Atomic Scale Coupling of Electromagnetic Radiation to Single Molecules. Wilson Ho University of California, Irvine

Size: px
Start display at page:

Download "Atomic Scale Coupling of Electromagnetic Radiation to Single Molecules. Wilson Ho University of California, Irvine"

Transcription

1

2 Atomic Scale Coupling of Electromagnetic Radiation to Single Molecules Wilson Ho University of California, Irvine

3 Surface Photochemistry

4

5 Direct Adsorbate Excitation

6 Photoelectron Mechanism

7 Objective How to achieve atomic scale resolution in probing matter with electromagnetic radiation? Spectroscopy Optical Phenomena

8 Resolution of Optical Spectroscopy

9 Tip-Induced Plasmon Modes ε t Plasmon ε s Plasmon size : dr

10 Combination of Electromagnetic Radiation With Spatial Resolution of the STM

11 Molecules in Double Barrier Junctions The oxide film spacer increases the lifetime of the transient charged molecular state created after electron injection/withdrawal.

12 Single Molecule Electroluminescence

13 Photon Emission from Single Molecules: Zn-Etioporphyrin on Partially Oxidized NiAl(110) Oxide NiAl(110) Zn-Etioporphyrin

14 Zn(II) Etioporphyrin on Al 2 O 3 & NiAl(110)

15 Mechanism of STM-induced Electroluminescence : Step 1

16 Mechanism of STM-induced Electroluminescence : Step 2

17 Mechanism of STM-induced Electroluminescence : Step 3

18 Light collection setup (electroluminescence) Focusing Lens Mirror 2 Collection Lens Sample Spectrometer & hv CCD Camera Mirror 1 Viewport STM Tip Collection Efficiency: 1% UHV chamber

19 Photon Emission From Molecules on Oxide Films

20 Ag tip Ag tip Photon Energy (ev) Wavelength (nm) TIF Ag vs. W Tips Peak Sequence W tip Ag tip Ag tip W tip Photon Count (arb. unit) Peak Energy (ev)

21 Tunneling Electron Induced Single Molecule Fluorescence: Zn-Etioporphyrin

22 Spatial Dependence of Single Molecule Fluorescence

23 Tunneling Electron Induced Single Molecule Fluorescence

24 LUMO & LUMO + 1: MgP

25 TIF Mechanism 2.0 Energy (ev) Tip evbias -4.0 NiAl Vacuum Oxide

26 RF Induced Rectification Current

27

28 STM Apparatus Low temperature (10 K) ultrahigh vacuum STM

29 Origin of Rectification Current ) cos( 2 t V V V J B ω + = +L + + = ) ( cos ) cos( 2 ) ( ) ( t V dv I d t V dv di V I V I J V J V B B B ω ω +K = 2 ) cos(2 1 ) cos( 2 ) ( ) ( t V dv I d t V dv di V I V I J V J V B B B ω ω + L + = + = V B J B J B R B J B dc dv I d V V I V V I V I V V I ) ( ), ( ) ( ), ( V B J J B R dv I d V V V I ), (

30 Spatial Localization of RF Field

31 Double Modulation Vibrational Rectification

32 Vibrational Rectification Current: C 2 D 2 and C 2 H 2 on Cu(001)

33 Vibrational Rectification Microscopy: C 2 D 2 and C 2 H 2 on Cu(001)

34 Rectification of Single Mn Atom

35 Photon Induced Tunneling

36 Single Molecule Electron Transfer

37 Mechanism of Photon-Induced Electron Transfer to a Single Molecule

38 Photon-Induced Electron Transfer Threshold

39 Photon Induced Tunneling

40 Spatial Variations of Electron Transfer within a Single Molecule

41 Ultrafast Optical Spectroscopy with Spatial Resolution of the STM Femtosecond Lasers: Chemistry at the Temporal Limit Scanning Tunneling Microscopes: Chemistry at the Spatial Limit

42 Acknowledgment Past Present Xi Chen Chi Chen Jennifer Gaudioso Ungdon Ham Jae Ryang Hahn Kiyeo Kim Martin Janson Markus Lackinger Lincoln Lauhon Gary Mikaelian Hyojune Lee George Nazin Joonhee Lee Freddy Toledo Ning Liu Xiuwen Tu Niklas Nilius Shiwei Wu Naoki Ogawa Nilay Pradhan Xiaohui Qiu Mohammad Rezaei Christophe Silien Barry Stipe Mitch Wallis Nicolas Lorente Shiwu Gao Mats Persson

43

44 Prospects Instrumentation Development Electron Spin - microwave-rf excitation - T sub-k, B 10 Tesla Zeeman spectroscopy - spin interactions: Kondo, nanomagnetism Laser-STM - simultaneous spatial + temporal limits 1 Å 10 fs - sub-molecular photochemistry, non-linear optics Non-Vacuum Environment - biological systems

45 < 1 K, 9 Tesla UHV STM

46 Mn Chains: 1 to 16 Atoms

47 Spin-Dependent Tunneling

48

49

50

51 Acknowledgment Past Present Jennifer Gaudioso Chi Chen Jae Ryang Hahn Xi Chen Lincoln Lauhon Ungdon Ham Hyojune Lee Martin Janson Joonhee Lee John Karnes Ning Liu Kiyeo Kim Niklas Nilius Markus Lackinger Nilay Pradhan Gary Mikaelian Xiaohui Qiu George Nazin Mohammad Rezaei Naoki Ogawa Christophe Silien Xiuwen Tu Barry Stipe Shiwei Wu Mitch Wallis Nicolas Lorente Shiwu Gao Mats Persson

