Neutron scattering. Niina Jalarvo. SMN/FERMiO, Department of Chemistry, University of Oslo Gaustadalleen 21 NO-0349 Oslo, Norway UNIVERSITY OF OSLO
|
|
- Priscilla Welch
- 6 years ago
- Views:
Transcription
1 Neutron scattering Niina Jalarvo SMN/FERMiO, Department of Chemistry, University of Oslo Gaustadalleen 21 NO-0349 Oslo, Norway UNIVERSITY OF OSLO
2 NEUTRON what is it? Neutrons are particles found in the atomic nuclei Mass No elecric charge! Spin m = 1675, 10 h s = 2 Lifetime about 20 min 24 g As all quantum particles, also neutrons, can exhibit wave phenomena. Due to the de Broglie relation 2 λ = v π = k h r p
3 Why Neutrons? Neutrons interact directly with the nuclei of the atoms strong but very short ranged nuclear interaction no electrostatic interaction (overall interaction is weak) => neutrons easily penetrate sample materials Most of other techniques for diffraction or inelastic scattering are based on interaction with the electron cloud surrounding each atom. difficulties to observe light elements in diffraction selection rules of observable modes for scattering
4 Why Neutrons? Neutron scattering is a very powerful tool to probe microscopic dynamical and geometrical properties of condensed matter. Especially dynamical processes of species containing hydrogen and structural properties of materials containing light elements, e.g. hydrogen (deuterium) or oxygen Nobel Prize in Physics was given to Brockhouse, for the development of neutron spectroscopy and to Shull, for the development of the neutron diffraction technique
5 Producing neutrons A neutron scattering measurement requires a neutron source (e.g. a nuclear reactor or spallation source). Research reactors in Europe: IFE, Kjeller, Norway ILL, Grenoble, France BENSC, Berlin, Germany FRM II, Munich, Germany LLB, Saclay, France Spallation Sources in Europe: ISIS, Oxfordshire, U.K. PSI, Zurich, Switzerland ESS,???,
6 Obtaining the desired wavelengths
7 Wavelength ~ Å s comparable to interatomic and intermolecular distances Energy ~ mev s comparable to the time scale of many motions in materials => vibrations, librations, reorientations, diffusion, and relaxational processes can be observed Problems: too low flux of neutrons long measuring times needed large amount of sample needed (normally hundreds or thousands of mg)
8 Interactions The neutron-nucleus interaction is described by a scattering cross section The scattering cross section varies randomly from isotope to isotope Cross section (σ) - Area related to the probability that a neutron will interact with a nucleus in a particular way (e.g. scattering or absorption) For systems containing a reasonable proportion of H atoms, scattering from H tends to dominate For a single nucleus σ cm 2 (unit barn) Relative total scattering cross sections for few isotopes
9 Structure and Dynamics Not all nuclei in a sample consisting of only one element or even only isotope necessarily scatter identically => RANDOMNESS If the scattered neutron waves from the different nuclei have RANDOM relative phases, they don t interfere => INCOHERENT SCATTERING If the scattered neutron waves from the different nuclei have definite relative phases, they can interfere => COHERENT SCATTERING DYNAMICS STRUCTURE
10 Structure and Dynamics Different atoms and isotopes have different coherent and incoherent scattering cross sections Element σ coh (barns) σ inc (barns) Hydrogen (H) Deuterium (D) Carbon (C) Oxygen (O) Deuterated sample for coherent Bragg diffraction to obtain structure Protonated to observe both single particle motion (quasielastic) and to weight the inelastic scattering spectrum in favor of hydrogen (vibrations) Deuteration can help to assign dynamics of particular groups
11 Scattering Kinematics The collision of two objects can be described in terms of momentum conservation and, in some cases, energy conservation. Neutron scattering events are described by means of energy and momentum transfer. r hq = hω = r r hk 1 hk 0 E1 E 0 hω = hω hω ELASTIC scattering INELASTIC scattering QUASIELASTIC scattering
12 If you want to study the structure of your hydrated oxide by neutrons a) Would you use elastic or inelastic neutron scattering? b) Would you prefer to deuterate your sample or not? Why? c) Which wavelength would you choose? Why?
