Young-June Kim Department of Physics University of Toronto Resonant Inelastic X-ray Scattering Investigation of Cuprates.

Slides:

Advertisements

Similar presentations

Theory of probing orbitons with RIXS

Advertisements

Isospin Dynamics in Iridates revealed by Resonant inelastic x-ray scattering The Advanced Photon Source is funded by the U.S. Department of Energy, Office.

Iron pnictides: correlated multiorbital systems Belén Valenzuela Instituto de Ciencia de Materiales de Madrid (ICMM-CSIC) ATOMS 2014, Bariloche Maria José.

Level Splitting in Frustrated non-Kramers doublet systems Collin Broholm and Joost van Duijn Department of Physics and Astronomy Johns Hopkins University.

Soft phonon mode and superconducting properties of 2H-NbS2

Spintronics with topological insulator Takehito Yokoyama, Yukio Tanaka *, and Naoto Nagaosa Department of Applied Physics, University of Tokyo, Japan *

Ion Beam Analysis techniques:

Saeedeh Ghaffari Nanofabrication Fall 2011 April 15 1.

Ultrashort Lifetime Expansion for Resonant Inelastic X-ray Scattering Luuk Ament In collaboration with Jeroen van den Brink and Fiona Forte.

Slide: 1 HSC17: Dynamical properties investigated by neutrons and synchrotron X-rays, 16 Sept

Spin dynamics of stripe-ordered layered nickelates Andrew Boothroyd Department of Physics, Oxford University Ni 2+ (S=1) Ni 3+ (S=1/2) Cu 2+ (S=1/2) Cu.

Condensed Matter Physics Research At Extreme Conditions: High Pressure and Pulsed Magnetic Fields The Advanced Photon Source is funded by the U.S. Department.

Hole-Doped Antiferromagnets: Relief of Frustration Through Stripe Formation John Tranquada International Workshop on Frustrated Magnetism September 13.

Some interesting physics in transition metal oxides: charge ordering, orbital ordering and spin-charge separation C. D. Hu Department of physics National.

SDW Induced Charge Stripe Structure in FeTe

M. Hücker Manipulating Competing Order with High Pressure Neutron Scattering Group (CMPMS) Correlated Electron Systems ( Superconductivity, Magnetism,

Interplay between spin, charge, lattice and orbital degrees of freedom Lecture notes Les Houches June 2006 lecture 3 George Sawatzky.

Ψ-k workshop on magnetism in complex systems, 16 th – 19 th April 2009, TU WienM. Stöger-Pollach Detection of magnetic properties on the nanometer scale.

Insights into quantum matter from new experiments Detecting new many body states will require: Atomic scale resolution of magnetic fields Measuring and.

X-ray Emission Spectroscopy Cormac McGuinness Physics Department Trinity College Dublin Soft x-ray emission and resonant inelastic.

Charge Inhomogeneity and Electronic Phase Separation in Layered Cuprate F. C. Chou Center for Condensed Matter Sciences, National Taiwan University National.

DYNAMICAL PROPERTIES OF THE ANISOTROPIC TRIANGULAR QUANTUM

What Pins Stripes in La2-xBaxCuO4? Neutron Scattering Group

1 BROOKHAVEN SCIENCE ASSOCIATES Welcome: Workshop Overview of the Workshop Yong Cai NSLS-II February 7-8, 2008.

First Principles Investigations of Plutonium Americium and their Mixtures using Dynamical Mean Field Theory Washington February 5-8 (2007). Gabriel.Kotliar.

Utilizing the short wavelength of X-ray to study low-energy local excitations q-dependence of the spectral weights and dispersions Wei Ku (BNL & SUNY Stony.

Surface Enhanced Raman Spectroscopy (SERS) Jeanne Bonner PHYS 275 November 26, 2007.

Seminar Author: Bojan Hiti Mentor: doc. dr. Matjaž Kavčič Determination of trace impurities on Si wafers with x-ray fluorescence.

Investigating the mechanism of High Temperature Superconductivity by Oxygen Isotope Substitution Eran Amit Amit Keren Technion- Israel Institute of Technology.

Nonisovalent La substitution in LaySr14-y-xCaxCu24O41: switching the transport from ladders.

Ying Chen Los Alamos National Laboratory Collaborators: Wei Bao Los Alamos National Laboratory Emilio Lorenzo CNRS, Grenoble, France Yiming Qiu National.

X-rays The electric field E(r,t) is given as a cosine function.

NMR evidence for spatial correlations between spin and charge order in (La,Eu) 2-x Sr x CuO 4 Nicholas Hans-Joachim Grafe, Los Alamos.

Ion Beam Analysis Dolly Langa Physics Department, University of Pretoria, South Africa Blane Lomberg Physics Department, University of the Western Cape,

VUV14, July 23, 2004 Electronic structures of Ca induced one-dimensional reconstructions on a Si(111) surface Kazuyuki Sakamoto Dept. Phys., Tohoku University,

Outline Damping mechanisms  Plasmons in ribbons Experimental results Graphene Nanophotonics Benasque, 2013, Mar Mar 08 Momentum dependence and losses.

Slide: 1 IXS with sub-meV resolution: opening new frontiers in the study of the high frequency dynamics Giulio Monaco ESRF, Grenoble (F) outline: High.

Solving Impurity Structures Using Inelastic Neutron Scattering Quantum Magnetism - Pure systems - vacancies - bond impurities Conclusions Collin Broholm*

X-Ray Scattering with synchrotron radiation E. Ercan Alp Advanced Photon Source Argonne National Laboratory, Argonne, Illinois JASS’02, October 19-28,

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.

Electronic Properties of Thin Film Organic Superconductors studied using Synchrotron Radiation-based Soft X-Ray Spectroscopies Kevin E. Smith, Boston University,

Giorgi Ghambashidze Institute of Condensed Matter Physics, Tbilisi State University, GE-0128 Tbilisi, Georgia Muon Spin Rotation Studies of the Pressure.

Neutron Scattering Studies of Tough Quantum Magnetism Problems

Chapter 3 Lattice vibration and crystal thermal properties Shuxi Dai Department of Physics Unit 4 : Experimental measurements of Phonons.

Min Kyu Lee ( 이민규 ) Kyoung Beom Lee ( 이경범 ) Yong-Hamb Kim ( 김용함 ) Low Temperature Detectors 2006 Workshop on the Underground Experiment at Yangyang TEXONO-KIMS.

Photon-in/Photon-out Soft-X-Ray Spectroscopy Soft-X-Ray Absorption (XAS); Soft-X-Ray Emission (XES) Resonant Inelastic Soft-X-Ray Scattering (RIXS) Jinghua.

Infrared and magneto- optical studies of topological insulators Saša V. Ðorđević Department of Physics.

Electron Energy Loss Spectroscopy (EELS) Suggested Reading: Used electron spectrometer Used TEM Review of theory for elastic + inelastic scattering Examples.

Raman Scattering As a Probe of Unconventional Electron Dynamics in the Cuprates Raman Scattering As a Probe of Unconventional Electron Dynamics in the.

Inelastic Scattering: Neutrons vs X-rays Stephen Shapiro Condensed Matter Physics/Materials Science February 7,2008.

Lecture 21 Optical properties. Incoming lightReflected light Transmitted light Absorbed light Heat Light impinging onto an object (material) can be absorbed,

Past and Future Insights from Neutron Scattering Collin Broholm * Johns Hopkins University and NIST Center for Neutron Research  Virtues and Limitations.

Magnon Another Carrier of Thermal Conductivity

Next Generation Science with Inelastic X-ray Scattering

Antiferromagnetic Resonances and Lattice & Electronic Anisotropy Effects in Detwinned La 2-x Sr x CuO 4 Crystals Crystals: Yoichi Ando & Seiki Komyia Adrian.

Brookhaven Science Associates U.S. Department of Energy Chi-Chang Kao National Synchrotron Light Source Brookhaven National Laboratory Recent Developments.

High Resolution Energy Loss Spectroscopy of “Sheet” Plasmons Roy F. Willis, Department of Physics, The Pennsylvania State University University Park, PA.

Frustrated magnetism in 2D Collin Broholm Johns Hopkins University & NIST  Introduction Two types of antiferromagnets Experimental tools  Frustrated.

Structure and dynamics of spin polarons induced by doping a Haldane spin-1 chain Collin Broholm * Johns Hopkins University and NIST Center for Neutron.

1.Introduction 2.Vortex Nernst effect 3.Enhanced Diamagnetism 4.Fragile London rigidity T>Tc 5.Low-temp. Quantum Vortex Liquid State Vorticity and the.

One Dimensional Magnetic Systems Strong Fluctuations in Condensed Matter Magnetism in one dimension Pure systems Doped systems Magnetized states Conclusions.

Search for New Topological Insulator Materials April 14, 2011 at NTNU Hsin Lin Northeastern University.

Solving Impurity Structures Using Inelastic Neutron Scattering Quantum Magnetism - Pure systems - vacancies - bond impurities Conclusions Collin Broholm*

Angle-resolved photoemission spectroscopy (ARPES)

Raman Effect The Scattering of electromagnetic radiation by matter with a change of frequency.

