Analytical Electron Microscopy
|
|
- Patience McGee
- 5 years ago
- Views:
Transcription
1 Analytical Electron Microscopy Walid Hetaba Fritz-Haber-Institut der MPG MPI für Chemische Energiekonversion W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
2 1 Introduction 2 EDX 3 EELS 4 Conclusion W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
3 Introduction Analytical Electron Microscopy Imaging Diffraction Spectrometry Williams, Carter: Transmission Electron Microscopy - A Textbook for Materials Science, Springer 2009 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
4 Introduction Mode of Operation Williams, Carter: Transmission Electron Microscopy - A Textbook for Materials Science, Springer 2009 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
5 EDX Introduction to EDX Williams, Carter: Transmission Electron Microscopy - A Textbook for Materials Science, Springer 2009 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
6 EDX Introduction to EDX Williams, Carter: Transmission Electron Microscopy - A Textbook for Materials Science, Springer 2009 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
7 EDX Fluorescence Yield Williams, Carter: Transmission Electron Microscopy - A Textbook for Materials Science, Springer 2009 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
8 Detectors EDX-Setup Detector area, collection angle SuperX (ChemiSTEM): 4 detectors Williams, Carter: Transmission Electron Microscopy - A Textbook for Materials Science, Springer 2009 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
9 Detectors EDX Detectors Dead Time Live Time Clock Time Williams, Carter: Transmission Electron Microscopy - A Textbook for Materials Science, Springer 2009 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
10 Detectors EDX Signal Williams, Carter: Transmission Electron Microscopy - A Textbook for Materials Science, Springer 2009 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
11 Qualitative Analysis EDX-Spectra Cu from System Be for low background sample holder W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
12 Qualitative Analysis EDX-Spectra W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
13 Qualitative Analysis EDX-Spectra W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
14 Qualitative Analysis EDX-Maps W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
15 Qualitative Analysis EDX-Maps W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
16 Quantitative Analysis Cliff-Lorimer Ratio Technique C A /C B = k AB I A /I B k AB... Cliff-Lorimer factor C A + C B = 1 For thin specimen, absorption can be neglected k AB either measured using standards or calculated W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
17 Quantitative Analysis ζ-factor Method ρt = ζ A I A /C A C A /C B = (I A ζ A )/(I B ζ B ) ζ-factors either measured using standards or calculated For both techniques absorption correction (ZAF) possible W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
18 Electron Energy Loss Spectrometry EELS Williams, Carter: Transmission Electron Microscopy - A Textbook for Materials Science, Springer 2009 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
19 Electron Energy Loss Spectrometry EELS Williams, Carter: Transmission Electron Microscopy - A Textbook for Materials Science, Springer 2009 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
20 Electron Energy Loss Spectrometry Williams, Carter: Transmission Electron Microscopy - A Textbook for Materials Science, Springer 2009 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
21 Electron Energy Loss Spectrometry Hetaba: Fine Structure and Site Specific Energy Loss Spectra of NiO, Diploma Thesis, TU Wien 2011 Schaffer et al., Phys. Rev. B, 79, (R), 2009 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
22 Electron Energy Loss Spectrometry NiO TiO 2 Cond. A Cond. B Cond. C Intensity [arb. u.] Energy Loss [ev] states / ev O p x O p y O p z Exp E - E F [ev] Hetaba: Fine Structure and Site Specific Energy Loss Spectra of NiO, Diploma Thesis, TU Wien 2011 Hetaba: The Theory and Application of Inelastic Coherence in the Electron Microscope, PhD Thesis, TU Wien 2015 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
23 Classical Scattering Theory Elastic vs. inelastic scattering Differential scattering cross section dσ/dω to describe scattering Elastic Scattering Transfer of momentum Transfer of kinetic energy No change of internal energy of particle and target Inelastic Scattering Transfer of momentum Transfer of energy Internal energy of target changed W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
24 Elastic vs. Inelastic Scattering Schattschneider, Werner, Hébert: Lecture Notes Electron Beam Techniques for Nanoanalysis, TU Wien 2007 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
25 Elastic Scattering Classical scattering p 0 = p 1 + p 2 E 0 = p2 0 2m = p2 1 2m + p2 2 2M E = p2 2 2M = 4mM (M+m) 2 E 0 4 m M E 0, with m M Demtröder: Experimentalphysik 1, Springer 2013 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