13 Dynamics and Neutron Scattering The dynamics of a system reflect the interatomic and intermolecular interactions which are responsible for the properties of materials Neutron Scattering is an excellent way to study dynamics Measure the number of scattered neutrons as a function of Q and ω => S(Q,ω) (the scattering function) depends ONLY on the sample
14
15 FANS DCS Backscattering Spin Echo Itinerant Magnets Spin Waves Heavy Fermions Critical Scattering Hydrogen Modes Molecular Vibrations Lattice Vibrations Molecular Rotations Diffusion Tunneling Polymers and Spectroscopy Biological Systems Relaxations in Glasses
16
17
18
19
20 References and literature G. H. Lander: The Neutron - an introduction (lecture on Web) D. Neumann: Dynamics and Neutron Scattering (lecture on Web) G. L. Squires: Introduction to the Theory of Thermal Neutron Scattering, S. W. Lovesey: Theory of Neutron Scattering from Condensed Matter
Small Angle Neutron Scattering in Different Fields of Research. Henrich Frielinghaus
Small Angle Neutron Scattering in Different Fields of Research Henrich Frielinghaus Jülich Centre for Neutron Science Forschungszentrum Jülich GmbH Lichtenbergstrasse 1 85747 Garching (München) h.frielinghaus@fz-juelich.de
More informationPart I. Basics of neutron scattering
Part I Basics of neutron scattering 13 Chapter 1 Introduction to neutron scattering Neutron scattering is one of the most powerful and versatile experimental methods to study the structure and dynamics
More informationThe Institute Laue Langevin (ILL) and its pioneering user system
The Institute Laue Langevin (ILL) and its pioneering user system B. Farago (Head of the TOF-HR Instrument Group ILL) Based on the talk of W.G. Stirling Director of the ILL EC JRC Brussels 29/01/2015 Examples
More informationDelft in Europe. Neutron & Positrons Oyster & the World
Delft in Europe Neutron & Positrons Oyster & the World where are we? Oyster - HOR Neutrons and Positrons European Spallation Source where are we? Oyster - HOR Neutrons and Positrons European Spallation
More informationIntroduction to Neutron Scattering
Introduction to Neutron Scattering Name: Guorong Li Email: gli6@utk.edu Solid State II, Spring 2008 Instructor: Elbio Dagotto Department of Physics University of Tennessee Introduction to Neutron Scattering
More informationIntroduction to Triple Axis Neutron Spectroscopy
Introduction to Triple Axis Neutron Spectroscopy Bruce D Gaulin McMaster University The triple axis spectrometer Constant-Q and constant E Practical concerns Resolution and Spurions Neutron interactions
More informationScattering Lecture. February 24, 2014
Scattering Lecture February 24, 2014 Structure Determination by Scattering Waves of radiation scattered by different objects interfere to give rise to an observable pattern! The wavelength needs to close
More informationNeutron scattering from Skyrmions in helimagnets. Jonas Kindervater
Neutron scattering from Skyrmions in helimagnets Jonas Kindervater Collaborations TU München - E21 A. Bauer F. Rucker S. Säubert F. Haslbeck G. Benka P. Schmakat G. Brandl A. Chacon P. Böni C. Pfleiderer
More informationReactor & Spallation Neutron Sources
Reactor & Spallation Neutron Sources Oxford School of Neutron Scattering Oxford, 2011-09-06 Ken Andersen ESS Instruments Division ISIS ILL Time evolution: Major neutron sources ILL BENSC (D) SINQ (CH)
More information1.1 Properties of thermal neutrons
1 Introduction In this introductory chapter we discuss some of the properties of the neutron and how it interacts with matter. We compare steady-state reactors to pulsed spallation neutron sources. After
More informationPutting Neutron Scattering into Perspective
