Polarization Dependence in X-ray Spectroscopy and Scattering. S P Collins et al Diamond Light Source UK

Similar documents
X-Rays and Magnetism From Fundamentals to Nanoscale Dynamics

Time out states and transitions

Automatic and Objective Measurement of Residual Stress and Cord in Glass

PHOTOELECTRIC EFFECT AND DUAL NATURE OF MATTER AND RADIATIONS

Acousto-optic modulator

Physics 441/2: Transmission Electron Microscope

Reflection Electron Microscopy and Spectroscopy for Surface Analysis

How To Understand Light And Color

Near-field scanning optical microscopy (SNOM)

Crystal Optics of Visible Light

Instytut Fizyki Doświadczalnej Wydział Matematyki, Fizyki i Informatyki UNIWERSYTET GDAŃSKI

6) How wide must a narrow slit be if the first diffraction minimum occurs at ±12 with laser light of 633 nm?

Raman spectroscopy Lecture

Introduction to Powder X-Ray Diffraction History Basic Principles

X-Ray Diffraction HOW IT WORKS WHAT IT CAN AND WHAT IT CANNOT TELL US. Hanno zur Loye

EDS system. CRF Oxford Instruments INCA CRF EDAX Genesis EVEX- NanoAnalysis Table top system

Arrangement of Electrons in Atoms

Electron Microscopy SEM and TEM

- thus, the total number of atoms per second that absorb a photon is

Wir schaffen Wissen heute für morgen

Raman Spectroscopy. 1. Introduction. 2. More on Raman Scattering. " scattered. " incident

PHYA2. General Certificate of Education Advanced Subsidiary Examination June Mechanics, Materials and Waves

Chapter 18: The Structure of the Atom

The Fundamentals of Infrared Spectroscopy. Joe Van Gompel, PhD

Damping Wigglers in PETRA III

X-ray Diffraction (XRD)

The Role of Electric Polarization in Nonlinear optics

Electron density is complex!

PHYSICS PAPER 1 (THEORY)

Preface Light Microscopy X-ray Diffraction Methods

It has long been a goal to achieve higher spatial resolution in optical imaging and

TIME OF COMPLETION NAME SOLUTION DEPARTMENT OF NATURAL SCIENCES. PHYS 3650, Exam 2 Section 1 Version 1 October 31, 2005 Total Weight: 100 points

Infrared Spectroscopy: Theory

Spectrophotometry and the Beer-Lambert Law: An Important Analytical Technique in Chemistry

Section 6 Raman Scattering (lecture 10)

Electron Orbits. Binding Energy. centrifugal force: electrostatic force: stability criterion: kinetic energy of the electron on its orbit:

Study of the anomalous magnetic behavior of nanostructures by X-ray magnetic circular dichroism

Atomic Structure Ron Robertson

Nanoelectronics 09. Atsufumi Hirohata Department of Electronics. Quick Review over the Last Lecture

where h = J s

Nanoscience Course Descriptions

Phase determination methods in macromolecular X- ray Crystallography

SPECTROSCOPY. Light interacting with matter as an analytical tool

Powder diffraction and synchrotron radiation

From lowest energy to highest energy, which of the following correctly orders the different categories of electromagnetic radiation?

Upcoming APS Summer Schools

A More Efficient Way to De-shelve 137 Ba +

Force on Moving Charges in a Magnetic Field

X-ray Diffraction and EBSD

Magnetic Dipoles. Magnetic Field of Current Loop. B r. PHY2061 Enriched Physics 2 Lecture Notes

Determination of Molecular Structure by MOLECULAR SPECTROSCOPY

Two bar magnets are brought near each other as shown. The magnets... A) attract B) repel C) exert no net force on each other.

Diffraction Course Series 2015

Jorge E. Fernández Laboratory of Montecuccolino (DIENCA), Alma Mater Studiorum University of Bologna, via dei Colli, 16, Bologna, Italy

One example: Michelson interferometer

INFRARED SPECTROSCOPY (IR)

Raman Scattering Theory David W. Hahn Department of Mechanical and Aerospace Engineering University of Florida

Proton Nuclear Magnetic Resonance Spectroscopy

Experiment #5: Qualitative Absorption Spectroscopy

PHYSIOLOGY AND MAINTENANCE Vol. II - On The Determination of Enzyme Structure, Function, and Mechanism - Glumoff T.