26 Elastic Scattering Rutherford scattering dσ/dω = f (q) 2, f (q)... scattering factor f (q) proportional to FT [V (r)], V (r)... atomic potential Coulomb potential yields Rutherford cross section: dσ/dω = 4γZ 2 a 2 0 q4, q = 2k 0 sin(θ/2) W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
27 Elastic Scattering Egerton: Electron energy-loss spectroscopy in the electron microscope, Plenum Press 1996 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
28 Elastic Scattering Rutherford scattering dσ/dω = f (q) 2, f (q)... scattering factor f (q) proportional to FT [V (r)], V (r)... atomic potential Coulomb potential yields Rutherford cross section: dσ/dω = 4γZ 2 a 2 0 q4, q = 2k 0 sin(θ/2) Unscreended potential Overestimates elastic scattering at small θ (large b) W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
29 Elastic Scattering Yukawa potential Screened potential: V (r) = (Ze/4πɛ 0 r) exp(r/r 0 ) dσ dω = 4γ2 Z 2 1 a0 2k4 0 (θ 2 +θ0 2)2 Characteristic scattering angle: θ 0 = (k 0 r 0 ) 1 Screening radius: r 0 = a 0 Z 1/3 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
30 Elastic Scattering Schattschneider, Werner, Hébert: Lecture Notes Electron Beam Techniques for Nanoanalysis, TU Wien 2007 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
31 Elastic Scattering Diffraction and channelling effects Bragg scattering in crystals Modifies scattering cross section Channelling effects: redistribution of electron flux inside crystal Elastic scattering changes probabilites for inelastic scattering W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
32 Elastic Scattering Schattschneider, Werner, Hébert: Lecture Notes Electron Beam Techniques for Nanoanalysis, TU Wien 2007 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
33 Elastic Scattering Diffraction and channelling effects Bragg scattering in crystals Modifies scattering cross section Channelling effects: redistribution of electron flux inside crystal Elastic scattering changes probabilites for inelastic scattering W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
34 Inelastic Scattering Inelastic differential scattering cross section { } dσ i dω = 4γ2 Z 1 1 a0 2q4 [1+(qr 0 ) 2 ] 2 q 2 = k 2 0 (θ2 + θ 2 E ) θ E = E/(γm 0 v 2 ), characteristic inelastic scattering angle θ 0 = (k 0 r 0 ) 1 θ E < θ < θ 0 : dσ/dω θ 2 θ > θ 0 : dσ/dω θ 4 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
35 Inelastic Scattering Egerton: Electron energy-loss spectroscopy in the electron microscope, Plenum Press 1996 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
36 Quantum Mechanical Description Double differential scattering cross section W i f = 2π Ψ f ˆV Ψ i 2 dv f δ ( ) E Ψf E Ψi dj = dσ(e, Ω) j i 2 σ E Ω = ( ) 2π 4 m 2 k f k i i p i f ψ f f ˆV i ψ i 2 δ ( E f E i E ) W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
37 Models for the DDSCS Single plane wave ψ i,f (r) = 1 (2π) 3/2 exp[ik i,f r] 2 σ E Ω = 4γ2 k f 1 a0 2 k i Q i p 4 i f j f e iq R j i 2 δ ( E f E i E ) Dynamic Form Factor (DFF): S(Q, E) = i p i f e iq R j f j 2 σ E Ω = 4γ2 k f 1 a0 2 k i S(Q, E) Q 4 i 2 δ ( E f E i E ) W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
38 Models for the DDSCS Superposition of plane waves ψ i = a 1 k 1 + a 2 k 2, a a 2 2 = 1 2 σ E Ω = 4γ2 a0 2 [ k f k i a S(Q, E) + a Q ] ] [ +2R a 1 a2 1 S(Q, Q 2 Q 2 Q, E) Q 4 S(Q, E)+ Mixed Dynamic Form Factor (MDFF): S(Q, Q, E) = i f f eiq R i i e iq R f δ ( E f E i E ) W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
39 Models for the DDSCS k 0 θ θ' k' k G I A A R[A 1A 2 exp i(φ 1 φ 2 )] q q' 0 G A B C Demtröder: Experimentalphysik 1, Springer 2013 Hetaba: The Theory and Application of Inelastic Coherence in the Electron Microscope, PhD Thesis, TU Wien 2015 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
40 Models for the DDSCS Bloch waves 2 σ E Ω = 4γ2 k f a0 2 k i x j,j,l,l X jlj l (x) S g,g,h,h g hg h x (Q,Q,E) Q 2 Q 2 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
41 MDFF for Crystals MDFF for Crystals S(Q, Q, E) = i λ λ 4π(2l + 1) ν mm λλ µµ LMS L M S (2L + 1)(2L + 1)(2λ + 1)(2λ + 1) Y µ λ (Q/Q) j λ (Q) νnjls Y µ λ (Q /Q ) j λ (Q ) νnjl S ( ) ( L λ l L λ ) ( ) ( l L λ l L λ ) l M µ m M µ m ( ) ( ) l 1 ( 1) M+M (2j + 1) 2 j l 1 2 j m S j z m S j z j z (D ν LMS ) (D ν L M S )δ(e f E i E) Löffler: Study of real space wave functions with electron energy loss spectrometry, PhD Thesis, TU Wien 2013 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
42 WIEN2k Simulations Features of WIEN2k Density Functional Theory, Kohn-Sham equation Electronic properties of crystal Electron density Bandstructure DOS TELNES.3 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
43 Density Functional Theory Kohn-Sham equation Ĥ = 2 2 N i 1 4πɛ 0 2 Ri N i,j M i 2 2 N i 2 r i m e e 2 Z i R i r j + 1 8πɛ 0 N i j e 2 r i r j + 1 8πɛ 0 N i j e 2 Z i Z j R i R j Ĥ KS = ˆT + ˆV H + ˆV xc + ˆV ext = 2 2 i + e2 2m e 4πɛ 0 i ρ( r ) r r d r + ˆV xc + ˆV ext W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
44 Calculated Spectra NiO G20 GGA LDA+U B3PW91 PBE0 G20 mbjlda Intensity [a.u.] Intensity [a.u.] Energy Loss [ev] Energy Loss [ev] Hetaba: Fine Structure and Site Specific Energy Loss Spectra of NiO, Diploma Thesis, TU Wien 2011 Hetaba et al., Phys. Rev. B 85, , 2012 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