Putting Neutron Scattering into Perspective H. Schober Institut Laue-Langevin, F-38042 Grenoble, France August 31, 2003 1 Introduction Whenever it is important to know precisely where atoms are or how
More informationNeutron and x-ray spectroscopy
Neutron and x-ray spectroscopy B. Keimer Max-Planck-Institute for Solid State Research outline 1. self-contained introduction neutron scattering and spectroscopy x-ray scattering and spectroscopy 2. application
More informationNeutron Interactions with Matter
Radioactivity - Radionuclides - Radiation 8 th Multi-Media Training Course with Nuclides.net (Institute Josžef Stefan, Ljubljana, 13th - 15th September 2006) Thursday, 14 th September 2006 Neutron Interactions
More informationExercise 1 Atomic line spectra 1/9
Exercise 1 Atomic line spectra 1/9 The energy-level scheme for the hypothetical one-electron element Juliettium is shown in the figure on the left. The potential energy is taken to be zero for an electron
More informationNeutron facilities and generation. Rob McQueeney, Ames Laboratory and Iowa State University
Neutron facilities and generation Rob McQueeney, Ames Laboratory and Iowa State University September 12, 2018 19-Sep-18 Physics 502 2 Neutrons compared to other probes of matter Bulk probe Interacts with
More informationNeutron Scattering: Theory, Instrumentation, and Simulation
Neutron Scattering: Theory, Instrumentation, and Simulation Kim Lefmann Department of Materials Research Risø National Laboratory Technical University of Denmark August 25, 2007 2 Foreword and acknowledgements
More informationNeutron 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
More informationNeutron 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
More informationChapter V: Interactions of neutrons with matter
Chapter V: Interactions of neutrons with matter 1 Content of the chapter Introduction Interaction processes Interaction cross sections Moderation and neutrons path For more details see «Physique des Réacteurs
More informationNeutrons as probe particles V pseudo Fermi
Neutrons as probe particles V pseudo Fermi Nuclear interaction range (~10-13 cm) b r R b ~ 510 13 cm 510 thermal neutrons 5 A E ~ 5 mev for thermal neutrons ~ Å for thermal neutrons b Penetration depth
More informationIntroduction to Neutron Scattering
Introduction to Neutron Scattering J.T.Haraldsen Department of Physics and Astronomy, University of Tennessee, Knoxville, TN 37996 Neutron scattering is a powerful and direct means for investigating the
More informationNeutron Scattering of Magnetic excitations
Neutron Scattering of Magnetic excitations Magnetic excitations, magnons, and spin chains by Ibrahima Diallo Technische Universität Muenchen Outline Properties of the Neutron Spin, spin waves, and magnons
More informationNeutron Sources Fall, 2017 Kyoung-Jae Chung Department of Nuclear Engineering Seoul National University
Neutron Sources Fall, 2017 Kyoung-Jae Chung Department of Nuclear Engineering Seoul National University Neutrons: discovery In 1920, Rutherford postulated that there were neutral, massive particles in
More information22.54 Neutron Interactions and Applications (Spring 2004) Chapter 1 (2/3/04) Overview -- Interactions, Distributions, Cross Sections, Applications
.54 Neutron Interactions and Applications (Spring 004) Chapter 1 (/3/04) Overview -- Interactions, Distributions, Cross Sections, Applications There are many references in the vast literature on nuclear
More information6 Neutrons and Neutron Interactions
6 Neutrons and Neutron Interactions A nuclear reactor will not operate without neutrons. Neutrons induce the fission reaction, which produces the heat in CANDU reactors, and fission creates more neutrons.
