Laboratoire de Chimie Physique - Matière et Rayonnement Physical Chemistry Matter and Radiation Laboratory LCPMR - UMR 7614
|
|
- Myron May
- 5 years ago
- Views:
Transcription
1 Laboratoire de Chimie Physique - Matière et Rayonnement Physical Chemistry Matter and Radiation Laboratory LCPMR - UMR 7614 Alain Dubois, Directeur Francis Penent, Sous-Directeur Affiliations: CNRS : Institut de Chimie (70%) et Institut de Physique (30%) CN : 13, 4, 6, 14 UPMC : "Energy, Matter et the Universe» center and Chemistry Faculty A Electronic strucuture of Complex materials Resp: J.-M. Mariot, PR B Surface and interface Reactivity Resp: F. Rochet, PR S. Carniato, MCF C Reactivity under radidation in gas phase Resp: M. Simon, DR
2 " 72 staff with " 45 permanents 11 DR/CR (+1) et 17 PR/MCF (+3) 7 ITA et 9 IATOS 15 PhDs, 6 postdoc + interns
3 A Electronic structure of complex materials Jean-Michel Mariot (PR) B Surface and interfaces Reactivity F. Rochet (PR) - S. Carniato (MCF) C - Reactivity under radiation in gas phase Marc Simon (DR) A-1. Strongly correlated systems - Magnetic materials femtosecond dynamics of (de-)magnetization Electronic properties under pressure, Excitation and collective dynamics in oxydes of transition elements, Ordered networks of magnetic objects, Diluted Magnetic Semiconductors, Resonante X-ray spectro (RIXS, XRMS), Coherente X-ray scattering, Spectro RIXS, XPS HE/HR, Magnetron (magnetic thin layers) + MOKE (Magneto Optical Kerr Effect) A-2. Interfaces and multimaterials - Sources et X-ray optics Physical chemistry at the interfaces in periodic multilayers, X-ray emission, reflectometry, Monochromators/sources IRIS, MONOX, XUV B-1. Modelling Inner shell spectroscopy, Fragmentation dynamics, Defaults in oxyds, interfaces Si-SiO 2, Si-HfO 2, B-2. Functionalized surfaces surfaces Sciences molecular adsorption on Si Reactivity on surfaces, CSEAL + STM HP + XPSHP + XPS B-3. Physical chemistry of environnemental and spatiales ices Reactivity on water ice surfaces, Spectroscopies MIES, IR, SUMO (ex SACEMOR) C-1. Relaxation of inner shell excited molecules Vector correlation spectro. e ion,rx-ion, RX resonante scattering, Ultra-fast nuclear dynamics CELIMENE + RIXS + photoém. HE/HR C-2. Electronic correlations studied in coincidence Dynamical aspects of Auger effects, Double ionisation in valence inner s shell, ICD, HERMES C-3. Dynamics of quantum systems in strong fields ion-atom/molecule collisions, Dynamique in IR strong laser fields, Imagery of molecular orbitals, Two-color IR-XUV
4 A Electronic structure of complex materials Jean-Michel Mariot (PR) B Surface and interfaces Reactivity F. Rochet (PR) - S. Carniato (MCF) C - Reactivity under radiation in gas phase Marc Simon (DR) A-1. Strongly correlated systems - Magnetic materials femtosecond dynamics of (de-)magnetization Electronic properties under pressure, Excitation and collective dynamics in oxydes of transition elements, Ordered networks of magnetic objects, Diluted Magnetic Semiconductors, Resonante X-ray spectro (RIXS, XRMS), Coherente X-ray scattering, Spectro RIXS, XPS HE/HR, Magnetron (magnetic thin layers) + MOKE (Magneto Optical Kerr Effect) A-2. Interfaces and multimaterials - Sources et X-ray optics Physical chemistry at the interfaces in periodic multilayers, X-ray emission, reflectometry, Monochromators/sources IRIS, MONOX, XUV B-1. Modelling Inner shell spectroscopy, Fragmentation dynamics, Defaults in oxyds, interfaces Si-SiO 2, Si-HfO 2, B-2. Functionalized surfaces surfaces Sciences molecular adsorption on Si Reactivity on surfaces, CSEAL + STM HP + XPSHP + XPS B-3. Physical chemistry of environnemental and spatiales ices Reactivity on water ice surfaces, Spectroscopies MIES, IR, SUMO (ex SACEMOR) C-1. Relaxation of inner shell excited molecules Vector correlation spectro. e ion,rx-ion, RX resonante scattering, Ultra-fast nuclear dynamics CELIMENE + RIXS + photoém. HE/HR C-2. Electronic correlations studied in coincidence Dynamical aspects of Auger effects, Double ionisation in valence inner s shell, ICD, HERMES C-3. Dynamics of quantum systems in strong fields ion-atom/molecule collisions, Dynamique in IR strong laser fields, Imagery of molecular orbitals, Two-color IR-XUV