45 Applications Oxidation State W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
46 Applications Oxidation State W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
47 Applications Crystallographic Structure - Coordination Egerton: Electron energy-loss spectroscopy in the electron microscope, Plenum Press 1996 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
48 Applications EMCD Hetaba: The Theory and Application of Inelastic Coherence in the Electron Microscope, PhD Thesis, TU Wien 2015 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
49 Applications Channelling effects states / ev O p x O p y O p z TELNES E - E F [ev] Hetaba: The Theory and Application of Inelastic Coherence in the Electron Microscope, PhD Thesis, TU Wien 2015 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
50 Applications Channelling effects Hetaba: The Theory and Application of Inelastic Coherence in the Electron Microscope, PhD Thesis, TU Wien 2015 Hetaba et al., Micron 63, 15-19, 2014 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
51 Applications Channelling effects Intensity [arb. u.] Cond. A Cond. B Cond. C Energy Loss [ev] θ θ' k 0 k G k' 0 q q' G A B C Hetaba: The Theory and Application of Inelastic Coherence in the Electron Microscope, PhD Thesis, TU Wien 2015 Hetaba et al., Micron 63, 15-19, 2014 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
52 Applications Channelling effects Cond. A Cond. B Cond. C O p x O p y O p z Intensity [arb. u.] states / ev Energy Loss [ev] E - E F [ev] Hetaba: The Theory and Application of Inelastic Coherence in the Electron Microscope, PhD Thesis, TU Wien 2015 Hetaba et al., Micron 63, 15-19, 2014 W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
53 Conclusion EDX and EELS complimentary techniques Understanding of theory necessary for interpretation Lots of different properties accessible Analytical Electron Microscopy versatile tool W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
54 Literature Useful books (linked) Analytical electron microscopy in general: Williams, Carter: Transmission Electron Micrsocopy - A Textbook for Materials Science Everything about EELS: Theory: Egerton: Electron energy-loss spectroscopy in the electron microscope Schattschneider: Fundamentals of Inelastic Electron Scattering Schattschneider: Linear and Chiral Dichroism in the Electron Microscope W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
55 Literature Links to cited articles and EELS Databases Schaffer et al., Phys. Rev. B, 79, (R), 2009 Hetaba et al., Phys. Rev. B 85, , 2012 Hetaba et al., Micron 63, 15-19, 2014 Demtröder: Experimentalphysik 1, Springer 2013 PhD thesis Löffler PhD thesis Hetaba EELS Database: Gatan EELS.info, EELS-Atlas EELS Data Base W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
56 Acknowledgments M. Willinger R. Farra G. Algara-Siller R. Schlögl P. Schattschneider S. Löffler M. Stöger-Pollach A. Hütten W. Hetaba (FHI, MPI-CEC) Analytical Electron Microscopy / 23
Core loss spectra (EELS, XAS)
Core loss spectra (EELS, XAS) Kevin Jorissen University of Washington (USA) WIENk 013 Penn State 1. Concepts WIENk calculates ELNES / XANES EELS : Electron Energy Loss Spectroscopy XAS: X-ray Absorption
More informationQuantum Physics III (8.06) Spring 2008 Assignment 10
May 5, 2008 Quantum Physics III (8.06) Spring 2008 Assignment 10 You do not need to hand this pset in. The solutions will be provided after Friday May 9th. Your FINAL EXAM is MONDAY MAY 19, 1:30PM-4:30PM,
More informationKMÜ 396 MATERIALS SCIENCE AND TECH. I PRESENTATION ELECTRON ENERGY LOSS SPECTROSCOPY (EELS) TUĞÇE SEZGİN
KMÜ 396 MATERIALS SCIENCE AND TECH. I PRESENTATION ELECTRON ENERGY LOSS SPECTROSCOPY (EELS) TUĞÇE SEZGİN 20970725 HACETTEPE UNIVERSITY DEPARTMENT OF CHEMICAL ENGINEERING, SPRING 2011,APRIL,ANKARA CONTENTS
More informationChemical Analysis in TEM: XEDS, EELS and EFTEM. HRTEM PhD course Lecture 5
Chemical Analysis in TEM: XEDS, EELS and EFTEM HRTEM PhD course Lecture 5 1 Part IV Subject Chapter Prio x-ray spectrometry 32 1 Spectra and mapping 33 2 Qualitative XEDS 34 1 Quantitative XEDS 35.1-35.4
More informationDFT calculations of dichroic effect in transmission electron microscope
DFT calculations of dichroic effect in transmission electron microscope ChiralTEM project Ján Rusz, Pavel Novák Institute of Physics Academy of Sciences of Czech Republic DFTEM, ChiralTEM Workshop, Vienna,
More informationQuantum Physics III (8.06) Spring 2005 Assignment 9
Quantum Physics III (8.06) Spring 2005 Assignment 9 April 21, 2005 Due FRIDAY April 29, 2005 Readings Your reading assignment on scattering, which is the subject of this Problem Set and much of Problem
More informationPhysic 492 Lecture 16
Physic 492 Lecture 16 Main points of last lecture: Angular momentum dependence. Structure dependence. Nuclear reactions Q-values Kinematics for two body reactions. Main points of today s lecture: Measured
More informationThe Basic of Transmission Electron Microscope. Text book: Transmission electron microscopy by David B Williams & C. Barry Carter.