More informationNeutron Scattering in Soft Matter Research: From Biology to Chemistry. Henrich Frielinghaus
Neutron Scattering in Soft Matter Research: From Biology to Chemistry Henrich Frielinghaus Jülich Centre for Neutron Science Forschungszentrum Jülich GmbH Lichtenbergstrasse 1 85747 Garching (München)
More informationGood Vibrations Studying phonons with momentum resolved spectroscopy. D.J. Voneshen 20/6/2018
Good Vibrations Studying phonons with momentum resolved spectroscopy D.J. Voneshen 20/6/2018 Overview What probe to use? Types of instruments. Single crystals example Powder example Thing I didn t talk
More informationQENS in the Energy Domain: Backscattering and Time-of
QENS in the Energy Domain: Backscattering and Time-of of-flight Alexei Sokolov Department of Polymer Science, The University of Akron Outline Soft Matter and Neutron Spectroscopy Using elastic scattering
More informationNeutron 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
More informationTotal Neutron Scattering. Methane Confined in Aerogel Glass. Haiyang Yan
Total Neutron Scattering Cross Section of Solid Methane Confined in Aerogel Glass Haiyang Yan Neutron Properties which makes it an unique probe Charge:0 Interact with atoms by short range residual nuclear
More informationTHE PROSPECT OF NEUTRON SCATTERING IN THE 21 ST CENTURY: A POWERFUL TOOL FOR MATERIALS RESEARCH
THE PROSPECT OF NEUTRON SCATTERING IN THE 21 ST CENTURY: A POWERFUL TOOL FOR MATERIALS RESEARCH E. Kartini Center for Nuclear Industry Material Technology - BATAN Puspiptek Serpong, Tangerang, Indonesia.
More information1. Nuclear Size. A typical atom radius is a few!10 "10 m (Angstroms). The nuclear radius is a few!10 "15 m (Fermi).
1. Nuclear Size We have known since Rutherford s! " scattering work at Manchester in 1907, that almost all the mass of the atom is contained in a very small volume with high electric charge. Nucleus with
More informationLecture 5 Wave and particle beams.
Lecture 5 Wave and particle beams. 1 What can we learn from scattering experiments The crystal structure, i.e., the position of the atoms in the crystal averaged over a large number of unit cells and over
More information4.2 Elastic and inelastic neutron scattering
4.2 ELASTIC AD IELASTIC EUTRO SCATTERIG 73 4.2 Elastic and inelastic neutron scattering If the scattering system is assumed to be in thermal equilibrium at temperature T, the average over initial states
More informationSummer School on Methods and Applications of Neutron Spectroscopy NIST Center for Neutron Research
The Magnetic Phase Transition and Spin Fluctuations in the Geometrically Frustrated Antiferromagnetic Spinel CdCr 2 O 4 : An Experiment Using the SPINS Triple-Axis Spectrometer Summer School on Methods
More informationNeutron scattering. Max Wolff. Division for Material Physics Department of Physics and Astronomy Uppsala University Uppsala Sweden
Neutron scattering Max Wolff Division for Material Physics Department of Physics and Astronomy Uppsala University Uppsala Sweden Outline Why is neutron scattering important? Peculiarities of neutrons How
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 informationRFSS: Lecture 2 Nuclear Properties
RFSS: Lecture 2 Nuclear Properties Readings: Modern Nuclear Chemistry: Chapter 2 Nuclear Properties Nuclear and Radiochemistry: Chapter 1 Introduction, Chapter 2 Atomic Nuclei Nuclear properties Masses
More informationSpectroscopy of Polymers
Spectroscopy of Polymers Jack L. Koenig Case Western Reserve University WOMACS Professional Reference Book American Chemical Society, Washington, DC 1992 Contents Preface m xiii Theory of Polymer Characterization
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 informationCalculate the volume of propane gas at 25.0 C and 1.08 atm required to provide 565 kj of heat using the reaction above.
167 Calculate the volume of propane gas at 25.0 C and 1.08 atm required to provide 565 kj of heat using the reaction above. 1 - Convert energy requirement to moles PROPANE using thermochemical equation.
