X-Ray Scattering and Absorption by Magnetic Materials

Neutron 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

Nuclear and Particle Physics

Nuclear and Particle Physics W. S. С Williams Department of Physics, University of Oxford and St Edmund Hall, Oxford CLARENDON PRESS OXFORD 1991 Contents 1 Introduction 1.1 Historical perspective 1 1.2

Unit title: Atomic and Nuclear Physics for Spectroscopic Applications

Unit title: Atomic and Nuclear Physics for Spectroscopic Applications Unit code: Y/601/0417 QCF level: 4 Credit value: 15 Aim This unit provides an understanding of the underlying atomic and nuclear physics

Highenergy Nuclear Optics of Polarized Particles

Highenergy Nuclear Optics of Polarized Particles Vladimir G. Baryshevsky Research Institute for Nuclear Problems Belarusian State University 1> World Scientific NEW JERSEY LONDON SINGAPORE BEIJING SHANGHAI

SYNCHROTRON RADIATION DIFFRACTION STUDIES OF MAGNETIC MATERIALS

Vol. 91 (1997) ACTA PHYSICA POLONICA A No. 4 Proceedings of the 3rd ISSSRNS Jaszowiec '96 SYNCHROTRON RADIATION DIFFRACTION STUDIES OF MAGNETIC MATERIALS TH. BRUCKEL Hamburger Synchrotron-Strahlungslabor

Magnetic neutron diffraction. Rob McQueeney, Ames Laboratory and Iowa State University

Magnetic neutron diffraction Rob McQueeney, Ames Laboratory and Iowa State University September 19, 2018 Magnetic moment-rare earths Progressive filling of 4f levels Strong Hund s rules Strong spin-orbit

X-RAY MAGNETIC SCATTERING

Vol. 82 (1992) ACTA PHYSICA POLONICA A No 1 Proceedings of the ISSSRNS,92, Jaszowiec 1992 X-RAY MAGNETIC SCATTERING M.J. COOPER Department of Physics, University of Warwick, Coventry CV4 7AL, UK Magnetic

APPLIED PHYSICS 216 X-RAY AND VUV PHYSICS (Sept. Dec., 2006)

APPLIED PHYSICS 216 X-RAY AND VUV PHYSICS (Sept. Dec., 2006) Course Meeting: Monday, Wednesdays 11-12:15 Professor: Office Hours: Secretary: Mid Term: Final Exam: Another Course: Zhi-Xun Shen McCullough

Reflection = EM strikes a boundary between two media differing in η and bounces back

Reflection = EM strikes a boundary between two media differing in η and bounces back Incident ray θ 1 θ 2 Reflected ray Medium 1 (air) η = 1.00 Medium 2 (glass) η = 1.50 Specular reflection = situation

Quantum Physics in the Nanoworld

Hans Lüth Quantum Physics in the Nanoworld Schrödinger's Cat and the Dwarfs 4) Springer Contents 1 Introduction 1 1.1 General and Historical Remarks 1 1.2 Importance for Science and Technology 3 1.3 Philosophical

Theory and Experiment

Theory and Experiment Mark Beck OXPORD UNIVERSITY PRESS Contents Table of Symbols Preface xiii xix 1 MATHEMATICAL PRELIMINARIES 3 1.1 Probability and Statistics 3 1.2 LinearAlgebra 9 1.3 References 17

Physics 126 Practice Exam #4 Professor Siegel

Physics 126 Practice Exam #4 Professor Siegel Name: Lab Day: 1. Light is usually thought of as wave-like in nature and electrons as particle-like. In which one of the following instances does light behave

Simo Huotari University of Helsinki, Finland TDDFT school, Benasque, Spain, January 2012

Overview of spectroscopies III Simo Huotari University of Helsinki, Finland TDDFT school, Benasque, Spain, January 2012 Motivation: why we need theory Spectroscopy (electron dynamics) Theory of electronic

Soft 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

Magnetic X-rays versus Neutrons

Magnetic X-rays versus Neutrons what can we learn from scattering experiments when studying magnetism? which probe to use to solve a given problem? neutrons or synchrotron x-rays? problems to be solved