The Basic of Transmission Electron Microscope Text book: Transmission electron microscopy by David B Williams & C. Barry Carter. 2009, Springer Background survey http://presemo.aalto.fi/tem1 Microscopy
More informationElectron Microscopy I
Characterization of Catalysts and Surfaces Characterization Techniques in Heterogeneous Catalysis Electron Microscopy I Introduction Properties of electrons Electron-matter interactions and their applications
More informationParticle Interactions in Detectors
Particle Interactions in Detectors Dr Peter R Hobson C.Phys M.Inst.P. Department of Electronic and Computer Engineering Brunel University, Uxbridge Peter.Hobson@brunel.ac.uk http://www.brunel.ac.uk/~eestprh/
More informationX-ray absorption spectroscopy.
X-ray absorption spectroscopy www.anorg.chem.uu.nl/people/staff/frankdegroot/ X-ray absorption spectroscopy www.anorg.chem.uu.nl/people/staff/frankdegroot/ Frank de Groot PhD: solid state chemistry U Nijmegen
More informationModified Becke-Johnson (mbj) exchange potential
Modified Becke-Johnson (mbj) exchange potential Hideyuki Jippo Fujitsu Laboratories LTD. 2015.12.21-22 OpenMX developer s meeting @ Kobe Overview: mbj potential The semilocal exchange potential adding
More informationStructural characterization. Part 1
Structural characterization Part 1 Experimental methods X-ray diffraction Electron diffraction Neutron diffraction Light diffraction EXAFS-Extended X- ray absorption fine structure XANES-X-ray absorption
More informationMS482 Materials Characterization ( 재료분석 ) Lecture Note 5: RBS
2016 Fall Semester MS482 Materials Characterization ( 재료분석 ) Lecture Note 5: RBS Byungha Shin Dept. of MSE, KAIST 1 Course Information Syllabus 1. Overview of various characterization techniques (1 lecture)
More informationFundamentals of Nanoscale Film Analysis
Fundamentals of Nanoscale Film Analysis Terry L. Alford Arizona State University Tempe, AZ, USA Leonard C. Feldman Vanderbilt University Nashville, TN, USA James W. Mayer Arizona State University Tempe,
More informationRoger Johnson Structure and Dynamics: X-ray Diffraction Lecture 6
6.1. Summary In this Lecture we cover the theory of x-ray diffraction, which gives direct information about the atomic structure of crystals. In these experiments, the wavelength of the incident beam must
More informationarxiv: v1 [cond-mat.mtrl-sci] 17 Mar 2008
Pushing the detection limit of Magnetic Circular Dichroism to 2 nm Peter Schattschneider and Michael Stöger-Pollach arxiv:83.2415v1 [cond-mat.mtrl-sci] 17 Mar 28 University Service Center for Transmission
More informationDecays and Scattering. Decay Rates Cross Sections Calculating Decays Scattering Lifetime of Particles
Decays and Scattering Decay Rates Cross Sections Calculating Decays Scattering Lifetime of Particles 1 Decay Rates There are THREE experimental probes of Elementary Particle Interactions - bound states
More information6. Analytical Electron Microscopy
Physical Principles of Electron Microscopy 6. Analytical Electron Microscopy Ray Egerton University of Alberta and National Institute of Nanotechnology Edmonton, Canada www.tem-eels.ca regerton@ualberta.ca
More informationSite-specific electron diffraction resolved via nuclear recoil
Site-specific electron diffraction resolved via nuclear recoil Aimo Winkelmann Maarten Vos Max-Planck-Institut für Mikrostrukturphysik Halle (Saale), Germany Research School of Physics and Engineering
More informationSmall-Angle X-ray Scattering (SAXS)/X-ray Absorption Near Edge Spectroscopy (XANES).
S1 Small-Angle X-ray Scattering (SAXS)/X-ray Absorption Near Edge Spectroscopy (XANES). The combined SAXS/XANES measurements were carried out at the µspot beamline at BESSY II (Berlin, Germany). The beamline
More informationNeutron and x-ray spectroscopy
Neutron and x-ray spectroscopy B. Keimer Max-Planck-Institute for Solid State Research outline 1. self-contained introduction neutron scattering and spectroscopy x-ray scattering and spectroscopy 2. application
More informationRutherford Backscattering Spectrometry
Rutherford Backscattering Spectrometry EMSE-515 Fall 2005 F. Ernst 1 Bohr s Model of an Atom existence of central core established by single collision, large-angle scattering of alpha particles ( 4 He
More informationQuantum Condensed Matter Physics Lecture 5
Quantum Condensed Matter Physics Lecture 5 detector sample X-ray source monochromator David Ritchie http://www.sp.phy.cam.ac.uk/drp2/home QCMP Lent/Easter 2019 5.1 Quantum Condensed Matter Physics 1. Classical
More informationElectron-Matter Interactions
Electron-Matter Interactions examples of typical EM studies properties of electrons elastic electron-matter interactions scattering processes; coherent and incoherent image formation; chemical contrast;
More informationMT Electron microscopy Scanning electron microscopy and electron probe microanalysis
MT-0.6026 Electron microscopy Scanning electron microscopy and electron probe microanalysis Eero Haimi Research Manager Outline 1. Introduction Basics of scanning electron microscopy (SEM) and electron
More informationTransmission Electron Microscopy
L. Reimer H. Kohl Transmission Electron Microscopy Physics of Image Formation Fifth Edition el Springer Contents 1 Introduction... 1 1.1 Transmission Electron Microscopy... 1 1.1.1 Conventional Transmission
More informationMethoden moderner Röntgenphysik I. Coherence based techniques II. Christian Gutt DESY, Hamburg
Methoden moderner Röntgenphysik I Coherence based techniques II Christian Gutt DESY Hamburg christian.gutt@desy.de 8. January 009 Outline 18.1. 008 Introduction to Coherence 8.01. 009 Structure determination
More information2. Passage of Radiation Through Matter
2. Passage of Radiation Through Matter Passage of Radiation Through Matter: Contents Energy Loss of Heavy Charged Particles by Atomic Collision (addendum) Cherenkov Radiation Energy loss of Electrons and
More informationIMAGING DIFFRACTION SPECTROSCOPY
TEM Techniques TEM/STEM IMAGING DIFFRACTION SPECTROSCOPY Amplitude contrast (diffracion contrast) Phase contrast (highresolution imaging) Selected area diffraction Energy dispersive X-ray spectroscopy
More informationEnergy Spectroscopy. Excitation by means of a probe
Energy Spectroscopy Excitation by means of a probe Energy spectral analysis of the in coming particles -> XAS or Energy spectral analysis of the out coming particles Different probes are possible: Auger
More informationExperimental Determination of Crystal Structure
Experimental Determination of Crystal Structure Branislav K. Nikolić Department of Physics and Astronomy, University of Delaware, U.S.A. PHYS 624: Introduction to Solid State Physics http://www.physics.udel.edu/~bnikolic/teaching/phys624/phys624.html
More informationQuantum Mechanics II Lecture 11 (www.sp.phy.cam.ac.uk/~dar11/pdf) David Ritchie
Quantum Mechanics II Lecture (www.sp.phy.cam.ac.u/~dar/pdf) David Ritchie Michaelmas. So far we have found solutions to Section 4:Transitions Ĥ ψ Eψ Solutions stationary states time dependence with time
More informationLecture 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 informationQuantum Physics Lecture 3
Quantum Physics Lecture 3 If light (waves) are particle-like, are particles wave-like? Electron diffraction - Davisson & Germer Experiment Particle in a box -Quantisation of energy Wave Particle?? Wave
More informationCHEM-E5225 :Electron Microscopy X-Ray Spectrometry
CHEM-E5225 :Electron Microscopy X-Ray Spectrometry 2016.11 Yanling Ge Outline X-ray Spectrometry X-ray Spectra and Images Qualitative and Quantitative X-ray Analysis and Imaging Discussion of homework
More informationMaking the Invisible Visible: Probing Antiferromagnetic Order in Novel Materials
Making the Invisible Visible: Probing Antiferromagnetic Order in Novel Materials Elke Arenholz Lawrence Berkeley National Laboratory Antiferromagnetic contrast in X-ray absorption Ni in NiO Neel Temperature
More information2. TranSIESTA 1. SIESTA. DFT In a Nutshell. Introduction to SIESTA. Boundary Conditions: Open systems. Greens functions and charge density
1. SIESTA DFT In a Nutshell Introduction to SIESTA Atomic Orbitals Capabilities Resources 2. TranSIESTA Transport in the Nanoscale - motivation Boundary Conditions: Open systems Greens functions and charge
More informationHigh-Resolution. Transmission. Electron Microscopy
Part 4 High-Resolution Transmission Electron Microscopy 186 Significance high-resolution transmission electron microscopy (HRTEM): resolve object details smaller than 1nm (10 9 m) image the interior of
More informationV 11: Electron Diffraction
Martin-Luther-University Halle-Wittenberg Institute of Physics Advanced Practical Lab Course V 11: Electron Diffraction An electron beam conditioned by an electron optical system is diffracted by a polycrystalline,
More informationNotes on x-ray scattering - M. Le Tacon, B. Keimer (06/2015)
Notes on x-ray scattering - M. Le Tacon, B. Keimer (06/2015) Interaction of x-ray with matter: - Photoelectric absorption - Elastic (coherent) scattering (Thomson Scattering) - Inelastic (incoherent) scattering
More informationTechniques EDX, EELS et HAADF en TEM: possibilités d analyse et applications
Techniques EDX, EELS et HAADF en TEM: possibilités d analyse et applications Thomas Neisius Université Paul Cézanne Plan Imaging modes HAADF Example: supported Pt nanoparticles Electron sample interaction
More informationX-Ray Scattering Studies of Thin Polymer Films
X-Ray Scattering Studies of Thin Polymer Films Introduction to Neutron and X-Ray Scattering Sunil K. Sinha UCSD/LANL Acknowledgements: Prof. R.Pynn( Indiana U.) Prof. M.Tolan (U. Dortmund) Wilhelm Conrad
More informationInteraction X-rays - Matter
Interaction X-rays - Matter Pair production hν > M ev Photoelectric absorption hν MATTER hν Transmission X-rays hν' < hν Scattering hν Decay processes hν f Compton Thomson Fluorescence Auger electrons
More informationPHYS Introduction to Synchrotron Radiation
PHYS 570 - Introduction to Synchrotron Radiation Term: Spring 2015 Meetings: Tuesday & Thursday 17:00-18:15 Location: 204 Stuart Building Instructor: Carlo Segre Office: 166A Life Sciences Phone: 312.567.3498
More informationPhonons In The Elk Code
Phonons In The Elk Code Kay Dewhurst, Sangeeta Sharma, Antonio Sanna, Hardy Gross Max-Planck-Institut für Mikrostrukturphysik, Halle If you are allowed to measure only one property of a material, make
More informationSome history. F p. 1/??