More informationMODERN 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
More informationAn Introduction to Diffraction and Scattering. School of Chemistry The University of Sydney
An Introduction to Diffraction and Scattering Brendan J. Kennedy School of Chemistry The University of Sydney 1) Strong forces 2) Weak forces Types of Forces 3) Electromagnetic forces 4) Gravity Types
More informationMultiple Choice Questions
Nuclear Physics & Nuclear Reactions Practice Problems PSI AP Physics B 1. The atomic nucleus consists of: (A) Electrons (B) Protons (C)Protons and electrons (D) Protons and neutrons (E) Neutrons and electrons
More informationChapter 29 Atomic Physics. Looking Ahead. Slide 29-1
Chapter 29 Atomic Physics Looking Ahead Slide 29-1 Atomic Spectra and the Bohr Model In the mid 1800s it became apparent that the spectra of atomic gases is comprised of individual emission lines. Slide
More informationAtomic Quantum number summary. From last time. Na Optical spectrum. Another possibility: Stimulated emission. How do atomic transitions occur?
From last time Hydrogen atom Multi-electron atoms This week s honors lecture: Prof. Brad Christian, Positron Emission Tomography Course evaluations next week Tues. Prof Montaruli Thurs. Prof. Rzchowski
More informationNeutron and X-ray Scattering Studies
Neutron and X-ray Scattering Studies Alexis G. Clare NYSCC Alfred NY Clare@alfred.edu clare@alfred.edu Scattering Studies4 1 Outline Review interpreting correlation functions Some more examples Inelastic
More informationCHEM 312: Lecture 9 Part 1 Nuclear Reactions
CHEM 312: Lecture 9 Part 1 Nuclear Reactions Readings: Modern Nuclear Chemistry, Chapter 10; Nuclear and Radiochemistry, Chapter 4 Notation Energetics of Nuclear Reactions Reaction Types and Mechanisms
More informationAPPLICATION OF SPALLATION NEUTRON SOURCES
Abstract APPLICATION OF SPALLATION NEUTRON SOURCES W.E. Fischer, Paul Scherrer Institut, Villigen, Switzerland The first part is devoted to an introduction into the physical principles of spallation neutron
More informationLewis 2.1, 2.2 and 2.3
Chapter 2(and 3) Cross-Sections TA Lewis 2.1, 2.2 and 2.3 Learning Objectives Understand different types of nuclear reactions Understand cross section behavior for different reactions Understand d resonance
More informationElastic scattering. Elastic scattering
Elastic scattering Now we have worked out how much energy is lost when a neutron is scattered through an angle, θ We would like to know how much energy, on average, is lost per collision In order to do
More informationApplications of scattering theory! From the structure of the proton! to protein structure!
Applications of scattering theory From the structure of the proton to protein structure Nicuşor Tîmneanu 2016 Contents and goals What is scattering and why study it? How is the structure of matter determined?
More informationFluorescence and Nuclear Magnetic Resonance (NMR) Spectroscopy
Fluorescence and Nuclear Magnetic Resonance (NMR) Spectroscopy Murphy, B. (2017). Fluorescence and Nuclear Magnetic Resonance Spectroscopy: Lecture 3. Lecture presented at PHAR 423 Lecture in UIC College
More informationIntroduction to Neutron Scattering and ORNL Neutron Facilities
Introduction to Neutron Scattering and ORNL Neutron Facilities Student: Xiangshi Yin (Email: xyin3@utk.edu) Instructor: Elbio Dagotto Course: Solid State II, 2010, Spring Introduction to Neutron Scattering
More informationSchool on Pulsed Neutrons: Characterization of Materials October Neurton Sources & Scattering Techniques (1-2)
1866-6 School on Pulsed Neutrons: Characterization of Materials 15-26 October 2007 Neurton Sources & Scattering Techniques (1-2) Guenter Bauer Forschungzentrum Julich GmbH Julich Germany The Abdus Salam
More informationWave 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
More information100 years of scattering and beyond
A 1 100 years of scattering and beyond Th. Brückel Jülich Centre for Neutron Science Forschungszentrum Jülich GmbH Contents 1 A brief history of x-ray and neutron scattering... 2 2 Introduction to scattering...