5 Dynamics of quantum systems in strong fields J. Caillat A. Maquet R. Taïeb N. Sisourat R. Guichard R. Della Picca G. Labaigt I. Pilskog H. Agueny S. Chqondi
6 Theory of ion-atom/molecule - One- and two-electron processes in multicenter collisional systems Electronic processes: A q+ + B* excitation A q+ + B A (q-1)+ + B + capture A q+ + B + + e - ionisation
7 " the modelisation of MOTIVATIONS the ultra-fast dynamics of atomic and molecular systems the interplay of the many open channels " non-perturbative treatments Dynamical electronic correlation and the complete atomic/molecular Intermediate to high energy range electronic spectrum (including continuum) E kev/u = 0.1 kev/u " Fundamental aspects of dynamical few-body quantum systems and 65 MeV/u => v " a.u. computations of cross sections for applications Interaction region a " 10 a.u. P v R ( t ) R (t) Collision time 200 a.u. < = a / v < 0.2 a.u. 1 a.u. of B time = s femtosecond - attosecond B time scale R ab R ab A A p e P E kev/u " 25 A v 2 v Single ionisation of molecules Double electron transfer from molecules to ions
8 Theoretical models : Semi-classical approach Sudden approximation (R AB fixed) Non-perturbative * For high impact energies (> 1 Mev/u) lattice representation : 1e-(1-3)D, 2e-1D * For intermediate energies (" 1 kev/u) travelling AO/MO basis sets expansion 2e v Collision geometry (3D) x P b e - R(t) r 1 B r 2 e - y R AB A z
9 High (MeV) energy processes : A q+ + H 2 A q+ + H e - ionisation Lattice representation
10 63 MeV/u 1e - 1D Kr H Kr H 2 N. Sisourat, J. Caillat, A. Dubois and P. D. Fainstein, Phys. Rev. A 76, (2007)
11 Low energy ion-molecule collisions Electron capture (1 electron system) (resonant system) Recent experimental results Bräuning et al, J. Phys. B (2001) Total capture Reiser et al, HCI-2002, Caen Orientation effects (COLTRIMS)
12 v = 1.0 a.u. $ = 90 $ = 0 //# dominates
HEAVY PARTICLE COLLISION PROCESSES. Alain Dubois
HEAVY PARTICLE COLLISION PROCESSES Alain Dubois Laboratoire de Chimie Physique - Matière et Rayonnement Université Pierre et Marie Curie - CNRS Paris FRANCE Heavy particle collision processes I - Introduction
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 informationMulti-electron coincidence spectroscopy: double photoionization from molecular inner-shell orbitals
Journal of Physics: Conference Series OPEN ACCESS Multi-electron coincidence spectroscopy: double photoionization from molecular inner-shell orbitals To cite this article: Y Hikosaka et al 2014 J. Phys.:
More informationPhotoelectron spectroscopy Instrumentation. Nanomaterials characterization 2
Photoelectron spectroscopy Instrumentation Nanomaterials characterization 2 RNDr. Věra V Vodičkov ková,, PhD. Photoelectron Spectroscopy general scheme Impact of X-ray emitted from source to the sample
More informationWavelength 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 informationLecture 3: Optical Properties of Insulators, Semiconductors, and Metals. 5 nm
Metals Lecture 3: Optical Properties of Insulators, Semiconductors, and Metals 5 nm Course Info Next Week (Sept. 5 and 7) no classes First H/W is due Sept. 1 The Previous Lecture Origin frequency dependence
More informationAMO at FLASH. FELs provide unique opportunities and challenges for AMO physics. due to essentially three reasons:
Experience at FLASH AMO at FLASH FELs provide unique opportunities and challenges for AMO physics due to essentially three reasons: AMO at FLASH 1. huge integrated flux dilute samples Highly charged ions
More informationCore 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 informationElectron Spectroscopy