Some history F 12 10 18 p. 1/?? F 12 10 18 p. 1/?? Some history 1600: Galileo Galilei 1564 1642 cf. section 7.0 Johannes Kepler 1571 1630 cf. section 3.7 1700: Isaac Newton 1643 1727 cf. section 1.1 1750
More information4. Other diffraction techniques
4. Other diffraction techniques 4.1 Reflection High Energy Electron Diffraction (RHEED) Setup: - Grazing-incidence high energy electron beam (3-5 kev: MEED,
More informationConventional Transmission Electron Microscopy. Introduction. Text Books. Text Books. EMSE-509 CWRU Frank Ernst
Text Books Conventional Transmission Electron Microscopy EMSE-509 CWRU Frank Ernst D. B. Williams and C. B. Carter: Transmission Electron Microscopy, New York: Plenum Press (1996). L. Reimer: Transmission
More informationLecture 06. Fundamentals of Lidar Remote Sensing (4) Physical Processes in Lidar
Lecture 06. Fundamentals of Lidar Remote Sensing (4) Physical Processes in Lidar Physical processes in lidar (continued) Doppler effect (Doppler shift and broadening) Boltzmann distribution Reflection
More informationLinear response theory and TDDFT
Linear response theory and TDDFT Claudio Attaccalite http://abineel.grenoble.cnrs.fr/ CECAM Yambo School 2013 (Lausanne) Motivations: +- hν Absorption Spectroscopy Many Body Effects!!! Motivations(II):Absorption
More informationANALYTICAL TRANSMISSION ELECTRON MICROSCOPY
Annu. Rev. Mater. Res. 2005. 35:239 314 doi: 10.1146/annurev.matsci.35.102303.091623 Copyright c 2005 by Annual Reviews. All rights reserved First published online as a Review in Advance on March 17, 2005
More informationSemiclassical formulation
The story so far: Transport coefficients relate current densities and electric fields (currents and voltages). Can define differential transport coefficients + mobility. Drude picture: treat electrons
More informationNanoelectronics 09. Atsufumi Hirohata Department of Electronics. Quick Review over the Last Lecture
Nanoelectronics 09 Atsufumi Hirohata Department of Electronics 13:00 Monday, 12/February/2018 (P/T 006) Quick Review over the Last Lecture ( Field effect transistor (FET) ): ( Drain ) current increases
More informationMagnetism in transition metal oxides by post-dft methods
Magnetism in transition metal oxides by post-dft methods Cesare Franchini Faculty of Physics & Center for Computational Materials Science University of Vienna, Austria Workshop on Magnetism in Complex
More informationName: (a) What core levels are responsible for the three photoelectron peaks in Fig. 1?
Physics 243A--Surface Physics of Materials: Spectroscopy Final Examination December 16, 2014 (3 problems, 100 points total, open book, open notes and handouts) Name: [1] (50 points), including Figures
More informationHigh-Resolution Transmission Electron Microscopy
Chapter 2 High-Resolution Transmission Electron Microscopy The most fundamental imaging mode of a transmission electron microscope is realized by illuminating an electron-transparent specimen with a broad
More informationHow can x-ray intensity fluctuation spectroscopy push the frontiers of Materials Science. Mark Sutton McGill University
How can x-ray intensity fluctuation spectroscopy push the frontiers of Materials Science Mark Sutton McGill University Coherent diffraction (001) Cu 3 Au peak Sutton et al., The Observation of Speckle
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 informationNon-relativistic scattering
Non-relativistic scattering Contents Scattering theory 2. Scattering amplitudes......................... 3.2 The Born approximation........................ 5 2 Virtual Particles 5 3 The Yukawa Potential
More informationSTM: 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 informationApplied Nuclear Physics (Fall 2006) Lecture 19 (11/22/06) Gamma Interactions: Compton Scattering
.101 Applied Nuclear Physics (Fall 006) Lecture 19 (11//06) Gamma Interactions: Compton Scattering References: R. D. Evans, Atomic Nucleus (McGraw-Hill New York, 1955), Chaps 3 5.. W. E. Meyerhof, Elements
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 informationMonte Carlo simulation of Secondary Electron Yield for Noble metals Martina Azzolini, Nicola M. Pugno, Simone Taioli, Maurizio Dapor
Monte Carlo simulation of Secondary Electron Yield for Noble metals Martina Azzolini, Nicola M. Pugno, Simone Taioli, Maurizio Dapor ECLOUD 18 - Elba Island- 3-7 June 2018 OUTLINE Description of the Monte
More informationOld Dominion University Physics 811 Fall 2008
Old Dominion University Physics 811 Fall 008 Projects Structure of Project Reports: 1 Introduction. Briefly summarize the nature of the physical system. Theory. Describe equations selected for the project.