More informationNeutron Spin Echo Spectroscopy
Neutron Spin Echo Spectroscopy Peter Fouquet fouquet@ill.eu Institut Laue-Langevin Grenoble, France Oxford Neutron School 2017 What you are supposed to learn in this tutorial 1. The length and time scales
More informationPrinciples of Physical Biochemistry
Principles of Physical Biochemistry Kensal E. van Hold e W. Curtis Johnso n P. Shing Ho Preface x i PART 1 MACROMOLECULAR STRUCTURE AND DYNAMICS 1 1 Biological Macromolecules 2 1.1 General Principles
More informationu d Fig. 6.1 (i) Identify the anti-proton from the table of particles shown in Fig [1]
1 (a) Fig. 6.1 shows the quark composition of some particles. proton neutron A B u u d u d d u d u u u u d Fig. 6.1 (i) Identify the anti-proton from the table of particles shown in Fig. 6.1. (ii) State
More informationWhat is Spallation???
What is Spallation??? Definition found in Nuclear Physics Academic press: projectile (p, n, π,...) target Spallation---a type of nuclear reaction in which the high-energy level of incident particles causes
More informationPROBING CRYSTAL STRUCTURE
PROBING CRYSTAL STRUCTURE Andrew Baczewski PHY 491, October 10th, 2011 OVERVIEW First - we ll briefly discuss Friday s quiz. Today, we will answer the following questions: How do we experimentally probe
More informationJ-PARC and the prospective neutron sciences
PRAMANA c Indian Academy of Sciences Vol. 71, No. 4 journal of October 2008 physics pp. 629 638 J-PARC and the prospective neutron sciences MASATOSHI ARAI J-PARC Center, Japan Atomic Energy Agency, Tokai,
More informationESS. Get Involved! Patrik Carlsson. Allen Weeks
ESS Get Involved! Patrik Carlsson Allen Weeks What is ESS? A European facility for materials research Lund 2025: The European Spallation Source (5 MW) One of Europe's largest planned research infrastructures
More informationQuantum Mechanics. Exam 3. Photon(or electron) interference? Photoelectric effect summary. Using Quantum Mechanics. Wavelengths of massive objects
Exam 3 Hour Exam 3: Wednesday, November 29th In-class, Quantum Physics and Nuclear Physics Twenty multiple-choice questions Will cover:chapters 13, 14, 15 and 16 Lecture material You should bring 1 page
More informationNuclear Physics 2. D. atomic energy levels. (1) D. scattered back along the original direction. (1)
Name: Date: Nuclear Physics 2. Which of the following gives the correct number of protons and number of neutrons in the nucleus of B? 5 Number of protons Number of neutrons A. 5 6 B. 5 C. 6 5 D. 5 2. The
More informationPhysic 492 Lecture 16
Physic 492 Lecture 16 Main points of last lecture: Angular momentum dependence. Structure dependence. Nuclear reactions Q-values Kinematics for two body reactions. Main points of today s lecture: Measured
More informationSlide 1 / 57. Nuclear Physics & Nuclear Reactions Practice Problems
Slide 1 / 57 Nuclear Physics & Nuclear Reactions Practice Problems Slide 2 / 57 Multiple Choice Slide 3 / 57 1 The atomic nucleus consists of: A B C D E Electrons Protons Protons and electrons Protons
More informationHour Exam 3 Review. Quantum Mechanics. Photoelectric effect summary. Photoelectric effect question. Compton scattering. Compton scattering question
Hour Exam 3 Review Hour Exam 3: Wednesday, Apr. 19 In-class (2241 Chamberlin Hall) Twenty multiple-choice questions Will cover: Basic Quantum Mechanics Uses of Quantum Mechanics Addl. Lecture Material
More informationSynchrotron Radiation. How is synchrotron light made? by accelerating electrons
Synchrotron Radiation How is synchrotron light made? by accelerating electrons Electromagnetic Radiation Electrons accelerating by running up and down in a radio antenna emit radio waves Radio waves are
More informationChapter 1. The Elements
Chapter 1. The Elements Electronic structure of atoms (p.1-10) Excitation of atoms (p.10-13) Periodic Table (p. 13-14) References Brownlow (Geochemistry) Gunter Faure (Geochemistry) Krane (Nuclear Physics)
More informationNeutron Interactions Part I. Rebecca M. Howell, Ph.D. Radiation Physics Y2.5321
Neutron Interactions Part I Rebecca M. Howell, Ph.D. Radiation Physics rhowell@mdanderson.org Y2.5321 Why do we as Medical Physicists care about neutrons? Neutrons in Radiation Therapy Neutron Therapy
More informationPHY-105: Introduction to Particle and Nuclear Physics
M. Kruse, Spring 2011, Phy-105 PHY-105: Introduction to Particle and Nuclear Physics Up to 1900 indivisable atoms Early 20th century electrons, protons, neutrons Around 1945, other particles discovered.