Electron Spectroscopy Photoelectron spectroscopy is based upon a single photon in/electron out process. The energy of a photon is given by the Einstein relation : E = h ν where h - Planck constant ( 6.62
More informationInelastic soft x-ray scattering, fluorescence and elastic radiation
Inelastic soft x-ray scattering, fluorescence and elastic radiation What happens to the emission (or fluorescence) when the energy of the exciting photons changes? The emission spectra (can) change. One
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 informationICPEAC XXX, Carins, Australia. Nonlinear resonant Auger spectroscopy in CO using an x-ray pump-control scheme 2017/07/31
ICPEAC XXX, Carins, Australia Nonlinear resonant Auger spectroscopy in CO using an x-ray pump-control scheme Song-Bin Zhang Shaanxi Normal University, Xi an, China 2017/07/31 Acknowledgements Victor Kimberg
More informationAttosecond laser systems and applications
Attosecond laser systems and applications Adrian N. Pfeiffer Chemical Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA 8th Annual Laser Safety Officer Workshop September
More informationSurface analysis techniques
Experimental methods in physics Surface analysis techniques 3. Ion probes Elemental and molecular analysis Jean-Marc Bonard Academic year 10-11 3. Elemental and molecular analysis 3.1.!Secondary ion mass
More informationElectron Spettroscopies
Electron Spettroscopies Spettroscopy allows to characterize a material from the point of view of: chemical composition, electronic states and magnetism, electronic, roto-vibrational and magnetic excitations.
More informationNuclear Physics and Astrophysics
Nuclear Physics and Astrophysics PHY-302 Dr. E. Rizvi Lecture 13 - Gamma Radiation Material For This Lecture Gamma decay: Definition Quantum interpretation Uses of gamma spectroscopy 2 Turn to γ decay
More informationJoint ICTP-IAEA Workshop on Fusion Plasma Modelling using Atomic and Molecular Data January 2012
2327-4 Joint ICTP- Workshop on Fusion Plasma Modelling using Atomic and Molecular Data 23-27 January 2012 Atomic Processes Modeling in Plasmas Modeling Spectroscopic Observables from Plasmas Hyun-Kyung
More informationEnergy Spectroscopy. Ex.: Fe/MgO
Energy Spectroscopy Spectroscopy gives access to the electronic properties (and thus chemistry, magnetism,..) of the investigated system with thickness dependence Ex.: Fe/MgO Fe O Mg Control of the oxidation
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 informationIntroduction to X-ray Photoelectron Spectroscopy (XPS) XPS which makes use of the photoelectric effect, was developed in the mid-1960
Introduction to X-ray Photoelectron Spectroscopy (XPS) X-ray Photoelectron Spectroscopy (XPS), also known as Electron Spectroscopy for Chemical Analysis (ESCA) is a widely used technique to investigate
More informationInternational Atomic Energy Agency, Vienna, Austria. Charge Transfer in Collisions of Ions with atoms and molecules.
International Centre for Theoretical Physics (ICTP), Trieste, Italy International Atomic Energy Agency, Vienna, Austria Training Workshop on Atomic and Molecular Data for Fusion Energy Research Charge
More informationMSE 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 informationX-ray production from resonant coherent excitation of relativistic HCIs in crystals as a model for polarization XFEL studies in the kev range
X-ray production from resonant coherent excitation of relativistic HCIs in crystals as a model for polarization XFEL studies in the kev range V.V.Balashov, A.A.Sokolik, A.V.Stysin D.V.Skobeltsyn Institute
More informationChapter VI: Ionizations and excitations
Chapter VI: Ionizations and excitations 1 Content Introduction Ionization in gases Ionization in solids Fano factor 2 Introduction (1) Ionizations created by charged particles (incident particles or particles
More informationX-ray Energy Spectroscopy (XES).