More informationSmall Angle Neutron Scattering in Different Fields of Research. Henrich Frielinghaus
Small Angle Neutron Scattering in Different Fields of Research Henrich Frielinghaus Jülich Centre for Neutron Science Forschungszentrum Jülich GmbH Lichtenbergstrasse 1 85747 Garching (München) h.frielinghaus@fz-juelich.de
More informationLecture: Scattering theory
Lecture: Scattering theory 30.05.2012 SS2012: Introduction to Nuclear and Particle Physics, Part 2 2 1 Part I: Scattering theory: Classical trajectoriest and cross-sections Quantum Scattering 2 I. Scattering
More informationSolid State Spectroscopy Problem Set 7
Solid State Spectroscopy Problem Set 7 Due date: June 29th, 2015 Problem 5.1 EXAFS Study of Mn/Fe substitution in Y(Mn 1-x Fe x ) 2 O 5 From article «EXAFS, XANES, and DFT study of the mixed-valence compound
More informationMS482 Materials Characterization ( 재료분석 ) Lecture Note 5: RBS. Byungha Shin Dept. of MSE, KAIST
2015 Fall Semester MS482 Materials Characterization ( 재료분석 ) Lecture Note 5: RBS Byungha Shin Dept. of MSE, KAIST 1 Course Information Syllabus 1. Overview of various characterization techniques (1 lecture)
More informationElectronic Structure Methodology 1
Electronic Structure Methodology 1 Chris J. Pickard Lecture Two Working with Density Functional Theory In the last lecture we learnt how to write the total energy as a functional of the density n(r): E
More informationDrickamer type. Disk containing the specimen. Pressure cell. Press
ε-fe Drickamer type Press Pressure cell Disk containing the specimen Low Temperature Cryostat Diamond Anvil Cell (DAC) Ruby manometry Re gasket for collimation Small size of specimen space High-density
More informationMT Electron microscopy Scanning electron microscopy and electron probe microanalysis
MT-0.6026 Electron microscopy Scanning electron microscopy and electron probe microanalysis Eero Haimi Research Manager Outline 1. Introduction Basics of scanning electron microscopy (SEM) and electron
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 informationIntroduction to spin and spin-dependent phenomenon
Introduction to spin and spin-dependent phenomenon Institut für Theoretische Physik Freie Universität Berlin, Germany and Fritz Haber Institute of the Max Planck Society, Berlin, Germany. May 16th, 2007
More informationSupplementary Figure 1: ADF images and profiles for several types of atomic chains encapsulated in DWNTs. (a d) ADF images of NaI, CsF, CsCl, and CsI
Supplementary Figure 1: ADF images and profiles for several types of atomic chains encapsulated in DWNTs. (a d) ADF images of NaI, CsF, CsCl, and CsI atomic chains encapsulated in DWNTs, respectively.
More informationPHYS Introduction to Synchrotron Radiation
C. Segre (IIT) PHYS 570 - Spring 2018 January 09, 2018 1 / 20 PHYS 570 - Introduction to Synchrotron Radiation Term: Spring 2018 Meetings: Tuesday & Thursday 13:50-15:05 Location: 213 Stuart Building Instructor:
More informationSoft X-ray Physics DELNOR-WIGGINS PASS STATE PARK
Soft X-ray Physics Overview of research in Prof. Tonner s group Introduction to synchrotron radiation physics Photoemission spectroscopy: band-mapping and photoelectron diffraction Magnetic spectroscopy
More informationSilver Thin Film Characterization
Silver Thin Film Characterization.1 Introduction Thin films of Ag layered structures, typically less than a micron in thickness, are tailored to achieve desired functional properties. Typical characterization
More informationPHY492: Nuclear & Particle Physics. Lecture 4 Nature of the nuclear force. Reminder: Investigate
PHY49: Nuclear & Particle Physics Lecture 4 Nature of the nuclear force Reminder: Investigate www.nndc.bnl.gov Topics to be covered size and shape mass and binding energy charge distribution angular momentum
More informationThe frequency-dependent Sternheimer equation in TDDFT
The frequency-dependent Sternheimer equation in TDDFT A new look into an old equation Miguel A. L. Marques 1 Centre for Computational Physics, University of Coimbra, Portugal 2 LPMCN, Université Claude
More informationCRYSTALLOGRAPHIC POINT AND SPACE GROUPS. Andy Elvin June 10, 2013
CRYSTALLOGRAPHIC POINT AND SPACE GROUPS Andy Elvin June 10, 2013 Contents Point and Space Groups Wallpaper Groups X-Ray Diffraction Electron Wavefunction Neumann s Principle Magnetic Point Groups Point
More informationStructure of Cement Phases from ab initio Modeling Crystalline C-S-HC
Structure of Cement Phases from ab initio Modeling Crystalline C-S-HC Sergey V. Churakov sergey.churakov@psi.ch Paul Scherrer Institute Switzerland Cement Phase Composition C-S-H H Solid Solution Model
More informationPhysics of Finite and Infinite Nuclear Systems Phys. 477 (542)
Physics of Finite and Infinite Nuclear Systems Phys. 477 (542) Class: Tu & Th from 11:30 am to 1:00 pm (Compton 241 mostly) Extra hour: Mo 4 pm make-up hour for planned trips to Tokyo, San Francisco, and
More informationElastic and Inelastic Scattering in Electron Diffraction and Imaging
Elastic and Inelastic Scattering in Electron Diffraction and Imaging Contents Introduction Symbols and definitions Part A Diffraction and imaging of elastically scattered electrons Chapter 1. Basic kinematical
More informationChapter 37 Early Quantum Theory and Models of the Atom
Chapter 37 Early Quantum Theory and Models of the Atom Units of Chapter 37 37-7 Wave Nature of Matter 37-8 Electron Microscopes 37-9 Early Models of the Atom 37-10 Atomic Spectra: Key to the Structure
More informationApplications of scattering theory! From the structure of the proton! to protein structure!