The Oxford Solid State Basics

The Oxford Solid State Basics Steven H. Simon University of Oxford OXFORD UNIVERSITY PRESS Contents 1 About Condensed Matter Physics 1 1.1 What Is Condensed Matter Physics 1 1.2 Why Do We Study Condensed

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

THE NATURE OF THE ATOM. alpha particle source

chapter THE NATURE OF THE ATOM www.tutor-homework.com (for tutoring, homework help, or help with online classes) Section 30.1 Rutherford Scattering and the Nuclear Atom 1. Which model of atomic structure

Discovery of the Atomic Nucleus. Conceptual Physics 11 th Edition. Discovery of the Electron. Discovery of the Atomic Nucleus

Conceptual Physics 11 th Edition Chapter 32: THE ATOM AND THE QUANTUM Discovery of the Atomic Nucleus These alpha particles must have hit something relatively massive but what? Rutherford reasoned that

SOLID STATE PHYSICS. Second Edition. John Wiley & Sons. J. R. Hook H. E. Hall. Department of Physics, University of Manchester

SOLID STATE PHYSICS Second Edition J. R. Hook H. E. Hall Department of Physics, University of Manchester John Wiley & Sons CHICHESTER NEW YORK BRISBANE TORONTO SINGAPORE Contents Flow diagram Inside front

Harald Ibach Hans Lüth SOLID-STATE PHYSICS. An Introduction to Theory and Experiment

Harald Ibach Hans Lüth SOLID-STATE PHYSICS An Introduction to Theory and Experiment With 230 Figures Springer-Verlag Berlin Heidelberg New York London Paris Tokyo Hong Kong Barcelona Budapest Contents

The Photoelectric Effect

The Photoelectric Effect Light can strike the surface of some metals causing an electron to be ejected No matter how brightly the light shines, electrons are ejected only if the light has sufficient energy

12 주 /15 주 작은구멍이나장애물을만나면넘어가거나돌아간다. 원거리에돌이 ( 프라운호퍼에돌이 ) 에돌이 ( 회절 )- 불확정성의원리 근거리에돌이 ( 프레스넬에돌이 )

12 주 /15 주 작은구멍이나장애물을만나면넘어가거나돌아간다. 원거리에돌이 ( 프라운호퍼에돌이 ) 에돌이 ( 회절 )- 불확정성의원리 근거리에돌이 ( 프레스넬에돌이 ) 2014-12-17 1 현대물리 : 광학 5 장 Diffraction 목포해양대학교기관공학부 김상훈 2014-12-17 2 2014-12-17 3 2014-12-17 4 2014-12-17 5

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,

Name : Roll No. :.... Invigilator s Signature :.. CS/B.Tech (NEW)/SEM-2/PH-201/2013 2013 PHYSICS - I Time Allotted : 3 Hours Full Marks : 70 The figures in the margin indicate full marks. Candidates are

Photoelectron Spectroscopy

Stefan Hüfner Photoelectron Spectroscopy Principles and Applications Third Revised and Enlarged Edition With 461 Figures and 28 Tables JSJ Springer ... 1. Introduction and Basic Principles 1 1.1 Historical

An 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

Magnetic x-ray microdiffraction

INSTITUTE OF PHYSICS PUBLISHING JOURNAL OF PHYSICS D: APPLIED PHYSICS J. Phys. D: Appl. Phys. 39 (2006) R245 R263 doi:10.1088/0022-3727/39/15/r01 TOPICAL REVIEW Magnetic x-ray microdiffraction Paul G Evans

Lecture 6 - Atomic Structure. Chem 103, Section F0F Unit II - Quantum Theory and Atomic Structure Lecture 6. Lecture 6 - Introduction

Chem 103, Section F0F Unit II - Quantum Theory and Atomic Structure Lecture 6 Light and other forms of electromagnetic radiation Light interacting with matter The properties of light and matter Lecture

MODERN PHYSICS Frank J. Blatt Professor of Physics, University of Vermont

MODERN PHYSICS Frank J. Blatt Professor of Physics, University of Vermont McGRAW-HILL, INC. New York St. Louis San Francisco Auckland Bogota Caracas Lisbon London Madrid Mexico Milan Montreal New Delhi

Chapter 27 Early Quantum Theory and Models of the Atom Discovery and Properties of the electron