X-ray Energy Spectroscopy (XES). X-ray fluorescence as an analytical tool for element analysis is based on 3 fundamental parameters: A. Specificity: In determining an x-ray emission energy E certainty
More informationLaser-controlled Molecular Alignment and Orientation. Marc Vrakking FOM Institute AMOLF
Laser-controlled Molecular Alignment and Orientation Marc Vrakking FOM Institute AMOLF Summer School Cargese - Tuesday August 19 th 2008 Contents What is molecular alignment resp. orientation, and why
More informationSolid 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 informationModeling cold collisions Atoms Molecules
Modeling cold collisions Atoms Molecules E. Tiemann, H. Knöckel, A. Pashov* Institute of Quantum Optics *University Sofia, Bulgaria collisional wave function for E 0 A R=0 hk r B adopted from J. Weiner
More informationMS482 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 informationTopic 3: Periodic Trends and Atomic Spectroscopy
Topic 3: Periodic Trends and Atomic Spectroscopy Introduction Valence Electrons are those in the outer most shell of an element and are responsible for the bonding characteristics of that element. Core
More informationLecture 10. Transition probabilities and photoelectric cross sections
Lecture 10 Transition probabilities and photoelectric cross sections TRANSITION PROBABILITIES AND PHOTOELECTRIC CROSS SECTIONS Cross section = = Transition probability per unit time of exciting a single
More informationMethods of surface analysis
Methods of surface analysis Nanomaterials characterisation I RNDr. Věra Vodičková, PhD. Surface of solid matter: last monoatomic layer + absorbed monolayer physical properties are effected (crystal lattice
More informationStudy Plan for Ph.D in Physics (2011/2012)
Plan Study Plan for Ph.D in Physics (2011/2012) Offered Degree: Ph.D in Physics 1. General Rules and Conditions:- This plan conforms to the regulations of the general frame of the higher graduate studies
More informationATOMIC AND LASER SPECTROSCOPY
ALAN CORNEY ATOMIC AND LASER SPECTROSCOPY CLARENDON PRESS OXFORD 1977 Contents 1. INTRODUCTION 1.1. Planck's radiation law. 1 1.2. The photoelectric effect 4 1.3. Early atomic spectroscopy 5 1.4. The postulates
More informationNew theoretical insights on the physics of compound nuclei from laser-nucleus reactions
New theoretical insights on the physics of compound nuclei from laser-nucleus reactions Adriana Pálffy Max Planck Institute for Nuclear Physics, Heidelberg, Germany Laser-Driven Radiation Sources for Nuclear
More informationChemistry Instrumental Analysis Lecture 5. Chem 4631
Chemistry 4631 Instrumental Analysis Lecture 5 Light Amplification by Stimulated Emission of Radiation High Intensities Narrow Bandwidths Coherent Outputs Applications CD/DVD Readers Fiber Optics Spectroscopy
More informationCurrent Research and Future Plans
Current Research and Future Plans Bhas Bapat PRL, Ahmedbad At IISER Pune, Jan 2014 Bhas Bapat (PRL, Ahmedbad) Current Research and Future Plans At IISER Pune, Jan 2014 1 / 21 Contents Broad Areas Dissociative
More informationX-Ray Photoelectron Spectroscopy (XPS)-2
