies.
PY482 Lecture. February 28 th, 2013 Studying Metal to Insulator Transitions in Solids using Synchrotron Radiation-based Spectroscopies. Kevin E. Smith Department of Physics Department of Chemistry Division
More informationDipole formation at metal/ptcda interfaces: Role of the Charge Neutrality Level
EUROPHYSICS LETTERS 15 March 2004 Europhys. Lett., 65 (6), pp. 802 808 (2004) DOI: 10.1209/epl/i2003-10131-2 Dipole formation at metal/ptcda interfaces: Role of the Charge Neutrality Level H. Vázquez 1,
More information1 Adsorption of NO 2 on Pd(100) Juan M. Lorenzi, Sebastian Matera, and Karsten Reuter,
Supporting information: Synergistic inhibition of oxide formation in oxidation catalysis: A first-principles kinetic Monte Carlo study of NO+CO oxidation at Pd(100) Juan M. Lorenzi, Sebastian Matera, and
More informationarxiv:cond-mat/ v1 [cond-mat.mes-hall] 19 Dec 2006
arxiv:cond-mat/678v [cond-mat.mes-hall] 9 Dec 6 Abstract Electronic structure of the Au/benzene-,-dithiol/Au transport interface: Effects of chemical bonding U. Schwingenschlögl, C. Schuster Institut für
More informationThe experimental work seems to be well carried out and the DFT calculations carefully crafted.
Reviewers' comments: Reviewer #1 (Remarks to the Author): The manuscript by Maier et al. reports on the on-surface synthesis of 1D and 2D polymers in ultra-high vacuum. A halogenated triphenylamine precursor
More informationSupporting Information for
Supporting Information for Dipolar Molecular Capping in Quantum Dot-Sensitized Oxides: Fermi Level Pinning Precludes Tuning Donor-Acceptor Energetics Hai I. Wang, 1,2 Hao Lu, 1 Yuki Nagata, 1 Mischa Bonn,
More informationElectronic Properties of Ultimate Nanowires. F. J. Himpsel, S. C. Erwin, I. Barke,
Electronic Properties of Ultimate Nanowires F. J. Himpsel, S. C. Erwin, I. Barke, Nanostructures with Atomic Precision Single-Atom Wire, Single Wave Function Ultimate Limits of Electronics, Data Storage
More informationSUPPLEMENTAL MATERIAL
SUPPLEMENTAL MATERIAL The fhi-aims code [1] was employed for the DFT calculations. The repeated slab method was used to model all the systems with the size of the vacuum gap chosen between 16 and 25 Å.
More informationECE236A Semiconductor Heterostructure Materials Basic Properties of Semiconductor Heterostructures Lectures 2 & 3 Oct. 5, 2017
ECE236A Semiconductor Heterostructure Materials Basic Properties of Semiconductor Heterostructures Lectures 2 & 3 Oct. 5, 217 Basic definitions. Types of band-alignment. Determination of band-offsets:
More informationElectronic Structure Theory for Periodic Systems: The Concepts. Christian Ratsch
Electronic Structure Theory for Periodic Systems: The Concepts Christian Ratsch Institute for Pure and Applied Mathematics and Department of Mathematics, UCLA Motivation There are 10 20 atoms in 1 mm 3
More informationX-Ray Spectroscopy at LCLS
LCLS proposal preparation workshop for experiments at XPP, June 21, 2008, SLAC, Menlo Park, CA ħω ħω e - X-Ray Spectroscopy at LCLS Uwe Bergmann SSRL Stanford Linear Accelerator Center bergmann@slac.stanford.edu
More informationSupporting Information. for. Advanced Materials, adma Wiley-VCH 2005
Supporting Information for Advanced Materials, adma.200501482 Wiley-VCH 2005 69451 Weinheim, Germany Supplementary Material Characterization of SAMs The HBCS monolayers were characterized by XPS, NEXAFS
More informationG. Gantefdr and W. Eberhardt Institut fiir Festkiirperforschung, Forschungszentrum Jiilich, 5170 Jiilich, Germany
Shell structure and s-p hybridization in small aluminum clusters G. Gantefdr and W. Eberhardt Institut fiir Festkiirperforschung, Forschungszentrum Jiilich, 5170 Jiilich, Germany Photoelectron spectra
More informationX-Ray Photoelectron Spectroscopy (XPS)
X-Ray Photoelectron Spectroscopy (XPS) Louis Scudiero http://www.wsu.edu/~scudiero; 5-2669 Electron Spectroscopy for Chemical Analysis (ESCA) The basic principle of the photoelectric effect was enunciated
More informationSpecial Properties of Au Nanoparticles
Special Properties of Au Nanoparticles Maryam Ebrahimi Chem 7500/750 March 28 th, 2007 1 Outline Introduction The importance of unexpected electronic, geometric, and chemical properties of nanoparticles
More informationDensity functional theory study of the energetics, electronic structure, and core-level shifts of NO adsorption on the Pt(111) surface
Density functional theory study of the energetics, electronic structure, and core-level shifts of NO adsorption on the Pt(111) surface Zhen-Hua Zeng, 1, Juarez L. F. Da Silva, 3, * Hui-Qiu Deng, and Wei-Xue
More informationProtection of excited spin states by a superconducting energy gap
Protection of excited spin states by a superconducting energy gap B. W. Heinrich, 1 L. Braun, 1, J. I. Pascual, 1, 2, 3 and K. J. Franke 1 1 Institut für Experimentalphysik, Freie Universität Berlin, Arnimallee
More informationSurvey of structural and electronic properties of C60 on close-packed metal surfaces
Hong Kong Baptist University From the SelectedWorks of Professor Michel Andre Van Hove 2012 Survey of structural and electronic properties of C60 on close-packed metal surfaces Xing-Qiang Shi, Department
More informationa b c Supplementary Figure S1
a b c Supplementary Figure S1 AFM measurements of MoS 2 nanosheets prepared from the electrochemical Liintercalation and exfoliation. (a) AFM measurement of a typical MoS 2 nanosheet, deposited on Si/SiO
More informationExploring the anomalous behavior of metal nanocatalysts with finite temperature AIMD and x-ray spectra
Exploring the anomalous behavior of metal nanocatalysts with finite temperature AIMD and x-ray spectra F.D. Vila DOE grant DE-FG02-03ER15476 With computer support from DOE - NERSC. Importance of Theoretical
More informationAll electron optimized effective potential method for solids
All electron optimized effective potential method for solids Institut für Theoretische Physik Freie Universität Berlin, Germany and Fritz Haber Institute of the Max Planck Society, Berlin, Germany. 22
More information5) Surface photoelectron spectroscopy. For MChem, Spring, Dr. Qiao Chen (room 3R506) University of Sussex.
For MChem, Spring, 2009 5) Surface photoelectron spectroscopy Dr. Qiao Chen (room 3R506) http://www.sussex.ac.uk/users/qc25/ University of Sussex Today s topics 1. Element analysis with XPS Binding energy,
More information