52 Atomic Scale Photochemistry Wilson Ho University of California, Irvine

53 Photon Emission from molecules on metal surfaces Photon Count (arb. unit) 400 Ag tip/nial Ag tip/znetioi/nial Metal Molecule Wavelength (nm)

54 Tunneling Electron Induced Single Molecule Fluorescence

55 IET vs. Single Molecule Fluorescence: Inelastic Electron Tunneling Fluorescence

56 Inelastic Electron Tunneling Spectroscopy (STM-IETS)

57

58 Frequency Dependence of RF Voltage Across Junction

59 RF Voltage Across STM Junction: VJ

60 Monitoring Photon-Induced Electron Transfer in a Single Molecule

61 Single Molecule Photon Induced Electron Transfer with Sub-Molecular Spatial Resolution

62 Mg-Porphine Orbitals

63 Single Molecule Vibronic States: MgP

64 Neutral and Charged States: MgP

65 Experimental Setup Focusing Lens Mirror 2 Collection Lens Sample Spectrometer & hv CCD Camera Mirror 1 Viewport STM Tip Collection Efficiency: 0.1% UHV chamber

66 Plasmon modes in the STM junction

67 Double Modulation Spectroscopy Modulate RF Signal at ω c f ( t) = 4 1 sin( nωct) π n (Square Wave 1 to +1 at ω c ) n= 1,3,5... f ( t) = sin( n ω t C ) + π n 2 (Square Wave 0 to +1 at ω c ) n= 1,3, = I( t) I0( VB ) I R sin( nωct) + π n= 1,3,5L n 2 (Modulated Current) 2 I1( t) = I R sin( ωct) π (First Harmonic Signal) 2 1 X 1 ( RMS) = I R π 2 (First Harmonic rms Amplitude) = π 1 (Absolute Rectification Current) I R X 2 Lock-in Sensitivity: 1 na/1 V I R 1 pa I 0 (V B ) 1 na

68 Vibrational Rectification: Single 12 C 16 O & 13 C 18 O

69 Single Molecule Photon Induced Electron Transfer

70 Single Molecule Photon Induced Electron Transfer with Sub-Molecular Spatial Resolution

71 Monitoring Photon-Induced Electron Transfer in a Single Molecule

72 Single Molecule Electron Transfer

Optics and Spectroscopy

Optics and Spectroscopy Introduction to Optics and Spectroscopy beyond the diffraction limit Chi Chen 陳祺 Research Center for Applied Science, Academia Sinica 2015Apr09 1 Light and Optics 2 Light as Wave Application 3 Electromagnetic

More information

Spectroscopy at nanometer scale

Spectroscopy 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 information

Microscopical and Microanalytical Methods (NANO3)

Microscopical and Microanalytical Methods (NANO3) Microscopical and Microanalytical Methods (NANO3) 06.11.15 10:15-12:00 Introduction - SPM methods 13.11.15 10:15-12:00 STM 20.11.15 10:15-12:00 STS Erik Zupanič erik.zupanic@ijs.si stm.ijs.si 27.11.15

More information

Local Optical Spectroscopy using Photon-Scanning Tunneling Microscopy and Beyond

Local Optical Spectroscopy using Photon-Scanning Tunneling Microscopy and Beyond Local Optical Spectroscopy using Photon-Scanning Tunneling Microscopy and Beyond Fernando Stavale and Niklas Nilius Scanning Probe Spectroscopy Group Department of Chemical Physics Fritz-Haber Institut

More information

Chemical imaging of single 4,7,12,15-tetrakis 2.2 paracyclophane by spatially resolved vibrational spectroscopy

Chemical imaging of single 4,7,12,15-tetrakis 2.2 paracyclophane by spatially resolved vibrational spectroscopy THE JOURNAL OF CHEMICAL PHYSICS 127, 244711 2007 Chemical imaging of single 4,7,12,15-tetrakis 2.2 paracyclophane by spatially resolved vibrational spectroscopy N. Liu, a C. Silien, b and W. Ho c Department

More information

Electrical generation and absorption of phonons in carbon nanotubes

Electrical generation and absorption of phonons in carbon nanotubes Electrical generation and absorption of phonons in carbon nanotubes B.J. LeRoy, S.G. Lemay, J. Kong, and C. Dekker Kavli Institute of Nanoscience, Delft University of Technology, Lorentzweg 1, 2628 CJ,

More information

Microscopy and Spectroscopy with Tunneling Electrons STM. Sfb Kolloquium 23rd October 2007

Microscopy 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 information

STM spectroscopy (STS)

STM spectroscopy (STS) STM spectroscopy (STS) di dv 4 e ( E ev, r) ( E ) M S F T F Basic concepts of STS. With the feedback circuit open the variation of the tunneling current due to the application of a small oscillating voltage

More information

Spectroscopy of Nanostructures. Angle-resolved Photoemission (ARPES, UPS)

Spectroscopy 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 information

doi: /PhysRevLett

doi: /PhysRevLett doi: 1.11/PhysRevLett.95.24612 P H Y S I C A L R E V I E W L E E R S week ending Excitation of Molecular Vibrational Modes with Inelastic Scanning unneling Microscopy Processes: Examination through Action

More information

MS482 Materials Characterization ( 재료분석 ) Lecture Note 2: UPS

MS482 Materials Characterization ( 재료분석 ) Lecture Note 2: UPS 2016 Fall Semester MS482 Materials Characterization ( 재료분석 ) Lecture Note 2: UPS Byungha Shin Dept. of MSE, KAIST 1 Course Information Syllabus 1. Overview of various characterization techniques (1 lecture)