X-Ray Photoelectron Spectroscopy (XPS)-2 Louis Scudiero http://www.wsu.edu/~scudiero; 5-2669 Fulmer 261A Electron Spectroscopy for Chemical Analysis (ESCA) The 3 step model: 1.Optical excitation 2.Transport
More informationAxion detection by atomic/molecular transitions
Axion detection by atomic/molecular transitions Dark matter axions may cause transitions between atomic states Due to very low interaction cross section, it necessary to look for axion induced transition
More informationReview of Optical Properties of Materials
Review of Optical Properties of Materials Review of optics Absorption in semiconductors: qualitative discussion Derivation of Optical Absorption Coefficient in Direct Semiconductors Photons When dealing
More informationClassification of spectroscopic methods
Introduction Spectroscopy is the study of the interaction between the electromagnetic radiation and the matter. Spectrophotometry is the measurement of these interactions i.e. the measurement of the intensity
More informationLECTURE NOTES. Ay/Ge 132 ATOMIC AND MOLECULAR PROCESSES IN ASTRONOMY AND PLANETARY SCIENCE. Geoffrey A. Blake. Fall term 2016 Caltech
LECTURE NOTES Ay/Ge 132 ATOMIC AND MOLECULAR PROCESSES IN ASTRONOMY AND PLANETARY SCIENCE Geoffrey A. Blake Fall term 2016 Caltech Acknowledgment Part of these notes are based on lecture notes from the
More informationLaser induced manipulation of atom pair interaction
Laser induced manipulation of atom pair interaction St. Falke, Chr. Samuelis, H. Knöckel, and E. Tiemann Institute of Quantum Optics, European Research Training Network Cold Molecules SFB 407 Quantum limited
More informationWP-3: HHG and ultrafast electron imaging
WORKPACKAGE WP-3: HHG and ultrafast electron imaging Coordinators: P. Salières (CEA), A. Assion (FEMTO, Spectra Physics Vienna) Period: Start Month 4 End Month 48 Leading Participants (Orange in the picture):
More information(DPHY 21) 1) a) Discuss the propagation of light in conducting surface. b) Discuss about the metallic reflection at oblique incidence.
(DPHY 21) ASSIGNMENT - 1, MAY - 2015. PAPER- V : ELECTROMAGNETIC THEORY AND MODERN OPTICS 1) a) Discuss the propagation of light in conducting surface. b) Discuss about the metallic reflection at oblique
More informationHigh Energy Channeling and the Experimental Search for the Internal Clock Predicted by L. de Broglie
Channeling 2014, Capri-Naples, Italy Joseph REMILLIEUX, IPNL, Lyon, France High Energy Channeling and the Experimental Search for the Internal Clock Predicted by L. de Broglie J. Remillieux 1, X. Artru
More informationChemistry Instrumental Analysis Lecture 3. Chem 4631
Chemistry 4631 Instrumental Analysis Lecture 3 Quantum Transitions The energy of a photon can also be transferred to an elementary particle by adsorption if the energy of the photon exactly matches the
More informationPhysics 107 Final Exam May 6, Your Name: 1. Questions
Physics 107 Final Exam May 6, 1996 Your Name: 1. Questions 1. 9. 17. 5.. 10. 18. 6. 3. 11. 19. 7. 4. 1. 0. 8. 5. 13. 1. 9. 6. 14.. 30. 7. 15. 3. 8. 16. 4.. Problems 1. 4. 7. 10. 13.. 5. 8. 11. 14. 3. 6.
More informationAcademic qualifications. Research experience. Research programs
Nicolas SISOURAT born 1981, september 7 Associate Professor e-mail: nicolas.sisourat@upmc.fr Tel. : 00 33 1 44 27 62 78 Fax. : 00 33 1 44 27 62 26 Laboratoire de Chimie Physique-Matière et Rayonnement
More informationX-Ray Photoelectron Spectroscopy (XPS)-2
X-Ray Photoelectron Spectroscopy (XPS)-2 Louis Scudiero http://www.wsu.edu/~pchemlab ; 5-2669 Fulmer 261A Electron Spectroscopy for Chemical Analysis (ESCA) The 3 step model: 1.Optical excitation 2.Transport
More informationSOFT X-RAYS AND EXTREME ULTRAVIOLET RADIATION
SOFT X-RAYS AND EXTREME ULTRAVIOLET RADIATION Principles and Applications DAVID ATTWOOD UNIVERSITY OF CALIFORNIA, BERKELEY AND LAWRENCE BERKELEY NATIONAL LABORATORY CAMBRIDGE UNIVERSITY PRESS Contents
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 informationConfining ultracold atoms on a ring in reduced dimensions
Confining ultracold atoms on a ring in reduced dimensions Hélène Perrin Laboratoire de physique des lasers, CNRS-Université Paris Nord Charge and heat dynamics in nano-systems Orsay, October 11, 2011 What
More informationLecture 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 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 informationFundamentals of Spectroscopy for Optical Remote Sensing. Course Outline 2009
Fundamentals of Spectroscopy for Optical Remote Sensing Course Outline 2009 Part I. Fundamentals of Quantum Mechanics Chapter 1. Concepts of Quantum and Experimental Facts 1.1. Blackbody Radiation and
More informationVibrational 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 informationEE 527 MICROFABRICATION. Lecture 5 Tai-Chang Chen University of Washington
EE 527 MICROFABRICATION Lecture 5 Tai-Chang Chen University of Washington MICROSCOPY AND VISUALIZATION Electron microscope, transmission electron microscope Resolution: atomic imaging Use: lattice spacing.
More informationS1. X-ray photoelectron spectroscopy (XPS) survey spectrum of
Site-selective local fluorination of graphene induced by focused ion beam irradiation Hu Li 1, Lakshya Daukiya 2, Soumyajyoti Haldar 3, Andreas Lindblad 4, Biplab Sanyal 3, Olle Eriksson 3, Dominique Aubel
More informationThe Use of Synchrotron Radiation in Modern Research
The Use of Synchrotron Radiation in Modern Research Physics Chemistry Structural Biology Materials Science Geochemical and Environmental Science Atoms, molecules, liquids, solids. Electronic and geometric
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 informationX-ray Magnetic Circular and Linear Dichroism (XMCD, XMLD) and X-ray Magnetic Imaging (PEEM,...)
X-ray Magnetic Circular and Linear Dichroism (XMCD, XMLD) and X-ray Magnetic Imaging (PEEM,...) Jan Vogel Institut Néel (CNRS, UJF), Nanoscience Department Grenoble, France - X-ray (Magnetic) Circular
More informationGraphene for THz technology
Graphene for THz technology J. Mangeney1, J. Maysonnave1, S. Huppert1, F. Wang1, S. Maero1, C. Berger2,3, W. de Heer2, T.B. Norris4, L.A. De Vaulchier1, S. Dhillon1, J. Tignon1 and R. Ferreira1 1 Laboratoire
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 informationCONTENTS. vii. CHAPTER 2 Operators 15
CHAPTER 1 Why Quantum Mechanics? 1 1.1 Newtonian Mechanics and Classical Electromagnetism 1 (a) Newtonian Mechanics 1 (b) Electromagnetism 2 1.2 Black Body Radiation 3 1.3 The Heat Capacity of Solids and
More informationCHAPTER 2 RADIATION INTERACTIONS WITH MATTER HDR 112 RADIATION BIOLOGY AND RADIATION PROTECTION MR KAMARUL AMIN BIN ABDULLAH
HDR 112 RADIATION BIOLOGY AND RADIATION PROTECTION CHAPTER 2 RADIATION INTERACTIONS WITH MATTER PREPARED BY: MR KAMARUL AMIN BIN ABDULLAH SCHOOL OF MEDICAL IMAGING FACULTY OF HEALTH SCIENCE Interactions
More informationRadiation Physics PHYS /251. Prof. Gocha Khelashvili
Radiation Physics PHYS 571-051/251 Prof. Gocha Khelashvili Interaction of Radiation with Matter: Heavy Charged Particles Directly and Indirectly Ionizing Radiation Classification of Indirectly Ionizing
More informationOverview: Attosecond optical technology based on recollision and gating
Overview: Attosecond optical technology based on recollision and gating Zenghu Chang Kansas State University Team members Kansas State University Zenghu Chang (Dept. of Phys.) Lew Cocke (Dept. of Phys.)
More informationConcepts in Surface Physics
M.-C. Desjonqueres D. Spanjaard Concepts in Surface Physics Second Edition With 257 Figures Springer 1. Introduction................................. 1 2. Thermodynamical and Statistical Properties of
More informationWeek 13. PHY 402 Atomic and Molecular Physics Instructor: Sebastian Wüster, IISERBhopal, Frontiers of Modern AMO physics. 5.
Week 13 PHY 402 Atomic and Molecular Physics Instructor: Sebastian Wüster, IISERBhopal,2018 These notes are provided for the students of the class above only. There is no warranty for correctness, please
More informationSUPPLEMENTARY INFORMATION
DOI: 1.138/NNANO.211.214 Control over topological insulator photocurrents with light polarization J.W. McIver*, D. Hsieh*, H. Steinberg, P. Jarillo-Herrero and N. Gedik SI I. Materials and device fabrication
More informationCHEMISTRY 110 EXAM 1 SEPTEMBER 20, 2010 FORM A
CHEMISTRY 110 EXAM 1 SEPTEMBER 20, 2010 FORM A 1. What are the correct numbers of protons, neutrons and electrons in a 39 K + ion? p n e A. 20 19 18 B. 20 19 19 C. 19 20 18 D. 19 20 19 E. 20 19 20 2. Which
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 informationPhotoelectron Peak Intensities in Solids
Photoelectron Peak Intensities in Solids Electronic structure of solids Photoelectron emission through solid Inelastic scattering Other excitations Intrinsic and extrinsic Shake-up, shake-down and shake-off
More informationSurfaces and Interfaces
1/16 Surfaces and Interfaces Fouad MAROUN Laboratoire de Physique de la Matière Condensée, Ecole Polytechnique CNRS Palaiseau, France 2/16 Outline Definition of surfaces and interfaces and 3 examples in
More informationPhysics of atoms and molecules
Physics of atoms and molecules 2nd edition B.H. Bransden and C.J. Joachain Prentice Hall An imprint of Pearson Education Harlow, England London New York Boston San Francisco Toronto Sydney Singapore Hong
More informationElectronic and Optoelectronic Properties of Semiconductor Structures
Electronic and Optoelectronic Properties of Semiconductor Structures Jasprit Singh University of Michigan, Ann Arbor CAMBRIDGE UNIVERSITY PRESS CONTENTS PREFACE INTRODUCTION xiii xiv 1.1 SURVEY OF ADVANCES
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 informationAstrophysics of Gaseous Nebulae and Active Galactic Nuclei
SECOND EDITION Astrophysics of Gaseous Nebulae and Active Galactic Nuclei Donald E. Osterbrock Lick Observatory, University of California, Santa Cruz Gary J. Ferland Department of Physics and Astronomy,
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 informationNuclear Physics. (PHY-231) Dr C. M. Cormack. Nuclear Physics This Lecture
Nuclear Physics (PHY-31) Dr C. M. Cormack 11 Nuclear Physics This Lecture This Lecture We will discuss an important effect in nuclear spectroscopy The Mössbauer Effect and its applications in technology
More informationIon traps. Trapping of charged particles in electromagnetic. Laser cooling, sympathetic cooling, optical clocks
Ion traps Trapping of charged particles in electromagnetic fields Dynamics of trapped ions Applications to nuclear physics and QED The Paul trap Laser cooling, sympathetic cooling, optical clocks Coulomb
More informationSpectroscopy. Practical Handbook of. J. W. Robinson, Ph.D., D.Sc, F.R.C.S. Department of Chemistry Louisiana State University Baton Rouge, Louisiana
Practical Handbook of Spectroscopy Edited by J. W. Robinson, Ph.D., D.Sc, F.R.C.S. Department of Chemistry Louisiana State University Baton Rouge, Louisiana CRC Press Boca Raton Ann Arbor Boston TABLE
More informationDEPARTMENT OF PHYSICS UNIVERSITY OF PUNE PUNE SYLLABUS for the M.Phil. (Physics ) Course
DEPARTMENT OF PHYSICS UNIVERSITY OF PUNE PUNE - 411007 SYLLABUS for the M.Phil. (Physics ) Course Each Student will be required to do 3 courses, out of which two are common courses. The third course syllabus
More informationPIs: Louis DiMauro & Pierre Agostini
Interaction of Clusters with Intense, Long Wavelength Fields PIs: Louis DiMauro & Pierre Agostini project objective: explore intense laser-cluster interactions in the strong-field limit project approach:
More informationBoltzmann Distribution
Boltzmann Distribution 0,4 N 0,3 0,2 T1 T2 T3 Τ 1 >Τ 2 >Τ 3 0,1 0,0 0 1 2 3 4 5 6 7 8 9 10 Energy Electronic transitions hν hν E 2 E 1 induced Absorption spontaneous Emission induced Emission Β 12 Α 21
More informationPhotoionized Gas Ionization Equilibrium
Photoionized Gas Ionization Equilibrium Ionization Recombination H nebulae - case A and B Strömgren spheres H + He nebulae Heavy elements, dielectronic recombination Ionization structure 1 Ionization Equilibrium
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 informationModeling interactions between a debris disc and planet: which initial conditions?