Chapter 27 Early Quantum Theory and Models of the Atom 27-1 Discovery and Properties of the electron Measure charge to mass ratio e/m (J. J. Thomson, 1897) When apply magnetic field only, the rays are

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

Name : Roll No. :.. Invigilator s Signature :.. CS/B.Tech/SEM-2/PH-201/2010 2010 ENGINEERING PHYSICS Time Allotted : 3 Hours Full Marks : 70 The figures in the margin indicate full marks. Candidates are

Making 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

11 Magnetic X-Ray and Polarised Neutron Scattering

11 Magnetic X-Ray and Polarised Neutron Scattering Th. Brückel Forschungszentrum Jülich GmbH, Institut für Festkörperforschung, 52425 JÜLICH, GERMANY Abstract. Since the advent of high brilliance synchrotron

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

Quantum dynamics in many body systems

Quantum dynamics in many body systems Eugene Demler Harvard University Collaborators: David Benjamin (Harvard), Israel Klich (U. Virginia), D. Abanin (Perimeter), K. Agarwal (Harvard), E. Dalla Torre (Harvard)

Unified School District of De Pere Physics Benchmarks

Content Standards: A. Students will understand that among the science disciplines, there are unifying themes: systems, order, organization, and interactions; evidence, models, and explanations; constancy,

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

DIFFRACTION PHYSICS THIRD REVISED EDITION JOHN M. COWLEY. Regents' Professor enzeritus Arizona State University

DIFFRACTION PHYSICS THIRD REVISED EDITION JOHN M. COWLEY Regents' Professor enzeritus Arizona State University 1995 ELSEVIER Amsterdam Lausanne New York Oxford Shannon Tokyo CONTENTS Preface to the first

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,

Polarization tunability and analysis for observing magnetic effects on BL39XU at SPring-8

1133 J. Synchrotron Rad. (1999). 6, 1133±1137 Polarization tunability and analysis for observing magnetic effects on BL39XU at SPring-8 H. Maruyama, a * M. Suzuki, b N. Kawamura, c M. Ito, d E. Arakawa,

4. Circular Dichroism - Spectroscopy

4. Circular Dichroism - Spectroscopy The optical rotatory dispersion (ORD) and the circular dichroism (CD) are special variations of absorption spectroscopy in the UV and VIS region of the spectrum. The

Electronic Spectra of Complexes

Electronic Spectra of Complexes Interpret electronic spectra of coordination compounds Correlate with bonding Orbital filling and electronic transitions Electron-electron repulsion Application of MO theory

A Brief Introduction to Medical Imaging. Outline

A Brief Introduction to Medical Imaging Outline General Goals Linear Imaging Systems An Example, The Pin Hole Camera Radiations and Their Interactions with Matter Coherent vs. Incoherent Imaging Length

Roll No. :... Invigilator's Signature :.. CS/B.TECH(N)/SEM-1/PH-101/ PHYSICS - I. Time Allotted : 3 Hours Full Marks : 70

Name : Roll No. :.... Invigilator's Signature :.. CS/B.TECH(N)/SEM-1/PH-101/2012-13 2012 PHYSICS - I Time Allotted : 3 Hours Full Marks : 70 The figures in the margin indicate full marks. Candidates are

Matter-Radiation Interaction

Matter-Radiation Interaction The purpose: 1) To give a description of the process of interaction in terms of the electronic structure of the system (atoms, molecules, solids, liquid or amorphous samples).

Neutron Diffraction: a general overview

RUG1 Neutron Diffraction: a general overview Graeme Blake Zernike Institute for Advanced Materials University of Groningen Outline Elastic scattering of neutrons from matter Comparison of neutron and X-ray

Magnetism in Condensed Matter

Magnetism in Condensed Matter STEPHEN BLUNDELL Department of Physics University of Oxford OXFORD 'UNIVERSITY PRESS Contents 1 Introduction 1.1 Magnetic moments 1 1 1.1.1 Magnetic moments and angular momentum

MIDTERM 3 REVIEW SESSION. Dr. Flera Rizatdinova

MIDTERM 3 REVIEW SESSION Dr. Flera Rizatdinova Summary of Chapter 23 Index of refraction: Angle of reflection equals angle of incidence Plane mirror: image is virtual, upright, and the same size as the

