Crucial interactions in BaIrO 3 : Spin-orbit coupling and Coulomb correlation W.W. Ju ( 琚伟伟 ) and Z. Q. Yang*( 杨中芹 ) Abstract The electronic structures.

Slides:



Advertisements
Similar presentations
CECAM workshop on Actinides, Manchester, June DFT+U calculations of the electronic structure of perfect and defective PuO 2 Eugene Kotomin and Denis.
Advertisements

CHAPTER 9 Beyond Hydrogen Atom
Microscopic time-dependent analysis of neutrons transfers at low-energy nuclear reactions with spherical and deformed nuclei V.V. Samarin.
Magnetism in 4d perovskite oxides Phillip Barton 05/28/10 MTRL 286G Final Presentation.
Physics “Advanced Electronic Structure” Lecture 3. Improvements of DFT Contents: 1. LDA+U. 2. LDA+DMFT. 3. Supplements: Self-interaction corrections,
Electronic structure of La2-xSrxCuO4 calculated by the
U N C L A S S I F I E D Operated by the Los Alamos National Security, LLC for the DOE/NNSA Suppression of Spin Diffusion: Modeling and Simulations Gennady.
Spin Excitations and Spin Damping in Ultrathin Ferromagnets D. L. Mills Department of Physics and Astronomy University of California Irvine, California.
Single Particle Energies
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Quasiparticle anomalies near ferromagnetic instability A. A. Katanin A. P. Kampf V. Yu. Irkhin Stuttgart-Augsburg-Ekaterinburg 2004.
Electronic structure and spectral properties of actinides: f-electron challenge Alexander Shick Institute of Physics, Academy of Sciences of the Czech.
Experimental observation of the Spin-Hall Effect in InGaN/GaN superlattices Student : Hsiu-Ju, Chang Advisor : Yang Fang, Chen.
Topics in Magnetism II. Models of Ferromagnetism Anne Reilly Department of Physics College of William and Mary.
Will the orbital energies for multielectron atoms depend on their angular momentum quantum number ℓ? (A) In the H atom, the orbital energies depend on.
Is graphene a strongly correlated electron system ? Antonio H. Castro Neto Buzios, August 2008.
Yoshida Lab M1 Yoshitaka Mino. C ONTENTS Computational Materials Design First-principles calculation Local Density Approximation (LDA) Self-Interaction.
Chapter 41 Atomic Structure
Collinear laser spectroscopy of 42g,mSc
Atomic-scale Engeered Spins at a Surface
Orbitals and Quantum Numbers. Objective Students will be able to describe the quantum numbers n, l, and m l used to define an orbital in an atom, and.
Pressure effect on electrical conductivity of Mott insulator “Ba 2 IrO 4 ” Shimizu lab. ORII Daisuke 1.
Magnetism Physics T Soft Gamma Repeater , is the most powerful known magnetic object in the universe. Only 10 of these unusual objects.
Dr. Nicolae Atodiresei (Molecular Electronics & Spintronics Subgroup in the Peter Grünberg Institut and Institute for Advanced Simulation, Jülich, Germany.)
Lecture 16: Beta Decay Spectrum 29/10/2003 (and related processes...) Goals: understand the shape of the energy spectrum total decay rate sheds.
Structural changes in rare-gas cluster cations. Aleš Vítek, František Karlický, René Kalus Department of Physics, University of Ostrava, Ostrava, Czech.
Chapter 10 Atomic Structure and Atomic Spectra. Spectra of complex atoms Energy levels not solely given by energies of orbitals Electrons interact and.
The first principle calculation study on half-metallic spinel My research work: Presenter: Min Feng Advisor: Professor Xu Zuo College of Information Technical.
¶ CNISM-Dipartimento di Fisica “A. