Muon Beam Research in Condensed Matter Science: achievements and prospects Vice President of the International Society for Muon Spectroscopy (ISMS) President.

Slides:



Advertisements
Similar presentations
Current 5 year plan (Sonier) 1. A high field low temperature muSR spectrometer (MacLaughlin and Kiefl) 2.Low energy muon beamline /s at TRIUMF.
Advertisements

MR TRACKING METHODS Dr. Dan Gamliel, Dept. of Medical Physics,
IKON7, Instrument clip session, September 2014, ESS Headquarters and Medicon Village, Lund, Sweden A cold neutron beamline for Particle
ESS and Reflectometry SAC Report 22 nd May The Reflectometry STAP John Ankner (SNS) Richard Campbell (ILL) Bob Cubitt (ILL) Robert Dalgliesh (ISIS)
Photons muons neutrons Tuning the static spin-stripe phase and superconductivity in La 2-x Ba x CuO 4 (x = 1/8) by hydrostatic pressure Zurab Guguchia.
NMR SPECTROSCOPY.
Outlook towards future Polish participation in the new Accelerator Facility Tomasz Matulewicz Warsaw University.
Structure Determination by NMR CHY 431 Biological Chemistry Karl D. Bishop, Ph.D. Lecture 1 - Introduction to NMR Lecture 2 - 2D NMR, resonance assignments.
Rinat Ofer Supervisor: Amit Keren. Outline Motivation. Magnetic resonance for spin 3/2 nuclei. The YBCO compound. Three experimental methods and their.
Presented by Steve Kliewer Muon Lifetime Experiment: A Model.
Nuclear Magnetic Resonance Spectrometry Chap 19
Nuclear Magnetic Resonance Spectrometry Chap 19. Absorption in CW Experiments Energy of precessing particle E = -μ z B o = -μ B o cos θ When an RF photon.
A short presentation in the group by Prem Basnet 09/29/04.
The attraction of  + to O 2- : using muons to study oxides Steve Blundell Clarendon Laboratory, Dept. Physics, University Of Oxford, UK.
Spectroscopy 3: Magnetic Resonance CHAPTER 15. Pulse Techniques in NMR The “new technique” Rather than search for and detect each individual resonance,
Superconductivity Characterized by- critical temperature T c - sudden loss of electrical resistance - expulsion of magnetic fields (Meissner Effect) Type.
Magnetic properties of SmFeAsO 1-x F x superconductors for 0.15 ≤ x ≤ 0.2 G. Prando 1,2, P. Carretta 1, A. Lascialfari 1, A. Rigamonti 1, S. Sanna 1, L.
III. Analytical Aspects Summary Cheetham & Day, Chapters 2, 3 Chemical Characterization of Solid-State Materials Chemical Composition: Bulk, Surface, …
Muon Spin Rotation (µSR) technique and its applications in superconductivity and magnetism Zurab Guguchia Physik-Institut der Universität Zürich, Winterthurerstrasse.
Condensed Matter Physics Big Facility Physics26th Jan 2004 Sub Heading “Big Facility” Physics in Grenoble ESRF: X-rays ILL: neutrons.
Physical and Chemical Tests 10-1 Purification: Chromatography Distillation Recrystallization Comparison to known compounds: Melting point Boiling point.
FFAG Fixed Field Alternating Gradient synchrotrons, FFAGs, combine some of the main advantages of both cyclotrons and synchrotrons:  Fixed magnetic field.
Muon Spectroscopy Koji Yokoyama School of Physics and Astronomy, QMUL (on behalf of Dr. Alan Drew) MRI Spectroscopy Workshop 29 th May, 2014.
Paul Scherrer Institut
Magnetic Resonance Imaging
Investigating the mechanism of High Temperature Superconductivity by Oxygen Isotope Substitution Eran Amit Amit Keren Technion- Israel Institute of Technology.
Frequency dependence of the anomalous Hall effect: possible transition from extrinsic to intrinsic behavior John Cerne, University at Buffalo, SUNY, DMR.
Magnetism in Azurite Studied by Muon Spin Rotation (a status report) M. Kraken, S. Süllow and F.J. Litterst IPKM, TU Braunschweig A.U.B. Wolter, IFW Dresden.
Chapter 31 Nuclear Energy; Effects and Uses of Radiation.
Future Muon Sources, University of Huddersfield, 12/13 January 2015 IIAA Welcome ! Professor Bob Cywinski Dean of the Graduate School and Special Adviser.
S.J. Brooks RAL, Chilton, OX11 0QX, UK Options for a Multi-GeV Ring Ramping field synchrotron provides fixed tunes and small.