Modeling interactions between a debris disc and planet: which initial conditions? Elodie Thilliez @ET_astro Supervisors : Prof Sarah Maddison (Swinburne) Prof Jarrod Hurley (Swinburne) Crédit : NASA/JPL-Caltech
More informationAdvanced 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 informationConnecting Attosecond Science and XUV FEL Research
Connecting Attosecond Science and XUV FEL Research Marc Vrakking Attosecond Workshop Imperial College, May 13th 2008 Overview Present status of attosecond science - recent example: electron localization
More informationKey to Understanding Pre-Earthquake Phenomena
Stress-Activated Positive Hole Charge Carriers Key to Understanding Pre-Earthquake Phenomena Friedemann Freund friedemann.t.freund@nasa.gov Carl Sagan Center Physics Department NASA Ames Research Center
More informationX-Ray Spectro-Microscopy Joachim Stöhr Stanford Synchrotron Radiation Laboratory
X-Ray Spectro-Microscopy Joachim Stöhr Stanford Synchrotron Radiation Laboratory X-Rays have come a long way Application to Magnetic Systems 1 µm 1895 1993 2003 http://www-ssrl.slac.stanford.edu/stohr/index.htm
More informationNuclear Physics for Applications
Stanley C. Pruss'm Nuclear Physics for Applications A Model Approach BICENTENNIAL WILEY-VCH Verlag GmbH & Co. KGaA VII Table of Contents Preface XIII 1 Introduction 1 1.1 Low-Energy Nuclear Physics for
More informationInteraction of Ionizing Radiation with Matter
Type of radiation charged particles photonen neutronen Uncharged particles Charged particles electrons (β - ) He 2+ (α), H + (p) D + (d) Recoil nuclides Fission fragments Interaction of ionizing radiation
More informationX-Ray transitions to low lying empty states
X-Ray Spectra: - continuous part of the spectrum is due to decelerated electrons - the maximum frequency (minimum wavelength) of the photons generated is determined by the maximum kinetic energy of the
More informationQUANTUM WELLS, WIRES AND DOTS
QUANTUM WELLS, WIRES AND DOTS Theoretical and Computational Physics of Semiconductor Nanostructures Second Edition Paul Harrison The University of Leeds, UK /Cf}\WILEY~ ^INTERSCIENCE JOHN WILEY & SONS,
More informationAtomic Transitions and Selection Rules
Atomic Transitions and Selection Rules The time-dependent Schrodinger equation for an electron in an atom with a time-independent potential energy is ~ 2 2m r2 (~r, t )+V(~r ) (~r, t )=i~ @ @t We found
More informationChem 442 Review of Spectroscopy
Chem 44 Review of Spectroscopy General spectroscopy Wavelength (nm), frequency (s -1 ), wavenumber (cm -1 ) Frequency (s -1 ): n= c l Wavenumbers (cm -1 ): n =1 l Chart of photon energies and spectroscopies
More informationX-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