More information

Industrial Applications of Ultrafast Lasers: From Photomask Repair to Device Physics

Industrial Applications of Ultrafast Lasers: From Photomask Repair to Device Physics Industrial Applications of Ultrafast Lasers: From Photomask Repair to Device Physics Richard Haight IBM TJ Watson Research Center PO Box 218 Yorktown Hts., NY 10598 Collaborators Al Wagner Pete Longo Daeyoung

More information

Ecole Franco-Roumaine : Magnétisme des systèmes nanoscopiques et structures hybrides - Brasov, Modern Analytical Microscopic Tools

Ecole Franco-Roumaine : Magnétisme des systèmes nanoscopiques et structures hybrides - Brasov, Modern Analytical Microscopic Tools 1. Introduction Solid Surfaces Analysis Group, Institute of Physics, Chemnitz University of Technology, Germany 2. Limitations of Conventional Optical Microscopy 3. Electron Microscopies Transmission Electron

More information

Multiphoton Imaging and Spectroscopy in Cell and Tissue Biophysics. J Moger and C P Winlove

Multiphoton Imaging and Spectroscopy in Cell and Tissue Biophysics. J Moger and C P Winlove Multiphoton Imaging and Spectroscopy in Cell and Tissue Biophysics J Moger and C P Winlove Relating Structure to Function Biochemistry Raman microspectrometry Surface enhanced Raman spectrometry (SERS)

More information

Time resolved optical spectroscopy methods for organic photovoltaics. Enrico Da Como. Department of Physics, University of Bath

Time resolved optical spectroscopy methods for organic photovoltaics. Enrico Da Como. Department of Physics, University of Bath Time resolved optical spectroscopy methods for organic photovoltaics Enrico Da Como Department of Physics, University of Bath Outline Introduction Why do we need time resolved spectroscopy in OPV? Short

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION SUPPLEMENTARY INFORMATION Electroluminescence from a single nanotube-molecule-nanotube junction Christoph W. Marquardt, Sergio Grunder, Alfred Błaszczyk, Simone Dehm, Frank Hennrich, Hilbert v. Löhneysen,

More information

Infrastructure of Thin Films Laboratory in Institute of Molecular Physics Polish Academy of Sciences

Infrastructure of Thin Films Laboratory in Institute of Molecular Physics Polish Academy of Sciences Infrastructure of Thin Films Laboratory in Institute of Molecular Physics Polish Academy of Sciences Outline Sample preparation Magnetron sputtering Ion-beam sputtering Pulsed laser deposition Electron-beam

More information

Ultrafast nanoscience with ELI ALPS

Ultrafast nanoscience with ELI ALPS Ultrafast nanoscience with ELI ALPS Péter Dombi Wigner Research Centre for Physics, Budapest & Max Planck Institute of Quantum Optics, Garching Overview ultrafast (femtosecond/attosecond) dynamicsin metal

More information

Molecule-mediated electron transport is one of the most

Molecule-mediated electron transport is one of the most Tunneling rates in electron transport through double-barrier molecular junctions in a scanning tunneling microscope G. V. Nazin, S. W. Wu, and W. Ho* Departments of Physics & Astronomy and Chemistry, University

More information

2) Atom manipulation. Xe / Ni(110) Model: Experiment:

2) 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 information

Advanced Spectroscopies of Modern Quantum Materials

Advanced Spectroscopies of Modern Quantum Materials Advanced Spectroscopies of Modern Quantum Materials The part about Advanced spectroscopies Some course goals: Better understand the link between experiment and the microscopic world of quantum materials.

More information

From manipulation of the charge state to imaging of individual molecular orbitals and bond formation

From manipulation of the charge state to imaging of individual molecular orbitals and bond formation Scanning Probe Microscopy of Adsorbates on Insulating Films: From manipulation of the charge state to imaging of individual molecular orbitals and bond formation Gerhard Meyer, Jascha Repp, Peter Liljeroth

More information

X-ray Photoelectron Spectroscopy (XPS)

X-ray Photoelectron Spectroscopy (XPS) X-ray Photoelectron Spectroscopy (XPS) As part of the course Characterization of Catalysts and Surfaces Prof. Dr. Markus Ammann Paul Scherrer Institut markus.ammann@psi.ch Resource for further reading:

More information

Chapter 103 Spin-Polarized Scanning Tunneling Microscopy

Chapter 103 Spin-Polarized Scanning Tunneling Microscopy Chapter 103 Spin-Polarized Scanning Tunneling Microscopy Toyo Kazu Yamada Keywords Spin-polarized tunneling current Spin polarization Magnetism 103.1 Principle Spin-polarized scanning tunneling microscopy

More information

Probing Molecular Electronics with Scanning Probe Microscopy

Probing Molecular Electronics with Scanning Probe Microscopy Probing Molecular Electronics with Scanning Probe Microscopy Mark C. Hersam Assistant Professor Department of Materials Science and Engineering, Northwestern University, Evanston, IL 60208-3108 Ph: 847-491-2696,

More information

INTRODUCTION TO SCA\ \I\G TUNNELING MICROSCOPY

INTRODUCTION TO SCA\ \I\G TUNNELING MICROSCOPY INTRODUCTION TO SCA\ \I\G TUNNELING MICROSCOPY SECOND EDITION C. JULIAN CHEN Department of Applied Physics and Applied Mathematics, Columbia University, New York OXFORD UNIVERSITY PRESS Contents Preface

More information

Advanced Lab Course. X-Ray Photoelectron Spectroscopy 1 INTRODUCTION 1 2 BASICS 1 3 EXPERIMENT Qualitative analysis Chemical Shifts 7

Advanced Lab Course. X-Ray Photoelectron Spectroscopy 1 INTRODUCTION 1 2 BASICS 1 3 EXPERIMENT Qualitative analysis Chemical Shifts 7 Advanced Lab Course X-Ray Photoelectron Spectroscopy M210 As of: 2015-04-01 Aim: Chemical analysis of surfaces. Content 1 INTRODUCTION 1 2 BASICS 1 3 EXPERIMENT 3 3.1 Qualitative analysis 6 3.2 Chemical

More information

Femtosecond laser microfabrication in. Prof. Dr. Cleber R. Mendonca

Femtosecond laser microfabrication in. Prof. Dr. Cleber R. Mendonca Femtosecond laser microfabrication in polymers Prof. Dr. Cleber R. Mendonca laser microfabrication focus laser beam on material s surface laser microfabrication laser microfabrication laser microfabrication

More information

Vibrational Spectroscopies. C-874 University of Delaware

Vibrational Spectroscopies. C-874 University of Delaware Vibrational Spectroscopies C-874 University of Delaware Vibrational Spectroscopies..everything that living things do can be understood in terms of the jigglings and wigglings of atoms.. R. P. Feymann Vibrational

More information

Scanning Tunneling Microscopy and its Application

Scanning Tunneling Microscopy and its Application Chunli Bai Scanning Tunneling Microscopy and its Application With 181 Figures SHANGHAI SCIENTIFIC & TECHNICAL PUBLISHERS Jpl Springer Contents 1. Introduction 1 1.1 Advantages of STM Compared with Other

More information

Multi-cycle THz pulse generation in poled lithium niobate crystals

Multi-cycle THz pulse generation in poled lithium niobate crystals Laser Focus World April 2005 issue (pp. 67-72). Multi-cycle THz pulse generation in poled lithium niobate crystals Yun-Shik Lee and Theodore B. Norris Yun-Shik Lee is an assistant professor of physics

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION doi:1.138/nature1878 I. Experimental setup OPA, DFG Ti:Sa Oscillator, Amplifier PD U DC U Analyzer HV Energy analyzer MCP PS CCD Polarizer UHV Figure S1: Experimental setup used in mid infrared photoemission

More information

MODERN TECHNIQUES OF SURFACE SCIENCE

MODERN TECHNIQUES OF SURFACE SCIENCE MODERN TECHNIQUES OF SURFACE SCIENCE Second edition D. P. WOODRUFF & T. A. DELCHAR Department ofphysics, University of Warwick CAMBRIDGE UNIVERSITY PRESS Contents Preface to first edition Preface to second

More information

X-Ray Photoelectron Spectroscopy (XPS) Auger Electron Spectroscopy (AES)

X-Ray Photoelectron Spectroscopy (XPS) Auger Electron Spectroscopy (AES) X-Ray Photoelectron Spectroscopy (XPS) Auger Electron Spectroscopy (AES) XPS X-ray photoelectron spectroscopy (XPS) is one of the most used techniques to chemically characterize the surface. Also known

More information

Ma5: Auger- and Electron Energy Loss Spectroscopy

Ma5: Auger- and Electron Energy Loss Spectroscopy Ma5: Auger- and Electron Energy Loss Spectroscopy 1 Introduction Electron spectroscopies, namely Auger electron- and electron energy loss spectroscopy are utilized to determine the KLL spectrum and the

More information

Two-photon Induced Hot Electron Transfer to a Single. Molecule in a Scanning Tunneling Microscope

Two-photon Induced Hot Electron Transfer to a Single. Molecule in a Scanning Tunneling Microscope Two-photon Induced Hot Electron Transfer to a Single Molecule in a Scanning Tunneling Microscope S.W. Wu * and W. Ho Department of Physics and Astronomy and Department of Chemistry, University of California,

More information

Site- 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 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 information

Surface Characte i r i zat on LEED Photoemission Phot Linear optics

Surface 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 information

Lecture 3: Light absorbance

Lecture 3: Light absorbance Lecture 3: Light absorbance Perturbation Response 1 Light in Chemistry Light Response 0-3 Absorbance spectrum of benzene 2 Absorption Visible Light in Chemistry S 2 S 1 Fluorescence http://www.microscopyu.com

More information

Recent Status of Polarized Electron Sources at Nagoya University

Recent Status of Polarized Electron Sources at Nagoya University Recent Status of Polarized Electron Sources at Nagoya University M. Kuwahara, N. Yamamoto, F. Furuta, T. Nakanishi, S. Okumi, M. Yamamoto, M. Kuriki *, T. Ujihara ** and K. Takeda ** Graduate School of

More information

Spectroscopy at nanometer scale

Spectroscopy 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 information

Solid Surfaces, Interfaces and Thin Films

Solid Surfaces, Interfaces and Thin Films Hans Lüth Solid Surfaces, Interfaces and Thin Films Fifth Edition With 427 Figures.2e Springer Contents 1 Surface and Interface Physics: Its Definition and Importance... 1 Panel I: Ultrahigh Vacuum (UHV)

More information

Contents. G. Hoffmann et al./ Tunnelling induced fluorescence as a probe of electromagnetic interaction at nanometre proximity 2