PMARIZED LI6HT FUNDAMENTALS AND APPLICATIONS EBWABD COLLETT. Measurement Concepts, Inc. Colts Neck, New Jersey

PMARIZED LI6HT FUNDAMENTALS AND APPLICATIONS EBWABD COLLETT Measurement Concepts, Inc. Colts Neck, New Jersey Marcel Dekker, Inc. New York Basel Hong Kong About the Series Preface A Historical Note iii

MOLECULAR SPECTROSCOPY

MOLECULAR SPECTROSCOPY First Edition Jeanne L. McHale University of Idaho PRENTICE HALL, Upper Saddle River, New Jersey 07458 CONTENTS PREFACE xiii 1 INTRODUCTION AND REVIEW 1 1.1 Historical Perspective

Radiochemistry and Nuclear Methods of Analysis

Radiochemistry and Nuclear Methods of Analysis WILLIAM D. EHMANN Professor, Department of Chemistry University of Kentucky Lexington, Kentucky DIANE E. VANCE Staff Development Scientist Analytical Services

Neutron Instruments I & II. Ken Andersen ESS Instruments Division

Neutron Instruments I & II ESS Instruments Division Neutron Instruments I & II Overview of source characteristics Bragg s Law Elastic scattering: diffractometers Continuous sources Pulsed sources Inelastic

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

Quantum and Atomic Physics - Multiple Choice

PSI AP Physics 2 Name 1. The Cathode Ray Tube experiment is associated with: (A) J. J. Thomson (B) J. S. Townsend (C) M. Plank (D) A. H. Compton 2. The electron charge was measured the first time in: (A)

Drickamer 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

DUAL NATURE OF RADIATION AND MATTER

Chapter Eleven DUAL NATURE OF RADIATION AND MATTER MCQ I 111 A particle is dropped from a height H The de Broglie wavelength of the particle as a function of height is proportional to (a) H (b) H 1/2 (c)

SECTION A Quantum Physics and Atom Models

AP Physics Multiple Choice Practice Modern Physics SECTION A Quantum Physics and Atom Models 1. Light of a single frequency falls on a photoelectric material but no electrons are emitted. Electrons may

12/04/2012. Models of the Atom. Quantum Physics versus Classical Physics The Thirty-Year War ( )

Quantum Physics versus Classical Physics The Thirty-Year War (1900-1930) Interactions between Matter and Radiation Models of the Atom Bohr s Model of the Atom Planck s Blackbody Radiation Models of the

Contents. Preface to the First Edition Preface to the Second Edition

Contents Preface to the First Edition Preface to the Second Edition Notes xiii xv xvii 1 Basic Concepts 1 1.1 History 1 1.1.1 The Origins of Nuclear Physics 1 1.1.2 The Emergence of Particle Physics: the

Magnetic neutron diffraction

Magnetic neutron diffraction Rob McQueeney Physics 590 1 Magnetic moment-rare earths Progressive filling of 4f levels Strong Hund s rules Strong spin-orbit interaction Weak CEF Unpaired electrons Total

Particles and Waves Particles Waves

Particles and Waves Particles Discrete and occupy space Exist in only one location at a time Position and velocity can be determined with infinite accuracy Interact by collisions, scattering. Waves Extended,

Magnetic X-Ray Scattering: An Introduction and Applications of Non-Resonant Magnetic Photon Diffraction

Magnetic X-Ray Scattering: An Introduction and Applications of Non-Resonant Magnetic Photon Diffraction Th. Brückel Forschungszentrum Jülich GmbH, Institut für Festkörperforschung, 545 JÜLICH, GERMANY

Skoog Chapter 6 Introduction to Spectrometric Methods

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

Unit 11 Instrumentation. Mass, Infrared and NMR Spectroscopy

Unit 11 Instrumentation Mass, Infrared and NMR Spectroscopy Spectroscopic identification of organic compounds Qualitative analysis: presence but not quantity (i.e. PEDs) Quantitative analysis: quantity

Name :. Roll No. :... Invigilator s Signature :.. CS/B. Tech (New)/SEM-1/PH-101/ PHYSICS-I