Symmetric Stretch: allows molecule to move through space

Amino Acids. Amino acids are the building blocks of proteins. All AA s have the same basic structure: Side Chain. Alpha Carbon. Carboxyl. Group.

Waves Sound and Light

Fraunhofer Diffraction

2. Spin Chemistry and the Vector Model

Lecture 20: Scanning Confocal Microscopy (SCM) Rationale for SCM. Principles and major components of SCM. Advantages and major applications of SCM.

X Ray Flourescence (XRF)

Introduction to X-Ray Powder Diffraction Data Analysis

Technician Licensing Class

Force on a square loop of current in a uniform B-field.

Organic Chemistry Tenth Edition

Status of the Free Electron Laser

A Guide to Acousto-Optic Modulators

Interaction of Atoms and Electromagnetic Waves

Introduction to Optics

X-ray thin-film measurement techniques

PCV Project: Excitons in Molecular Spectroscopy

Nuclear Magnetic Resonance (NMR) Spectroscopy cont... Recommended Reading:

E. K. A. ADVANCED PHYSICS LABORATORY PHYSICS 3081, 4051 NUCLEAR MAGNETIC RESONANCE

Chapter 7: Basics of X-ray Diffraction

Using light scattering method to find The surface tension of water

Introduction to Nuclear Magnetic Resonance Spectroscopy

Refraction of Light at a Plane Surface. Object: To study the refraction of light from water into air, at a plane surface.

CREOL, College of Optics & Photonics, University of Central Florida

Copyright by Mark Brandt, Ph.D. 12

After a wave passes through a medium, how does the position of that medium compare to its original position?

Crystal Structure Determination I

Preview of Period 3: Electromagnetic Waves Radiant Energy II

Microscopy: Principles and Advances

Optical Storage Technology. Optical Disc Storage

Spin-flip excitation spectroscopy with STM excitation of allowed transition adds an inelastic contribution (group of Andreas Heinrich, IBM Almaden)

Chapter 27 Magnetic Field and Magnetic Forces

13C NMR Spectroscopy

STRUCTURAL STUDIES OF MULTIFERROIC THIN FILMS

Basic principles and mechanisms of NSOM; Different scanning modes and systems of NSOM; General applications and advantages of NSOM.

Sample Exercise 6.1 Concepts of Wavelength and Frequency

5. Scanning Near-Field Optical Microscopy 5.1. Resolution of conventional optical microscopy

Theory of electrons and positrons

Insertion Devices Lecture 4 Permanent Magnet Undulators. Jim Clarke ASTeC Daresbury Laboratory

Transcription:

Polarization Dependence in X-ray Spectroscopy and Scattering S P Collins et al Diamond Light Source UK

Overview of talk 1. Experimental techniques at Diamond: why we care about x-ray polarization 2. How polarized x-rays are generated 3. Future directions

X-ray interactions with matter: Key techniques Absorption/transmission Elastic scattering Inelastic scattering (resonant, non-resonant) Photoelectron spectroscopy

Max von Laue 1914 Nobel Laureate in Physics for his discovery of the diffraction of X-rays by crystals. Laue predicted that if x-rays were a form of short-wavelength electromagnetic radiation then they should produce diffraction effects as they pass through crystals This idea was put to the test by Friedrich The field of X-ray diffraction and crystallography was born

X-ray Diffraction and Crystallography ( and why we need synchrotrons)

Polarization by scattering x ( ε ε ˆ ˆ ) 1 E E ( ε ε ˆ ˆ ) 1 y ( ε ε ˆ ˆ ) 0 2 ( εˆ εˆ ) cos2 z ( ε ε ˆ ˆ ) 1

Polarization of Synchrotron Radiation Intense beams of linearly polarized x-rays

X-ray Diffraction & Scattering: Why do we care about polarization? Because the scattering depends strongly on linear polarization; scattering can become very weak in the horizontal plane; data must be corrected for polarization. But the polarization dependence tells us nothing about the sample, it just reminds us that light is a transverse wave. Bragg scattering can be used as a polarization analyser.

Absorption/transmission Is polarization important in absorption?

Polarizing glasses are very cool Linear dichroism and birefringence gives information about internal polarization of materials. Does it work with x-rays?