Applications of scattering theory From the structure of the proton to protein structure Nicuşor Tîmneanu 2016 Contents and goals What is scattering and why study it? How is the structure of matter determined?
More informationQuantum physics. Anyone who is not shocked by the quantum theory has not understood it. Niels Bohr, Nobel Price in 1922 ( )
Quantum physics Anyone who is not shocked by the quantum theory has not understood it. Niels Bohr, Nobel Price in 1922 (1885-1962) I can safely say that nobody understand quantum physics Richard Feynman
More informationPhys 622 Problems Chapter 6
1 Problem 1 Elastic scattering Phys 622 Problems Chapter 6 A heavy scatterer interacts with a fast electron with a potential V (r) = V e r/r. (a) Find the differential cross section dσ dω = f(θ) 2 in the
More informationAn Approximate DFT Method: The Density-Functional Tight-Binding (DFTB) Method
Fakultät für Mathematik und Naturwissenschaften - Lehrstuhl für Physikalische Chemie I / Theoretische Chemie An Approximate DFT Method: The Density-Functional Tight-Binding (DFTB) Method Jan-Ole Joswig
More informationTDDFT in Chemistry and Biochemistry III
TDDFT in Chemistry and Biochemistry III Dmitrij Rappoport Department of Chemistry and Chemical Biology Harvard University TDDFT Winter School Benasque, January 2010 Dmitrij Rappoport (Harvard U.) TDDFT
More informationB k k. Fig. 1: Energy-loss spectrum of BN, showing the how K-loss intensities I K (β, ) for boron and nitrogen are defined and measured.
The accuracy of EELS elemental analysis The procedure of EELS elemental analysis can be divided into three parts, each of which involves some approximation, with associated systematic or statistical errors.
More informationTechnical University of Denmark. Center for Electron Nanoscopy. Advanced TEM (16 September 2010) Microanalysis in the electron microscope
Microanalysis in the electron microscope MH1 1 Technical University of Denmark Center for Electron Nanoscopy Advanced TEM (16 September 2010) Microanalysis in the electron microscope Dr C B Boothroyd Synopsis
More informationElectron Energy Loss Spectrometry
Electron Energy Loss Spectrometry Cécile Hébert Centre Interdisciplinaire de Microscopie Electronique Laboratoire de Spectrométrie et Microscopie Electronique Ecole Polytechnique Fédérale de Lausanne Abstract
More informationAn Introduction to Diffraction and Scattering. School of Chemistry The University of Sydney
An Introduction to Diffraction and Scattering Brendan J. Kennedy School of Chemistry The University of Sydney 1) Strong forces 2) Weak forces Types of Forces 3) Electromagnetic forces 4) Gravity Types
More informationScattering of Electromagnetic Radiation. References:
Scattering of Electromagnetic Radiation References: Plasma Diagnostics: Chapter by Kunze Methods of experimental physics, 9a, chapter by Alan Desilva and George Goldenbaum, Edited by Loveberg and Griem.
More information1. Nuclear Size. A typical atom radius is a few!10 "10 m (Angstroms). The nuclear radius is a few!10 "15 m (Fermi).
1. Nuclear Size We have known since Rutherford s! " scattering work at Manchester in 1907, that almost all the mass of the atom is contained in a very small volume with high electric charge. Nucleus with
More informationKey concepts in Density Functional Theory (I) Silvana Botti
From the many body problem to the Kohn-Sham scheme European Theoretical Spectroscopy Facility (ETSF) CNRS - Laboratoire des Solides Irradiés Ecole Polytechnique, Palaiseau - France Temporary Address: Centre
More informationInteraction theory Photons. Eirik Malinen
Interaction theory Photons Eirik Malinen Introduction Interaction theory Dosimetry Radiation source Ionizing radiation Atoms Ionizing radiation Matter - Photons - Charged particles - Neutrons Ionizing
More informationAb initio phonon calculations in mixed systems
Ab initio phonon calculations in mixed systems Andrei Postnikov apostnik@uos.de Outline: Experiment vs. ab initio theory Ways of theory: linear response and frozen phonon approaches Applications: Be x
More informationCore-Level spectroscopy. Experiments and first-principles calculations. Tomoyuki Yamamoto. Waseda University, Japan
Core-Level spectroscopy Experiments and first-principles calculations Tomoyuki Yamamoto Waseda University, Japan 22 nd WIEN2k workshop Jun. 26 th, 2015@Singapore Outline What is core-level spectroscopy
More information