Name :. Roll No. :..... Invigilator s Signature :.. CS/B. Tech (New)/SEM-1/PH-101/2011-12 2011 PHYSICS-I Time Allotted : 3 Hours Full Marks : 70 The figures in the margin indicate full marks. Candidates

Practical Quantum Mechanics

Siegfried Flügge Practical Quantum Mechanics With 78 Figures Springer-Verlag Berlin Heidelberg New York London Paris Tokyo Hong Kong Barcelona Budapest Contents Volume I I. General Concepts 1. Law of probability

PRINCIPLES OF NONLINEAR OPTICAL SPECTROSCOPY

PRINCIPLES OF NONLINEAR OPTICAL SPECTROSCOPY Shaul Mukamel University of Rochester Rochester, New York New York Oxford OXFORD UNIVERSITY PRESS 1995 Contents 1. Introduction 3 Linear versus Nonlinear Spectroscopy

Planck s Quantum Hypothesis Blackbody Radiation

Planck s Quantum Hypothesis Blackbody Radiation The spectrum of blackbody radiation has been measured(next slide); it is found that the frequency of peak intensity increases linearly with temperature.

Chapter 6 Electronic Structure of Atoms

Chapter 6 Electronic Structure of Atoms What is the origin of color in matter? Demo: flame tests What does this have to do with the atom? Why are atomic properties periodic? 6.1 The Wave Nature of Light

Transmission 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

Crystals, X-rays and Proteins

Crystals, X-rays and Proteins Comprehensive Protein Crystallography Dennis Sherwood MA (Hons), MPhil, PhD Jon Cooper BA (Hons), PhD OXFORD UNIVERSITY PRESS Contents List of symbols xiv PART I FUNDAMENTALS

O WILEY- MODERN NUCLEAR CHEMISTRY. WALTER D. LOVELAND Oregon State University. DAVID J. MORRISSEY Michigan State University

MODERN NUCLEAR CHEMISTRY WALTER D. LOVELAND Oregon State University DAVID J. MORRISSEY Michigan State University GLENN T. SEABORG University of California, Berkeley O WILEY- INTERSCIENCE A JOHN WILEY &

Electronic structure of atoms

Chapter 1 Electronic structure of atoms light photons spectra Heisenberg s uncertainty principle atomic orbitals electron configurations the periodic table 1.1 The wave nature of light Much of our understanding

1 The Cathode Rays experiment is associated. with: Millikan A B. Thomson. Townsend. Plank Compton

1 The Cathode Rays experiment is associated with: A B C D E Millikan Thomson Townsend Plank Compton 1 2 The electron charge was measured the first time in: A B C D E Cathode ray experiment Photoelectric

1. 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

Laboratory Manual 1.0.6

Laboratory Manual 1.0.6 Background What is X-ray Diffraction? X-rays scatter off of electrons, in a process of absorption and re-admission. Diffraction is the accumulative result of the x-ray scattering

Modern Optical Spectroscopy

Modern Optical Spectroscopy With Exercises and Examples from Biophysics and Biochemistry von William W Parson 1. Auflage Springer-Verlag Berlin Heidelberg 2006 Verlag C.H. Beck im Internet: www.beck.de

Solid State Physics. GIUSEPPE GROSSO Professor of Solid State Physics, Department of Physics, University of Pavia, and INFM

Solid State Physics GIUSEPPE GROSSO Professor of Solid State Physics, Department of Physics, University of Pisa, and INFM GIUSEPPE PASTORI PARRAVICINI Professor of Solid State Physics, Department of Physics,

CHAPTER I Review of Modern Physics. A. Review of Important Experiments

CHAPTER I Review of Modern Physics A. Review of Important Experiments Quantum Mechanics is analogous to Newtonian Mechanics in that it is basically a system of rules which describe what happens at the

Neutron scattering from quantum materials

Neutron scattering from quantum materials Bernhard Keimer Max Planck Institute for Solid State Research Max Planck UBC UTokyo Center for Quantum Materials Detection of bosonic elementary excitations in

4/14/2015. Models of the Atom. Quantum Physics versus Classical Physics The Thirty-Year War ( ) Classical Model of Atom

Quantum Physics versus Classical Physics The Thirty-Year War (1900-1930) Models of the Atom Interactions between Matter and Radiation Models of the Atom Bohr s Model of the Atom Planck s Blackbody Radiation