More informationIntroduction: Neutron Scattering in Contemporary Research
Introduction: Neutron Scattering in Contemporary Research Th. Brückel This document has been published in Thomas Brückel, Gernot Heger, Dieter Richter, Georg Roth and Reiner Zorn (Eds.): Lectures of the
More informationPhET Interactive Chemistry Simulations Aligned to an Example General Chemistry Curriculum
PhET Interactive Chemistry Simulations Aligned to an Example General Chemistry Curriculum Alignment is based on the topics and subtopics addressed by each sim. Sims that directly address the topic area
More informationTHREE AXES SPECTROMETRY
12 th CENTRAL EUROPEAN TRAINING SCHOOL ON NEUTRON SCATTERING 6 11 May 2018 BUDAPEST NEUTRON CENTRE (BNC) THREE AXES SPECTROMETRY Gerhard Krexner Faculty of Physics, University of Vienna 1 O V E R V I E
More informationGlobal properties of atomic nuclei
Global properties of atomic nuclei How to probe nuclear size? Electron Scattering from nuclei For low energies and under conditions where the electron does not penetrate the nucleus, the electron scattering
More informationNeutron Reflectometry as In Situ Probe of Thin Film Composition and Layer Structure for Investigating Corrosion and Hydrogen Absorption in Titanium
Neutron Reflectometry as In Situ Probe of Thin Film Composition and Layer Structure for Investigating Corrosion and Hydrogen Absorption in Titanium Jamie Noël, Zin Tun *, and David Shoesmith University
More informationMaterials for energy, heath, environment
WHAT DO WE STUDY WITH NEUTRONS? Materials for energy, heath, environment archaeological artefacts, commercial products 2010 2000 1990 1980 phase transitions magnetic orderings magnetic fluctuations exchanges
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 informationNanomaterials and their Optical Applications
Nanomaterials and their Optical Applications Winter Semester 2013 Lecture 02 rachel.grange@uni-jena.de http://www.iap.uni-jena.de/multiphoton Lecture 2: outline 2 Introduction to Nanophotonics Theoretical
More informationHeat of formation / enthalpy of formation!
165 Heat of formation / enthalpy of formation! What is the enthalpy change at standard conditions when 25.0 grams of hydrogen sulfide gas is reacted? 1 - Use Hess' Law to find the enthalpy change of the
More informationThe Vortex Lattice of a Type II Superconductors Studied by Small Angle Neutron Scattering
Paul Scherrer Institut Laboratory for Neutron Scattering and Imagingg Student Laboratory Work The Vortex Lattice of a Type II Superconductors Studied by Small Angle Neutron Scattering Author: Dr. J. L.
More informationHigh-precision studies in fundamental physics with slow neutrons. Oliver Zimmer Institut Laue Langevin
High-precision studies in fundamental physics with slow neutrons Oliver Zimmer Institut Laue Langevin ILL, 20 September 2016 Topics The impossible particle and its properties Search for an electric dipole
More informationOutline. Chapter 6 The Basic Interactions between Photons and Charged Particles with Matter. Photon interactions. Photoelectric effect
Chapter 6 The Basic Interactions between Photons and Charged Particles with Matter Radiation Dosimetry I Text: H.E Johns and J.R. Cunningham, The physics of radiology, 4 th ed. http://www.utoledo.edu/med/depts/radther
More informationA new UCN source at TRIUMF for EDM, β decay, gravity etc.