Tutorial on Quanty at ESRF Intro

Bumsoo Kyung, Vasyl Hankevych, and André-Marie Tremblay

X-ray Emission Spectroscopy

Diagnosis of a High Harmonic Beam Using

Neutron studies of iron-based superconductors

Presentation transcript:

Young-June Kim Department of Physics University of Toronto Resonant Inelastic X-ray Scattering Investigation of Cuprates

NSLS-II Workshop Feb 2008 Young-June Kim Outline Resonant IXS What is indirect RIXS? Considering outgoing resonance response function? but there is more Charge transfer excitation (> 2 eV) Orbital selective d-d excitation (< 2eV) Multi-magnon excitation (< 1eV) Conclusions and Outlook

NSLS-II Workshop Feb 2008 Young-June Kim Experimental Setup overall energy resolution: ~130 meV (FWHM) 9ID Advanced Photon Source Si(111) Si(444) channel-cut Analyzer Ge(733) Detector Sample

NSLS-II Workshop Feb 2008 Young-June Kim MERIX spectrometer credit: Yuri Shvydko

NSLS-II Workshop Feb 2008 Young-June Kim Incident energy dependence La 2 CuO 4 Brillouin zone center

NSLS-II Workshop Feb 2008 Young-June Kim Third order theory Collapse onto a single curve Abbamonte et al. 1999

NSLS-II Workshop Feb 2008 Young-June Kim E i -independent spectrum Dielectric loss function from ellipsometry EELS Theory (van den Brink and van Veenendaal)

NSLS-II Workshop Feb 2008 Young-June Kim E i -independent spectrum Dielectric loss function from ellipsometry EELS Theory (van den Brink and van Veenendaal) S(q=0,  ) ~

NSLS-II Workshop Feb 2008 Young-June Kim How about other cuprates?

NSLS-II Workshop Feb 2008 Young-June Kim La 2 CuO 4 Momentum dependence q Q Ellis et al. PRB in pressKim et al. PRB 2007

NSLS-II Workshop Feb 2008 Young-June Kim Comparison with L and M edges M 2,3 -edge (Kuiper et al. 1998) L 3 -edge (Ghiringelli et al. 2004)

NSLS-II Workshop Feb 2008 Young-June Kim dd excitation using hard X-ray Going to very large Q Using quadrupole transition as an intermediate state Larson et al., PRL 2007 Sr 2 CuO 3 - Seo et al., PRB 2006

NSLS-II Workshop Feb 2008 Young-June Kim d-d excitation in Sr 2 CuO 2 Cl 2 pre-edge (quadrupole) intermediate state

NSLS-II Workshop Feb 2008 Young-June Kim Magnetic Excitation? La 2 CuO 4 on-resonance off-resonance  Hill et al. PRL in press

NSLS-II Workshop Feb 2008 Young-June Kim Doping Momentum

NSLS-II Workshop Feb 2008 Young-June Kim Possibilities? Two magnon excitation Donkov+Chubukov PRB 2007 Vernay et al. PRB 2007

NSLS-II Workshop Feb 2008 Young-June Kim More possibilities? Charge 2e boson (Choy, Leigh, and P. Phillips) What about d-d excitation? d(3z 2 -r 2 ) to d(x 2 -y 2 ) is not experimentally identified yet in cuprates But…  t Im[1/  (q,  )]

NSLS-II Workshop Feb 2008 Young-June Kim Perhaps in the future? Cvetkovic et al., cond-mat/ Lee and Nagaosa, PRB 2003 CeB6, Zirngiebl et al. PRB 1984

NSLS-II Workshop Feb 2008 Young-June Kim Old instrumentation (1m) New instrumentation (2m)

NSLS-II Workshop Feb 2008 Young-June Kim NSLS-II wish list Improved energy resolution meV resolution will allow us to study excitations in the meV range Pseudo gap in high Tc superconductors Magnetic excitation Crystal field in Rare-earths Magnon-phonon-electron interaction Smaller beam size (20 nm?) Scanning IXS? Probing electronic structure in inhomogeneous sample

NSLS-II Workshop Feb 2008 Young-June Kim Conclusion and Outlook Resonant Inelastic X-ray Scattering can probe d-d orbital excitations Charge-transfer gap Dispersion bandwidth Perhaps magnetic excitation Needs more work Mid-IR excitation at ( , 0) In La 2-x Sr x CuO 4  two magnon? Future: Fermi surface probe? Needs energy resolution improvement ~1.8 eV For La 2 CuO 4 ~2.2 eV ~0.3 eV ~0.5 eV

NSLS-II Workshop Feb 2008 Young-June Kim Thanks to Toronto Jung Ho Kim David Ellis John P. Hill (BNL) Girsh Blumberg (Lucent) APS XOR T. Gog D. Casa Y. Shvydko Samples N. Motoyama, K. M. Kojima, and S. Uchida (U. Tokyo) F. C. Chou (MIT) S. Wakimoto (JAEA) G. Gu, M. Huecker (BNL) S. Komiya, Y. Ando (CRIEPI) H. Zhang (Toronto)