Laboratoire de Chimie Physique - Matière et Rayonnement Physical Chemistry Matter and Radiation Laboratory LCPMR - UMR 7614

Size: px
Start display at page:

Download "Laboratoire de Chimie Physique - Matière et Rayonnement Physical Chemistry Matter and Radiation Laboratory LCPMR - UMR 7614"

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 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 information

Probing Matter: Diffraction, Spectroscopy and Photoemission

Probing 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 information

Multi-electron coincidence spectroscopy: double photoionization from molecular inner-shell orbitals

Multi-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 information

Photoelectron spectroscopy Instrumentation. Nanomaterials characterization 2

Photoelectron 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 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

Lecture 3: Optical Properties of Insulators, Semiconductors, and Metals. 5 nm

Lecture 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 information

AMO at FLASH. FELs provide unique opportunities and challenges for AMO physics. due to essentially three reasons:

AMO 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 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

Electron Spectroscopy

Electron 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 information

Inelastic soft x-ray scattering, fluorescence and elastic radiation

Inelastic 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 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

ICPEAC 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 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 information

Attosecond laser systems and applications

Attosecond 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 information

Surface analysis techniques

Surface 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 information

Electron Spettroscopies

Electron 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 information

Nuclear Physics and Astrophysics

Nuclear 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 information

Joint ICTP-IAEA Workshop on Fusion Plasma Modelling using Atomic and Molecular Data January 2012

Joint 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 information

Energy Spectroscopy. Ex.: Fe/MgO

Energy 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 information

Elastic and Inelastic Scattering in Electron Diffraction and Imaging

Elastic 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 information

Introduction 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) 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 information

International Atomic Energy Agency, Vienna, Austria. Charge Transfer in Collisions of Ions with atoms and molecules.

International 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 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

X-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 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 information

Chapter VI: Ionizations and excitations

Chapter 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 information

X-ray Energy Spectroscopy (XES).

X-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 information

Laser-controlled Molecular Alignment and Orientation. Marc Vrakking FOM Institute AMOLF

Laser-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 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

Modeling cold collisions Atoms Molecules

Modeling 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 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

Topic 3: Periodic Trends and Atomic Spectroscopy

Topic 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 information

Lecture 10. Transition probabilities and photoelectric cross sections

Lecture 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 information

Methods of surface analysis

Methods 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 information

Study Plan for Ph.D in Physics (2011/2012)

Study 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 information

ATOMIC AND LASER SPECTROSCOPY

ATOMIC 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 information

New 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 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 information

Chemistry Instrumental Analysis Lecture 5. Chem 4631

Chemistry 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 information

Current Research and Future Plans

Current 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 information

X-Ray Photoelectron Spectroscopy (XPS)-2

X-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 information

Axion detection by atomic/molecular transitions

Axion 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 information

Review of Optical Properties of Materials

Review 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 information

Classification of spectroscopic methods

Classification 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 information

LECTURE 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 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 information

Laser induced manipulation of atom pair interaction

Laser 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 information

WP-3: HHG and ultrafast electron imaging

WP-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) 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 information

High Energy Channeling and the Experimental Search for the Internal Clock Predicted by L. de Broglie

High 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 information

Chemistry Instrumental Analysis Lecture 3. Chem 4631

Chemistry 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 information

Physics 107 Final Exam May 6, Your Name: 1. Questions

Physics 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 information

Academic qualifications. Research experience. Research programs

Academic 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 information

X-Ray Photoelectron Spectroscopy (XPS)-2

X-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 information

SOFT X-RAYS AND EXTREME ULTRAVIOLET RADIATION

SOFT 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 information

Fundamentals of Nanoscale Film Analysis

Fundamentals 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 information

Confining ultracold atoms on a ring in reduced dimensions

Confining 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 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

Studying Metal to Insulator Transitions in Solids using Synchrotron Radiation-based Spectroscopies.

Studying 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 information

Fundamentals of Spectroscopy for Optical Remote Sensing. Course Outline 2009

Fundamentals 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 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

EE 527 MICROFABRICATION. Lecture 5 Tai-Chang Chen University of Washington

EE 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 information

S1. X-ray photoelectron spectroscopy (XPS) survey spectrum of

S1. 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 information

The Use of Synchrotron Radiation in Modern Research

The 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 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

X-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,...) 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 information

Graphene for THz technology

Graphene 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 information

Core-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 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

CONTENTS. vii. CHAPTER 2 Operators 15

CONTENTS. 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 information

CHAPTER 2 RADIATION INTERACTIONS WITH MATTER HDR 112 RADIATION BIOLOGY AND RADIATION PROTECTION MR KAMARUL AMIN BIN ABDULLAH

CHAPTER 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 information

Radiation Physics PHYS /251. Prof. Gocha Khelashvili

Radiation 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 information

Overview: Attosecond optical technology based on recollision and gating

Overview: 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 information

Concepts in Surface Physics

Concepts 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 information

Week 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, 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 information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY 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 information

CHEMISTRY 110 EXAM 1 SEPTEMBER 20, 2010 FORM A

CHEMISTRY 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 information

MS482 Materials Characterization ( 재료분석 ) Lecture Note 5: RBS

MS482 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 information

Photoelectron Peak Intensities in Solids

Photoelectron 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 information

Surfaces and Interfaces

Surfaces 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 information

Physics of atoms and molecules

Physics 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 information

Electronic and Optoelectronic Properties of Semiconductor Structures

Electronic 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 information

X-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 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 information

Astrophysics of Gaseous Nebulae and Active Galactic Nuclei

Astrophysics 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 information

Energy Spectroscopy. Excitation by means of a probe

Energy 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 information

Nuclear Physics. (PHY-231) Dr C. M. Cormack. Nuclear Physics This Lecture

Nuclear 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 information

Ion traps. Trapping of charged particles in electromagnetic. Laser cooling, sympathetic cooling, optical clocks

Ion 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 information

Spectroscopy. Practical Handbook of. J. W. Robinson, Ph.D., D.Sc, F.R.C.S. Department of Chemistry Louisiana State University Baton Rouge, Louisiana

Spectroscopy. 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 information

DEPARTMENT OF PHYSICS UNIVERSITY OF PUNE PUNE SYLLABUS for the M.Phil. (Physics ) Course

DEPARTMENT 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 information

PIs: Louis DiMauro & Pierre Agostini

PIs: 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 information

Boltzmann Distribution

Boltzmann 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 information

Photoionized Gas Ionization Equilibrium

Photoionized 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 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

Modeling interactions between a debris disc and planet: which initial conditions?

Modeling 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 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

Connecting Attosecond Science and XUV FEL Research

Connecting 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 information

Key to Understanding Pre-Earthquake Phenomena

Key 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 information

X-Ray Spectro-Microscopy Joachim Stöhr Stanford Synchrotron Radiation Laboratory

X-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 information

Nuclear Physics for Applications

Nuclear 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 information

Interaction of Ionizing Radiation with Matter

Interaction 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 information

X-Ray transitions to low lying empty states

X-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 information

QUANTUM WELLS, WIRES AND DOTS

QUANTUM 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 information

Atomic Transitions and Selection Rules

Atomic 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 information

Chem 442 Review of Spectroscopy

Chem 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 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