Contents. G. Hoffmann et al./ Tunnelling induced fluorescence as a probe of electromagnetic interaction at nanometre proximity 2 Contents G. Hoffmann et al./ Tunnelling induced fluorescence as a probe of electromagnetic interaction at nanometre proximity 2 TUNNELLING INDUCED FLUORESCENCE AS A PROBE OF ELECTROMAGNETIC INTERACTION

More information

Harmonic Generation for Photoionization Experiments Christian J. Kornelis Physics REU Kansas State University

Harmonic Generation for Photoionization Experiments Christian J. Kornelis Physics REU Kansas State University Harmonic Generation for Photoionization Experiments Christian J. Kornelis Physics REU Kansas State University The Basic Setup for the KLS Photoionization Experiment V. Kumarappan Femtosecond Pump-Probe

More information

Spatially resolving density-dependent screening around a single charged atom in graphene

Spatially resolving density-dependent screening around a single charged atom in graphene Supplementary Information for Spatially resolving density-dependent screening around a single charged atom in graphene Dillon Wong, Fabiano Corsetti, Yang Wang, Victor W. Brar, Hsin-Zon Tsai, Qiong Wu,

More information

Quantum Condensed Matter Physics Lecture 12

Quantum Condensed Matter Physics Lecture 12 Quantum Condensed Matter Physics Lecture 12 David Ritchie QCMP Lent/Easter 2016 http://www.sp.phy.cam.ac.uk/drp2/home 12.1 QCMP Course Contents 1. Classical models for electrons in solids 2. Sommerfeld

More information

Scanning tunneling microscopy of monoatomic gold chains on vicinal Si(335) surface: experimental and theoretical study

Scanning tunneling microscopy of monoatomic gold chains on vicinal Si(335) surface: experimental and theoretical study phys. stat. sol. (b) 4, No., 33 336 (005) / DOI 10.100/pssb.00460056 Scanning tunneling microscopy of monoatomic gold chains on vicinal Si(335) surface: experimental and theoretical study M. Krawiec *,

More information

= 6 (1/ nm) So what is probability of finding electron tunneled into a barrier 3 ev high?

= 6 (1/ nm) So what is probability of finding electron tunneled into a barrier 3 ev high? STM STM With a scanning tunneling microscope, images of surfaces with atomic resolution can be readily obtained. An STM uses quantum tunneling of electrons to map the density of electrons on the surface

More information

Quantum wells and Dots on surfaces

Quantum 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 information

STM: Scanning Tunneling Microscope

STM: Scanning Tunneling Microscope STM: Scanning Tunneling Microscope Basic idea STM working principle Schematic representation of the sample-tip tunnel barrier Assume tip and sample described by two infinite plate electrodes Φ t +Φ s =

More information

Studies of the Spin Dynamics of Charge Carriers in Semiconductors and their Interfaces. S. K. Singh, T. V. Shahbazyan, I. E. Perakis and N. H.

Studies of the Spin Dynamics of Charge Carriers in Semiconductors and their Interfaces. S. K. Singh, T. V. Shahbazyan, I. E. Perakis and N. H. Studies of the Spin Dynamics of Charge Carriers in Semiconductors and their Interfaces S. K. Singh, T. V. Shahbazyan, I. E. Perakis and N. H. Tolk Department of Physics and Astronomy Vanderbilt University,

More information

Surface Analysis - The Principal Techniques

Surface Analysis - The Principal Techniques Surface Analysis - The Principal Techniques 2nd Edition Editors johnc.vickerman Manchester Interdisciplinary Biocentre, University of Manchester, UK IAN S. GILMORE National Physical Laboratory, Teddington,

More information

Visualization of Xe and Sn Atoms Generated from Laser-Produced Plasma for EUV Light Source

Visualization of Xe and Sn Atoms Generated from Laser-Produced Plasma for EUV Light Source 3rd International EUVL Symposium NOVEMBER 1-4, 2004 Miyazaki, Japan Visualization of Xe and Sn Atoms Generated from Laser-Produced Plasma for EUV Light Source H. Tanaka, A. Matsumoto, K. Akinaga, A. Takahashi

More information

Lecture 12. Electron Transport in Molecular Wires Possible Mechanisms

Lecture 12. Electron Transport in Molecular Wires Possible Mechanisms Lecture 12. Electron Transport in Molecular Wires Possible Mechanisms In Lecture 11, we have discussed energy diagrams of one-dimensional molecular wires. Here we will focus on electron transport mechanisms

More information

Optical Spectroscopy of Advanced Materials

Optical Spectroscopy of Advanced Materials Phys 590B Condensed Matter Physics: Experimental Methods Optical Spectroscopy of Advanced Materials Basic optics, nonlinear and ultrafast optics Jigang Wang Department of Physics, Iowa State University

More information

Characterisation of vibrational modes of adsorbed species

Characterisation of vibrational modes of adsorbed species 17.7.5 Characterisation of vibrational modes of adsorbed species Infrared spectroscopy (IR) See Ch.10. Infrared vibrational spectra originate in transitions between discrete vibrational energy levels of

More information

Natallia Strekal. Plasmonic films of noble metals for nanophotonics

Natallia Strekal. Plasmonic films of noble metals for nanophotonics Natallia Strekal Plasmonic films of noble metals for nanophotonics The aim of our investigation is the mechanisms of light interactions with nanostructure and High Tech application in the field of nanophotonics

More information

Protection of excited spin states by a superconducting energy gap

Protection 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 information

Set-up for ultrafast time-resolved x-ray diffraction using a femtosecond laser-plasma kev x-ray-source