0.56 0.54 0.52 0.50 Relative transmittance 1.02 1.00 0.98 0.96 0.94 0.92 b=-45 o a=90 o a=0 0.90 0.88 b=+45 o m(cm -1 ) 0.48 0.86 0.84 0.46 0.82 0.44 HN22 0 30 60 90 120 150 180 210 240 270 300 330 360 Polarizer angle a (degrees) 0.42 0.40 33.10 33.15 33.20 33.25 33.30 33.35 Energy (kev)

X-ray Absorption: Why do we care about polarization? Because absorption from anisotropic systems depends on linear polarization. This effect can give rise to x-ray dichroism and birefringence at particular photon energies One could construct polarizing devices or study, for example, orientations of chemical bonds. And going beyond the electric dipole approximation one can observe more exotic high-order atomic multipoles such as hexadecapoles in cubic systems

Fluorescence Strontium titanate SrTiO 3 A B C C A B

Sir William Henry Bragg (1862-1942) Sir William Lawrence Bragg (1890-1971) So what was left for the Bragg s to do? The father and son team carried out their own experiments and, in analogy with optical diffraction, worked out a formula for the wavelength of the diffracted wave: the famous Bragg s Law 1915 Nobel prize for physics "for their services in the analysis of crystal structure by means of X- rays".

Resonant forbidden scattering: Why do we care about polarization? Because the polarization breaks the symmetry that normally causes an exact cancellation of the scattering at these positions The residual scattering is extremely interesting as it provides direct information about very weak processes that are normally hidden, e.g. exotic electronic polarization effects, magnetism

Magnetic forces on electron: Magnetic scattering Electromagnetic wave E Electron S H There are several other magnetic terms, each having different polarization dependence. They are all very weak. Forces: electric magnetic (Zeeman) f f = -ee = -2 ( S H) mb Ratio of Zeeman force to electric force: I I f f Z e mag charge 1 2 ~ 10 2 m c 6 e ~ 10 2 or less!

FeBO 3 : A weak ferromagnet studied by x-ray diffraction (Diamond I16)

Magnetic x-ray scattering: Why do we care about polarization? Because the magnetic x-ray scattering has a very different polarization dependence from change scattering This enables it to be identified as magnetic It also allows us uniquely to obtain information about the distribution of spin and orbital magnetic moments in the material N S S N N S

A circular dichroism measurement Magnet poles I=I e -( m m) t o Ferromagnetic sample Circularly polarized beam Magnetizing field I=I o

X-ray absorption and orbital polarization

Beamline I06 - Nanoscience A polarised soft x-ray beamline for microscopy and spectroscopy PEEM images recorded using X-Ray Magnetic Circular Dichroism (left) and X- ray Magnetic Linear Dichroism (right) showing ferromagnetic and antiferromagnetic domains, respectively, in Co thin films grown on NiO.

Magnetic Circular Dichroism: Why do we care about polarization? Because the angular momentum of the photon circular polarization couples directly to the angular momentum of electronic states to give a huge sensitivity to magnetism. Synchrotron radiation is now one of the major tools for studying magnetic materials This process also forms the basis of novel microscopy techniques allowing magnetic domains and dynamics to be studied 10 nm resolution There are similar effects in resonant scattering.

Diamond Beamline I16

Tellurium results from I16: 001 and 002 forbidden reflections

Studies of Chiral Systems: Why do we care about polarization? Because circular polarization breaks the mirrors symmetry of the photon beam, allowing studies of chiral samples These are of fundamental importance to chemistry and biology (nature is chiral) These effects play an important role in contemporary condensed matter physics, i.e. the magnetoelectric effect, chiral magnetic structures

X-ray birefringence imaging - Dynamical Diffraction Transmission image through diamond - horizontal polarization Vertical polarization

Polarization of Synchrotron Radiation Intense beams of linearly polarized x-rays Quarter-wave phase plate

The Future: Production of linear and circular beams: already very efficient, especially linear polarization Reversible circular polarizers to pick out very small changes that couple to photon helicity: still challenging. The state-of-the-art is sensitivity at 10-5 level but this if very difficult. 10-3 is more typical; 10-7 would certainly provide new techniques such as x- ray natural circular dichroism in chiral liquids. Polarization analysers and polarization sensitive detector: very challenging. The efficiency and complexity of current devices is perhaps the main limiting factor is synchrotron techniques such as magnetic scattering.