Different methods for structure elucidation. Spectroscopy: Studying the properties of matter through its interaction with different frequency components.
Dynamics Neutron Scattering and Dan Neumann
WG4 Summary -Intense Muon Physics- Conveners Y. Semertzdis (BNL), M. Grassi (Pisa), K. Ishida (RIKEN) summary-1 for muon applications by K. Ishida.
NUCLEAR MAGNETIC RESONANCE SPECTROSCOPY Basics of …….. NMR phenomenonNMR phenomenon Chemical shiftChemical shift Spin-spin splittingSpin-spin splitting.
Nuclear Magnetic Resonance I Magnetization properties Generation and detection of signals.
Structure in the mixed phase
Introduction to Helicity Particle Physics of μSR The World's μSR Facilities Basic Techniques of μSR Applications of μSR Jess H. Brewer 15 May 2004 Jess.
Introduction to Neutron Scattering Jason T. Haraldsen Advanced Solid State II 2/27/2007.
Low–field NMR (or MRI) Images of Laser polarized Noble Gas.
Towards a Next Generation  SR Facility Bob Cywinski School of Applied Sciences FFAG’08, Manchester, September 2008.
Giorgi Ghambashidze Institute of Condensed Matter Physics, Tbilisi State University, GE-0128 Tbilisi, Georgia Muon Spin Rotation Studies of the Pressure.
Managed by UT-Battelle for the Department of Energy Dynamically Polarized Solid Target for Neutron Scattering Josh Pierce, J.K. Zhao Oak Ridge National.
Petersburg Nuclear Physics Institute. Petersburg Nuclear Physics Institute was founded in 1954 as a part of Physical-Technical Institute of the Academy.
Introduction to Helicity Particle Physics of μSR The World's μSR Facilities Basic Techniques of μSR Applications of μSR Jess H. Brewer 15 May 2004 Jess.
Beam Dynamics in the ESS Linac Under the Influence of Monopole and Dipole HOMs A.Farricker 1, R.M.Jones 1, R.Ainsworth 2 and S.Molloy 3 1 The University.
IDS-NF Accelerator Baseline The Neutrino Factory [1, 2] based on the muon storage ring will be a precision tool to study the neutrino oscillations.It may.
Past and Future Insights from Neutron Scattering Collin Broholm * Johns Hopkins University and NIST Center for Neutron Research  Virtues and Limitations.
M. Ueda, T. Yamasaki, and S. Maegawa Kyoto University Magnetic resonance of Fe8 at low temperatures in the transverse field.
NMR and The Designing and Manufacturing of an NMR Probe for 109 Ag in Li x Ag 3 V 4 O 11 Cathode Material, for 0.72
Magnetic Resonance Imaging Glenn Pierce, King’s College London, Department of Physics Introduction Edward Purcell and Felix Bloch were both awarded the.
Next Generation Science with Inelastic X-ray Scattering
First Principle Calculation of Nuclear Magnetic Resonance (NMR) chemical shift Kanchan Sonkar Center of Biomedical Magnetic Resonance SGPGIMS-Campus, Lucknow,
MOLECULAR STRUCTURE ANALYSIS NMR Spectroscopy VCE Chemistry Unit 3: Chemical Pathways Area of Study 2 – Organic Chemistry.
NUCLEAR MAGNETIC RESONANCE
All in a spin – An introduction to muon science
Muons in condensed matter research Tom Lancaster Durham University, UK.
1 Instrumental Analysis Tutorial 10 Nuclear Magnetic Resonance NMR.
Introduction to The World's μSR Facilities Basic Techniques of μSR μSR “Toolbox” for QM Examples of μSR in HT c SC Jess H. Brewer CIAR QM Summer School.
PSI, Zurich February 29 – March Session classification : Accelerator Concepts Tuesday, March 1, 2016 Introduction Vyacheslav Yakovlev Fermilab,
AFTERWORD Town Meeting 2002
(Instrument part) Thanundon Kongnok M
ESS Gold A Proposal for a Next Generation European Neutron Source
the s process: messages from stellar He burning
Continuous Change of Landau Renormalization from Heavy Fermion to Mixed Valence in Ce1-xYbxCoIn5 Zhaofeng Ding, J. Zhang, C. Tan, K. Huang, Lei Shu (Fudan.
10.4 Continuous Wave NMR Instrumentation coherent detection
at the University of Alabama
Advanced Pharmaceutical Analysis
(4)ELECTRONIC SUPPORT SYSTEM
HiFi The high-field muon instrument at ISIS
Presentation transcript:

Muon Beam Research in Condensed Matter Science: achievements and prospects Vice President of the International Society for Muon Spectroscopy (ISMS) President of ISMS-Europe Department of Physics and Astronomy University of Leeds, Yorkshire, UK Bob Cywinski European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002

The European Spallation Source The scientific and technical case for ESS has now been made... ESS is emerging as the “European Source of Science” …….not just as a world leading source of neutrons but also of exotic nuclei, neutrinos, pions and muons…..

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002 Applications of muon beams Physics Magnetism Superconductivity Surfaces Fundamental physics Materials Polymers Semiconductors Hydrogen in metals Chemistry Molecular dynamics Oxides Muonium Biology Proteins

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002 Some  SR highlights First observation of magnetic order in the high T c cuprate superconductors Detailed characterisation of the vortex state in conventional and exotic superconductors First direct observation of the predicted evolution of Kohlrausch relaxation in spin glasses above T g Observation of ultra small moment ordering in heavy fermion and organic compounds New insights in to the trapping and detrapping of hydrogen in semiconductors 1S-2S transitions in muonium and challenges to the Standard Model

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002  SR - a universal acronym …..which stands for Muon Spin Rotation, Relaxation Resonance rotation describes the dephasing of muon spins by local magnetic fields with an applied field transverse to the muon spin direction relaxation describes the time-dependent loss of polarisation of the muon spins by internal fields either in zero applied field or in a field applied parallel to the initial muon spin direction resonance is associated with RF induced transitions (cf NMR)

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002 Muon production from pions Charge state  +  - Mean lifetime (s) 26x x10 -9 Spin 0 0 Mass (MeV) Decay mode  +  + +   -  - +  100% polarised “surface” positive muons (~4MeV) are generally used for condensed matter studies

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002 Pion production Single pion production See Eaton and Kilcoyne in “Muon Science” eds Lee, Kilcoyne and Cywinski, MeV eg, proton bombardment of a graphite target

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002 Pulsed muon production at ISIS RAL’s 800MeV, 200mA proton accelerator-based pulsed neutron and muon facility (UK)

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002 Pion production Double pion production See Eaton and Kilcoyne in “Muon Science” eds Lee, Kilcoyne and Cywinski, GeV

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002 Europe’s muon facilities PSI, (Villigen, Switzerland) - a continuous muon source ISIS, (RAL, UK) - a pulsed muon source

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002 Properties of the muon Mass: x M p Charge: + (-) Gyromagnetic ratio: x10 8 s -1 T -1 Lifetime:  s Decay asymmetry: W(  ) = 1+a 0 cos  a o ~0.25