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

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

Compton Source of Twisted Photons

Compton Source of Twisted Photons Andrei Afanasev The George Washington University Washington, DC LDRS 2015 International Meeting on Laser-Driven Radiation Sources for Nuclear Applications George Washington

Chap. 3. Elementary Quantum Physics

Chap. 3. Elementary Quantum Physics 3.1 Photons - Light: e.m "waves" - interference, diffraction, refraction, reflection with y E y Velocity = c Direction of Propagation z B z Fig. 3.1: The classical view

ACTIVE GALACTIC NUCLEI: FROM THE CENTRAL BLACK HOLE TO THE GALACTIC ENVIRONMENT

Julian H. Krolik ACTIVE GALACTIC NUCLEI: FROM THE CENTRAL BLACK HOLE TO THE GALACTIC ENVIRONMENT PRINCETON UNIVERSITY PRESS Princeton, New Jersey Preface Guide for Readers xv xix 1. What Are Active Galactic

Physical Electronics. First class (1)

Physical Electronics First class (1) Bohr s Model Why don t the electrons fall into the nucleus? Move like planets around the sun. In circular orbits at different levels. Amounts of energy separate one

Chapter 4 Section 2 Notes

Chapter 4 Section 2 Notes Vocabulary Heisenberg Uncertainty Principle- states that it is impossible to determine simultaneously both the position and velocity of an electron or any other particle. Quantum

X-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

Chapter 8 Magnetic Resonance

Chapter 8 Magnetic Resonance 9.1 Electron paramagnetic resonance 9.2 Ferromagnetic resonance 9.3 Nuclear magnetic resonance 9.4 Other resonance methods TCD March 2007 1 A resonance experiment involves

Characterizations and Diagnostics of Compton Light Source

Characterizations and Diagnostics of Compton Light Source Advance Light Source (ALS) (LBNL) Ying K. Wu Duke Free Electron Laser Laboratory (DFELL) Acknowledgments: DFELL: B. Jia, G. Swift, H. Hao, J. Li,

INTRODUCTION TO SCA\ \I\G TUNNELING MICROSCOPY

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

CHEMISTRY Topic #1: Atomic Structure and Nuclear Chemistry Fall 2017 Dr. Susan Findlay See Exercises 3.1 to 3.3

CHEMISTRY 1000 Topic #1: Atomic Structure and Nuclear Chemistry Fall 2017 Dr. Susan Findlay See Exercises 3.1 to 3.3 Light: Wave? Particle? Both! Modern models of the atom were derived by studying the

Chapter 6 - Electronic Structure of Atoms

Chapter 6 - Electronic Structure of Atoms 6.1 The Wave Nature of Light To understand the electronic structure of atoms, one must understand the nature of electromagnetic radiation Visible light is an example

X-ray non-resonant and resonant magnetic scattering Laurent C. Chapon, Diamond Light Source. European School on Magnetism L. C.

X-ray non-resonant and resonant magnetic scattering Laurent C. Chapon, Diamond Light Source 1 The Diamond synchrotron 3 GeV, 300 ma Lienard-Wiechert potentials n.b: Use S.I units throughout. rq : position

WAVE NATURE OF LIGHT

WAVE NATURE OF LIGHT Light is electromagnetic radiation, a type of energy composed of oscillating electric and magnetic fields. The fields oscillate perpendicular to each other. In vacuum, these waves

Wave Nature of Matter

Wave Nature of Matter Wave-Particle Duality de Broglie proposed that particles with momentum could have an associated wavelength (converse of photons having momentum) de Broglie wavelength h λ = p or p

QUANTUM MECHANICS. Franz Schwabl. Translated by Ronald Kates. ff Springer

Franz Schwabl QUANTUM MECHANICS Translated by Ronald Kates Second Revised Edition With 122Figures, 16Tables, Numerous Worked Examples, and 126 Problems ff Springer Contents 1. Historical and Experimental

Chapter 7: The Quantum-Mechanical Model of the Atom

C h e m i s t r y 1 A : C h a p t e r 7 P a g e 1 Chapter 7: The Quantum-Mechanical Model of the Atom Homework: Read Chapter 7. Work out sample/practice exercises Check for the MasteringChemistry.com assignment