The Advanced Photon Source

Slides:



Advertisements
Similar presentations
Bragg’s Law nl=2dsinΘ Just needs some satisfaction!! d Θ l
Advertisements

Ion Beam Analysis techniques:
Crystal diffraction Laue Nobel prize Max von Laue
Internal – External Order We described symmetry of crystal habit (32 point groups) We also looked at internal ordering of atoms in 3-D structure (230 space.
X-Ray Crystallography The most important technique for mineralogy The most important technique for mineralogy Direct measurement of atomic arrangement.
Solid State Physics 2. X-ray Diffraction 4/15/2017.
January 23, 2001Physics 8411 Elastic Scattering of Electrons by Nuclei We want to consider the elastic scattering of electrons by nuclei to see (i) how.
Grazing incident X-ray Diffraction (XRD) X-rays are electromagnetic radiation with very short wavelength (  m), very suitable to do diffraction.
P460 - transitions1 Transition Rates and Selection Rules Electrons in a atom can make transitions from one energy level to another not all transitions.
Properties of Multilayer Optics An Investigation of Methods of Polarization Analysis for the ICS Experiment at UCLA 8/4/04 Oliver Williams.
R.T. Jones, Newport News, Mar 21, 2002 Effects of Crystal Quality on Beam Intensity The graph at right shows how the width of a diamond’s Bragg peak affects.
Absorption and Emission Spectrum
X-Ray Diffraction ME 215 Exp#1. X-Ray Diffraction X-rays is a form of electromagnetic radiation having a range of wavelength from nm (0.01x10 -9.
Nuclear de-excitation Outline of approach… Source of radiation Propagation of radiation field Detection of radiation ?? nucleus.
Chapter 19 NMR Spectroscopy. Introduction... Nuclear Magnetic Resonance Spectrometry is based on the measurement of absorption of electromagnetic radiation.
Synchrotron Radiation Interaction with Matter; Different Techniques Anders Nilsson Stanford Synchrotron Radiation Laboratory What can we hope to learn?
X-Ray Diffraction Spectroscopy RAMAN Microwave. What is X-Ray Diffraction?
Joachim Stöhr Stanford Synchrotron Radiation Laboratory X-Ray Absorption Spectroscopy J. Stöhr, NEXAFS SPECTROSCOPY,
X-ray Diffraction Outline Crystals and Bragg Diffraction
III. Analytical Aspects Summary Cheetham & Day, Chapters 2, 3 Chemical Characterization of Solid-State Materials Chemical Composition: Bulk, Surface, …
Chapter 7 X-Ray diffraction. Contents Basic concepts and definitions Basic concepts and definitions Waves and X-rays Waves and X-rays Crystal structure.
Phys 102 – Lecture 26 The quantum numbers and spin.
A. Magerl Crystallography and Structural Physics University of Erlangen-Nürnberg Neutrons versus X-rays Novosibirsk 10. Oct
Ch ; Lecture 26 – Quantum description of absorption.
 Magnetism and Neutron Scattering: A Killer Application  Magnetism in solids  Bottom Lines on Magnetic Neutron Scattering  Examples Magnetic Neutron.
Applications of polarized neutrons V.R. Skoy Frank Laboratory of Neutron Physics, Joint Institute for Nuclear Research Dubna, Moscow Region, Russia.
Introduction to Neutron Scattering Jason T. Haraldsen Advanced Solid State II 2/27/2007.
Resonant magnetic x-ray scattering and Summary Resonant scattering –Why do it? –What is it? –How is it done? –Example(s) The Real World …. CaFe 2 As 2.
The physics of electron backscatter diffraction Maarten Vos AMPL, RSPHYSSE, Australian National University, Acton 0200, Canberra Aimo Winkelmann Max Planck.
Resolution Limits for Single-Slits and Circular Apertures  Single source  Two sources.
Size and Structure Mikhail Bashkanov University of Edinburgh UK Nuclear Physics Summer School III.
Wave nature of light Light is an electromagnetic wave. EM waves are those waves in which there are sinusoidal variation of electric and magnetic fields.
Methods of excitation: nuclear reactions
The Structure and Dynamics of Solids
X-ray absorption spectroscopy (XAS)
The Muppet’s Guide to: The Structure and Dynamics of Solids Material Characterisation.
The Structure and Dynamics of Solids
Physics 1202: Lecture 28 Today’s Agenda Announcements: –Midterm 2: solutions HW 8 this FridayHW 8 this Friday Diffraction –Review Polarization –Reflection.
Förster Resonance Energy Transfer (FRET)
Mineral Spectroscopy Visible Infrared Raman Mössbauer NMR.
Bremsstrahlung of fast electron on graphene
Dipole radiation during collisions LL2 Section 68.
Presentation on.  There are many methods for measuring of fiber structure. Such as:  The absorption of infrared radiation  Raman scattering of light.
Phys102 Lecture 26, 27, 28 Diffraction of Light Key Points Diffraction by a Single Slit Diffraction in the Double-Slit Experiment Limits of Resolution.
Raman Effect The Scattering of electromagnetic radiation by matter with a change of frequency.
Polarization Dependence in X-ray Spectroscopy and Scattering
Ch.4 Atomic Structure of Solid Surfaces.
A: Wave Phenomena A.6 Polarisation.
CHAPTER 3: STRUCTURE OF CRYSTALLINE SOLIDS