Set-up for ultrafast time-resolved x-ray diffraction using a femtosecond laser-plasma kev x-ray-source Set-up for ultrafast time-resolved x-ray diffraction using a femtosecond laser-plasma kev x-ray-source C. Blome, K. Sokolowski-Tinten *, C. Dietrich, A. Tarasevitch, D. von der Linde Inst. for Laser- and

More information

Scanning Tunneling Microscopy

Scanning Tunneling Microscopy Scanning Tunneling Microscopy References: 1. G. Binnig, H. Rohrer, C. Gerber, and Weibel, Phys. Rev. Lett. 49, 57 (1982); and ibid 50, 120 (1983). 2. J. Chen, Introduction to Scanning Tunneling Microscopy,

More information

IV. Surface analysis for chemical state, chemical composition

IV. Surface analysis for chemical state, chemical composition IV. Surface analysis for chemical state, chemical composition Probe beam Detect XPS Photon (X-ray) Photoelectron(core level electron) UPS Photon (UV) Photoelectron(valence level electron) AES electron

More information

Photoelectron Spectroscopy using High Order Harmonic Generation

Photoelectron Spectroscopy using High Order Harmonic Generation Photoelectron Spectroscopy using High Order Harmonic Generation Alana Ogata Yamanouchi Lab, University of Tokyo ABSTRACT The analysis of photochemical processes has been previously limited by the short

More information

Surface Analysis - The Principal Techniques

Surface Analysis - The Principal Techniques Surface Analysis - The Principal Techniques Edited by John C. Vickerman Surface Analysis Research Centre, Department of Chemistry UMIST, Manchester, UK JOHN WILEY & SONS Chichester New York Weinheim Brisbane

More information

Curriculum Vitae- Jay Anil Gupta. Education PhD, Physics, University of California, Santa Barbara

Curriculum Vitae- Jay Anil Gupta. Education PhD, Physics, University of California, Santa Barbara Curriculum Vitae- Jay Anil Gupta Ohio State University Department of Physics 191 W. Woodruff Ave Columbus, OH 43210 Phone: (614) 247-8457 Fax: (614) 292-7557 Email: jgupta@mps.ohio-state.edu Education

More information

Supporting Information s for

Supporting Information s for Supporting Information s for # Self-assembling of DNA-templated Au Nanoparticles into Nanowires and their enhanced SERS and Catalytic Applications Subrata Kundu* and M. Jayachandran Electrochemical Materials

More information

MSE 321 Structural Characterization

MSE 321 Structural Characterization Auger Spectroscopy Auger Electron Spectroscopy (AES) Scanning Auger Microscopy (SAM) Incident Electron Ejected Electron Auger Electron Initial State Intermediate State Final State Physical Electronics

More information

Chapter 5 Nanomanipulation. Chapter 5 Nanomanipulation. 5.1: With a nanotube. Cutting a nanotube. Moving a nanotube

Chapter 5 Nanomanipulation. Chapter 5 Nanomanipulation. 5.1: With a nanotube. Cutting a nanotube. Moving a nanotube Objective: learn about nano-manipulation techniques with a STM or an AFM. 5.1: With a nanotube Moving a nanotube Cutting a nanotube Images at large distance At small distance : push the NT Voltage pulse

More information

Core Level Spectroscopies

Core Level Spectroscopies Core Level Spectroscopies Spectroscopies involving core levels are element-sensitive, and that makes them very useful for understanding chemical bonding, as well as for the study of complex materials.

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION DOI: 10.1038/NCHEM.1488 Submolecular control, spectroscopy and imaging of bond-selective chemistry in single functionalized molecules Ying Jiang 1,2*, Qing Huan 1,3*, Laura Fabris 4, Guillermo C. Bazan

More information

OPTICAL PROPERTIES AND SPECTROSCOPY OF NANOAAATERIALS. Jin Zhong Zhang. World Scientific TECHNISCHE INFORMATIONSBIBLIOTHEK

OPTICAL PROPERTIES AND SPECTROSCOPY OF NANOAAATERIALS. Jin Zhong Zhang. World Scientific TECHNISCHE INFORMATIONSBIBLIOTHEK OPTICAL PROPERTIES AND SPECTROSCOPY OF NANOAAATERIALS Jin Zhong Zhang University of California, Santa Cruz, USA TECHNISCHE INFORMATIONSBIBLIOTHEK Y World Scientific NEW JERSEY. t'on.don SINGAPORE «'BEIJING

More information

THE ELECTROLUMINESCENCE AND SCANNING TUNNELING MICROSCOPY OF SINGLE MOLECULES

THE ELECTROLUMINESCENCE AND SCANNING TUNNELING MICROSCOPY OF SINGLE MOLECULES THE ELECTROLUMINESCENCE AND SCANNING TUNNELING MICROSCOPY OF SINGLE MOLECULES by John William Buker M. Sc, Simon Fraser University 2003 THESIS SUBMITTED IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE

More information

Lecture 5. X-ray Photoemission Spectroscopy (XPS)

Lecture 5. X-ray Photoemission Spectroscopy (XPS) Lecture 5 X-ray Photoemission Spectroscopy (XPS) 5. Photoemission Spectroscopy (XPS) 5. Principles 5.2 Interpretation 5.3 Instrumentation 5.4 XPS vs UV Photoelectron Spectroscopy (UPS) 5.5 Auger Electron