A new UCN source at TRIUMF for EDM, β decay, gravity etc. UCN For these experiments, Phase space density is crucial. Momentum space is limited by Fermi potential (E c = 100~200 nev) and magnetic potential
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 informationSECTION 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
More informationA Light for Science. EIROFORUM Teachers School 09/10/2011 W.G. Stirling
A Light for Science EIROforum Teachers School 2011 The EPN campus Overview of EMBL, ESRF and ILL Neutrons and synchrotron X-rays: properties, sources Upgrade programmes ILL and ESRF The future: new sources,
More informationAPPLIED RADIATION PHYSICS
A PRIMER IN APPLIED RADIATION PHYSICS F A SMITH Queen Mary & Westfield College, London fe World Scientific m Singapore * New Jersey London Hong Kong CONTENTS CHAPTER 1 : SOURCES of RADIATION 1.1 Introduction
More informationLECTURE 6: INTERACTION OF RADIATION WITH MATTER
LCTUR 6: INTRACTION OF RADIATION WITH MATTR All radiation is detected through its interaction with matter! INTRODUCTION: What happens when radiation passes through matter? Interlude The concept of cross-section
More informationPrentice Hall. Physics: Principles with Applications, Updated 6th Edition (Giancoli) High School
Prentice Hall Physics: Principles with Applications, Updated 6th Edition (Giancoli) 2009 High School C O R R E L A T E D T O Physics I Students should understand that scientific knowledge is gained from
More information1 v. L18.pdf Spring 2010, P627, YK February 22, 2012
L18.pdf Spring 2010, P627, YK February 22, 2012 18 T2 Nuclear Information Service at LANL: http://t2.lanl.gov/data/ ENDF/B VI Neutron Data : http://t2.lanl.gov/cgi bin/nuclides/endind Thermal neutron x
More informationWhat did you learn in the last lecture?
What did you learn in the last lecture? Charge density distribution of a nucleus from electron scattering SLAC: 21 GeV e s ; λ ~ 0.1 fm (to first order assume that this is also the matter distribution
More information(Refer Slide Time: 1:15)
Principles and Applications of NMR spectroscopy Professor Hanudatta S. Atreya NMR Research Centre Indian Institute of Science Bangalore Module 1 Lecture No 01. Welcome every one. This is going to be a
More informationLecture 6 Scattering theory Partial Wave Analysis. SS2011: Introduction to Nuclear and Particle Physics, Part 2 2
Lecture 6 Scattering theory Partial Wave Analysis SS2011: Introduction to Nuclear and Particle Physics, Part 2 2 1 The Born approximation for the differential cross section is valid if the interaction
More informationPhysics 107 Final Exam December 13, Your Name: Questions
Physics 107 Final Exam December 13, 1993 Your Name: Questions 1. 11. 21. 31. 41. 2. 12. 22. 32. 42. 3. 13. 23. 33. 43. 4. 14. 24. 34. 44. 5. 15. 25. 35. 45. 6. 16. 26. 36. 46. 7. 17. 27. 37. 47. 8. 18.
More informationNotes on x-ray scattering - M. Le Tacon, B. Keimer (06/2015)
Notes on x-ray scattering - M. Le Tacon, B. Keimer (06/2015) Interaction of x-ray with matter: - Photoelectric absorption - Elastic (coherent) scattering (Thomson Scattering) - Inelastic (incoherent) scattering
More informationFundamental aspects of the thermal neutron scattering
Fundamental aspects of the thermal neutron scattering Florencia Cantargi cantargi@cab.cnea.gov.ar Departamento de Física de Neutrones Gerencia de Ingeniería Nuclear Instituto Balseiro (UNCuyo) Centro Atómico
More informationSPALLATION NEUTRON SOURCES FOR SCIENCE AND TECHNOLOGY
Proceedings of the 8 th Conference on Nuclear and Particle Physics, 20-24 Nov. 2011, Hurghada, Egypt SPALLATION NEUTRON SOURCES FOR SCIENCE AND TECHNOLOGY M.N.H. Comsan Nuclear Research Center, Atomic
More information