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002 Implanting the muon in a sample ~1-3 mm Implantation is rapid and occurs without loss of muon polarisation

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002 Muon precession and decay

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002 MuSR and Emu, ISIS ( EU sponsored muon facility ) Muon spectrometers

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002 Muon Spin Rotation and Relaxation  F B Rotation B x >0 Relaxation B z or B=0  F B

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002 a-Zr 76 Fe 24 Some science…...muon spin rotation The time evolution of the muon polarisation in a transverse field B is where  L =  B G x (t) is simply the Fourier transform of the field distribution averaged over all muon sites. Muon spin rotation has provided remarkable insights into the nature of the superconducting flux line lattice a-Zr 76 Fe 24 =500nm,  = 29nm, T C =1.7K

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002  = 0.3  s -1 aoao R=  t(  s) Some science....muon spin relaxation G z (t) depends upon the distribution and dynamics of internal fields at the muon site - usually in the absence of applied fields - eg for dynamic Gaussian fields of rms width  and a fluctuation rate : Static (Kubo-Toyabe) limit Dynamic (exponential) limit

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002 Muon spin relaxation - time scales …..and  SR is sufficiently sensitive for ultra-small magnetic moments (~10 -3  B ) to be detected A time window sufficiently wide for studies of fast itinerant electron spin fluctuations through to slow distributed spin relaxation in spin glasses …or of fast muon hopping through to slow diffusional processes….

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002 Spin dynamics in itinerant magnets  Mn 0.94 Al 0.06  Mn 0.85 Al 0.15 Spin liquid phase Stretched exponential µSRSimple exponential µSR Spin glass phase  -Mn an elemental spin fluctuator Stewart and Cywinski PRB59 (1999) 4305 Campbell, Cywinski et al PRL 72 (1994) 1291

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002 Magnetic order in organic magnets Spontaneous muon precession in a coherent internal field at mK temperatures Blundell et al Europhysics Letters 31 (1995) 573

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002 Modelling Hydrogen in Semiconductors Ge GaAs (Zn) GaAs(Si) GaN Muon hopping rates measured over three decades in frequency in Ge, GaAs, GaN and Si- based semconductors Cox, Davis et al, PRL 2001

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002 The future ? - “cold” muons Muons are cryogenically moderated and energy selected to tune localisation depth within the sample: See Morenzoni in “Muon Science” eds Lee, Kilcoyne and Cywinski, 1998

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002 Cold muons at PSI ….but the efficiency is still very low (~10 -5 )

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002 Flux distribution at surface of YBa 2 Cu 3 O 7 simulated measured Niedermayer, Forgan et al PRL83, 3935, 1999 YBa 2 Cu 2 O 7 Ag

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002 The European Spallation Source The future source for European neutron and muon users ? High power (12kW) target for pulsed muon production serving two surface muon channels (several instruments) with only 1.6% beam loss to short pulse target ~ISIS x 100

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002 Muons at ESS The newly constituted European Chapter of the International Society for Muon Spectroscopy has placed the development of a world leading muon facility at the ESS high on its agenda …… ESS offers: High intensity, small beams for high countrate (kinetic?) studies Ultra-small beam size for tomographic studies High intensity for development of analogue counting methods Sufficient intensities for development of rapid scanning RF techniques Routine application of cold muon techniques…….

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002 Conclusions  SR is making an increasingly significant contribution to condensed matter science research There is already strong competition to host the ESS from Lund (Scandinavia), Julich and Halle-Leipzig (Germany) and Yorkshire (UK)…. Emerging techniques, such as cold muon spectroscopy are extending the already broad range of applications…... …and ESS will extend the possibilities still further The European muon community therefore strongly supports the speedy construction of ESS

European Research Infrastructure Symposium - EPS12 Budapest - 27 August 2002 YESS! bringing the European Spallation Source to Yorkshire a world class science facility for a world class region Yorkshire Forward and the White Rose University Consortium