More information

Spectroscopies for Unoccupied States = Electrons

Spectroscopies 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 information

Ultrafast Dynamics and Single Particle Spectroscopy of Au-CdSe Nanorods

Ultrafast Dynamics and Single Particle Spectroscopy of Au-CdSe Nanorods Supporting Information Ultrafast Dynamics and Single Particle Spectroscopy of Au-CdSe Nanorods G. Sagarzazu a, K. Inoue b, M. Saruyama b, M. Sakamoto b, T. Teranishi b, S. Masuo a and N. Tamai a a Department

More information

Carbon Nanomaterials

Carbon Nanomaterials Carbon Nanomaterials STM Image 7 nm AFM Image Fullerenes C 60 was established by mass spectrographic analysis by Kroto and Smalley in 1985 C 60 is called a buckminsterfullerene or buckyball due to resemblance

More information

The photoelectric effect

The photoelectric effect The photoelectric effect E K hν-e B E F hν E B A photoemission experiment Lifetime broadening ΔE.Δτ~ħ ΔE~ħ/Δτ + Experimental resolution Hüfner, Photoelectron Spectroscopy (Springer) A photoemission experiment

More information

Free-electron laser SACLA and its basic. Yuji Otake, on behalf of the members of XFEL R&D division RIKEN SPring-8 Center

Free-electron laser SACLA and its basic. Yuji Otake, on behalf of the members of XFEL R&D division RIKEN SPring-8 Center Free-electron laser SACLA and its basic Yuji Otake, on behalf of the members of XFEL R&D division RIKEN SPring-8 Center Light and Its Wavelength, Sizes of Material Virus Mosquito Protein Bacteria Atom

More information

Photon Interaction. Spectroscopy

Photon 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 information

Detection of Single Photon Emission by Hanbury-Brown Twiss Interferometry

Detection of Single Photon Emission by Hanbury-Brown Twiss Interferometry Detection of Single Photon Emission by Hanbury-Brown Twiss Interferometry Greg Howland and Steven Bloch May 11, 009 Abstract We prepare a solution of nano-diamond particles on a glass microscope slide

More information

Ultrafast dynamics in multiferroics HoMnO 3 revealed by fs spectroscopy. Chih Wei Luo ( 羅志偉 )

Ultrafast dynamics in multiferroics HoMnO 3 revealed by fs spectroscopy. Chih Wei Luo ( 羅志偉 ) Ultrafast dynamics in multiferroics HoMnO 3 revealed by fs spectroscopy Chih Wei Luo ( 羅志偉 ) Outline Introduction of femtosecond (fs) laser pulses Ultrafast dynamics in multiferroics HoMnO 3 Summary I

More information

Vibrational Spectroscopy of Molecules on Surfaces

Vibrational Spectroscopy of Molecules on Surfaces Vibrational Spectroscopy of Molecules on Surfaces Edited by John T. Yates, Jr. University of Pittsburgh Pittsburgh, Pennsylvania and Theodore E. Madey National Bureau of Standards Gaithersburg, Maryland

More information

Doctor of Philosophy

Doctor of Philosophy FEMTOSECOND TIME-DOMAIN SPECTROSCOPY AND NONLINEAR OPTICAL PROPERTIES OF IRON-PNICTIDE SUPERCONDUCTORS AND NANOSYSTEMS A Thesis Submitted for the degree of Doctor of Philosophy IN THE FACULTY OF SCIENCE

More information

Strong Field Quantum Control. CAMOS Spring Meeting 2012 o

Strong Field Quantum Control. CAMOS Spring Meeting 2012 o Strong Field Quantum Control CAMOS Spring Meeting 2012 o p Motivation & Outline Motivation: Want to control molecular dynamics and develop control based spectroscopy 1. Controlling Molecular Dissociation

More information

Time-Resolved and Momentum-Resolved Resonant Soft X-ray Scattering on Strongly Correlated Systems

Time-Resolved and Momentum-Resolved Resonant Soft X-ray Scattering on Strongly Correlated Systems Time-Resolved and Momentum-Resolved Resonant Soft X-ray Scattering on Strongly Correlated Systems Wei-Sheng Lee Stanford Institute of Material and Energy Science (SIMES) SLAC & Stanford University Collaborators

More information

Chem 681: Student Seminar Series. Two-Photon Induced Fluorescence

Chem 681: Student Seminar Series. Two-Photon Induced Fluorescence Speaker: Brooke Kocsis Date: Monday, April 17, 2000 Time: 4:00 PM Room: 2121 Advisor: Richard M. Crooks Chem 681: Student Seminar Series Two-Photon Induced Fluorescence Two-photon fluorescence (TPF) is

More information

ENERGY DISTRIBUTION OF PHOTO-STIMULATED ELECTRON EMISSION FROM FATIGUE SPECIMENS. Thousand Oaks, California

ENERGY DISTRIBUTION OF PHOTO-STIMULATED ELECTRON EMISSION FROM FATIGUE SPECIMENS. Thousand Oaks, California ENERGY DISTRIBUTION OF PHOTO-STIMULATED ELECTRON EMISSION FROM FATIGUE SPECIMENS Fredrick J. Szalkowski Science Cente11, Rockwell International Thousand Oaks, California I would like to thank Larry Himmel

More information

Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown and Twiss Photon Antibunching Setup

Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown and Twiss Photon Antibunching Setup 1 Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown and Twiss Photon Antibunching Setup Abstract Jacob Begis The purpose of this lab was to prove that a source of light can be

More information

Because light behaves like a wave, we can describe it in one of two ways by its wavelength or by its frequency.