Chem E5225 – Electron Microscopy P
Nuclear Magnetic Resonance Spectroscopy
de Broglie Waves de Broglie argued
Crystallography H. K. D. H. Bhadeshia Introduction and point groups
11: Wave Phenomena 11.5 Polarization.
Light Waves Interacting with Matter
PHL424: γ-decay γ-decay is an electromagnetic process where the nucleus decreases in excitation energy, but does not change proton or neutron numbers This.
X-Ray Diffraction and Reciprocal Lattice
Light Waves Interacting with Matter
X-ray Emission Spectroscopy
PHY 752 Solid State Physics
What use is Reciprocal Space? An Introduction
Nuclear Magnetic Resonance (NMR) Spectroscopy
Diffraction T. Ishikawa Part 2, Dynamical Diffraction 1/16/2019 JASS02.
Chap 8 Analytical Instruments
Interaction of Radiation with Matter
Val Kostroun and Bruce Dunham
Ion-beam, photon and hyperfine methods in nano-structured materials
Chapter 19 NMR Spectroscopy.
Presentation transcript:

The Advanced Photon Source You are here 6-BM-A 6-BM-B 6-ID-A 6-ID-B 6-ID-C 6-ID-D

Diffraction from ordered structures • Incoming X-rays diffract from crystal planes. Adapted from Fig. 3.2W, Callister 6e. d= n l /2sin q c 2q Measurement of the scattered intensity as a function of 2q provides the atomic spacing, d. Intensity

Magnetic periodicity leads to magnetic Bragg peaks t =2p/2d t 1 10-6 d Q 2p/d

Why Bother? For magnetic scattering compared to charge or nuclear scattering: (ds/dW)X-ray = 10-5 10-6 (ds/dW)Neutron Why Bother? Many of the technologically important RE compounds contain neutron opaque elements. Superior reciprocal space (Q) resolution allows more detailed study … reinvestigation of “solved” structures. Can be used for investigations of submillimeter-sized single crystals. Resonant magnetic scattering occurs at well-defined energies specific to elements of interest -- probe local magnetism. Studies of magnetic surfaces and interfaces.

X-ray Resonant Magnetic Scattering (XRMS) (L2, L3)-edge for rare-earths (6-10KeV) Electric multipole transition (dipole : 2p – 5d, quadrupole 2p – 4f) Dipole transition is dominant 4f : magnetic properties 5d : exchange splitting by 4f EF P3/2 P1/2 LIII & LII Incoming photon outgoing photon Scattering matrix element is identical to the matrix element for XMCD!

The angular piece is used to determine moment directions Non-resonant: ds/dW  [S2sinQ]2 (outgoing s- pol.)  [2sin2Q  cosQ{(L1+S1) + S3sinQ}]2 (outgoing p- pol.) Resonant (E1): ds/dW  0 (outgoing s- pol.)  (-M1cosQ + M3sinQ)2 (outgoing p- pol.)  (k′· M)2 Resonant (Quadrupole): Much more complicated, but can probe M1, M2, M3 How do we measure magnetic scattering. 1) Orient crystal axes with respect to scattering plane 2) incident and outgoing wavevectors k and k’ define the scattering plane. Incident polarization is sigma, outgoing polarization is sigma or pi and we can do polarization analysis. For nonresonant scattering we are scattering directly from the magnetic electrons (e.g. 4f) - primarily sensitive (except at high angles) to the comp. of the moment out of the scattering plane along u2 Resonant scattering involves eletric dipole transitions from the p-d states. Sensitive to magnetization through polarization from f-electrons - sensitive to the components of the moment in the scattering plane. J. P. Hill, and D. F. McMorrow, Acta Crystallogr. Sec.A 52, 236 (1996). M. Blume, and Doon Gibbs, Phys. Rev. B 37, 1779 (1988).