Because light behaves like a wave, we can describe it in one of two ways by its wavelength or by its frequency. Light We can use different terms to describe light: Color Wavelength Frequency Light is composed of electromagnetic waves that travel through some medium. The properties of the medium determine how light

More information

Wavelength λ Velocity v. Electric Field Strength Amplitude A. Time t or Distance x time for 1 λ to pass fixed point. # of λ passing per s ν= 1 p

Wavelength λ Velocity v. Electric Field Strength Amplitude A. Time t or Distance x time for 1 λ to pass fixed point. # of λ passing per s ν= 1 p Introduction to Spectroscopy (Chapter 6) Electromagnetic radiation (wave) description: Wavelength λ Velocity v Electric Field Strength 0 Amplitude A Time t or Distance x Period p Frequency ν time for 1

More information

Part II. X-ray Absorption Spectroscopy (XAS)

Part II. X-ray Absorption Spectroscopy (XAS) Part II XAFS: Principles XANES/NEXAFS Applications 1 X-ray Absorption Spectroscopy (XAS) X-ray Absorption spectroscopy is often referred to as - NEXAFS for low Z elements (C, N, O, F, etc. K-edge, Si,

More information

Skoog Chapter 6 Introduction to Spectrometric Methods

Skoog Chapter 6 Introduction to Spectrometric Methods Skoog Chapter 6 Introduction to Spectrometric Methods General Properties of Electromagnetic Radiation (EM) Wave Properties of EM Quantum Mechanical Properties of EM Quantitative Aspects of Spectrochemical

More information

SCANNING-PROBE TECHNIQUES OR APPARATUS; APPLICATIONS OF SCANNING-PROBE TECHNIQUES, e.g. SCANNING PROBE MICROSCOPY [SPM]

SCANNING-PROBE TECHNIQUES OR APPARATUS; APPLICATIONS OF SCANNING-PROBE TECHNIQUES, e.g. SCANNING PROBE MICROSCOPY [SPM] G01Q SCANNING-PROBE TECHNIQUES OR APPARATUS; APPLICATIONS OF SCANNING-PROBE TECHNIQUES, e.g. SCANNING PROBE MICROSCOPY [SPM] Scanning probes, i.e. devices having at least a tip of nanometre sized dimensions

More information

Time Resolved (Pump Probe) Experiment to watch structural dynamics by using the pulsed nature of synchrotron radiation

Time Resolved (Pump Probe) Experiment to watch structural dynamics by using the pulsed nature of synchrotron radiation SESAME-JSPS School November 14-16, 2011 Amman, Jordan Time Resolved (Pump Probe) Experiment to watch structural dynamics by using the pulsed nature of synchrotron radiation Shin-ichi Adachi (Photon Factory,

More information

MOLECULAR SPECTROSCOPY AND PHOTOCHEMISTRY

MOLECULAR SPECTROSCOPY AND PHOTOCHEMISTRY 20 CHAPTER MOLECULAR SPECTROSCOPY AND PHOTOCHEMISTRY 20.1 Introduction to Molecular Spectroscopy 20.2 Experimental Methods in Molecular Spectroscopy 20.3 Rotational and Vibrational Spectroscopy 20.4 Nuclear

More information

Supplementary Information for. Vibrational Spectroscopy at Electrolyte Electrode Interfaces with Graphene Gratings

Supplementary Information for. Vibrational Spectroscopy at Electrolyte Electrode Interfaces with Graphene Gratings Supplementary Information for Vibrational Spectroscopy at Electrolyte Electrode Interfaces with Graphene Gratings Supplementary Figure 1. Simulated from pristine graphene gratings at different Fermi energy

More information

Real-space investigation of energy transfer with Single-molecule luminescence and Absorption Spectroscopy

Real-space investigation of energy transfer with Single-molecule luminescence and Absorption Spectroscopy AuGuSt 2018 vol. 28 no. 4 feature articles DOI: 10.22661/AAPPSBL.2018.28.4.03 Real-space investigation of energy transfer with Single-molecule luminescence and Absorption Spectroscopy HIROSHI IMADA AND

More information

Electron temperature is the temperature that describes, through Maxwell's law, the kinetic energy distribution of the free electrons.

Electron temperature is the temperature that describes, through Maxwell's law, the kinetic energy distribution of the free electrons. 10.3.1.1 Excitation and radiation of spectra 10.3.1.1.1 Plasmas A plasma of the type occurring in spectrochemical radiation sources may be described as a gas which is at least partly ionized and contains

More information

Femtosecond laser applied to biophotonics. Prof. Cleber R. Mendonca

Femtosecond laser applied to biophotonics. Prof. Cleber R. Mendonca Femtosecond laser applied to biophotonics Prof. Cleber R. Mendonca introduction short pulse duration ö high intensity (even at low energy) introduction how short is a femtosecond pulse? 1fs= 10-15 s introduction

More information

Experimental methods in physics. Local probe microscopies I

Experimental methods in physics. Local probe microscopies I Experimental methods in physics Local probe microscopies I Scanning tunnelling microscopy (STM) Jean-Marc Bonard Academic year 09-10 1. Scanning Tunneling Microscopy 1.1. Introduction Image of surface

More information

5.33 Lecture Notes: Introduction to Spectroscopy

5.33 Lecture Notes: Introduction to Spectroscopy 5.33 Lecture Notes: ntroduction to Spectroscopy What is spectroscopy? Studying the properties of matter through its interaction with different frequency components of the electromagnetic spectrum. Latin:

More information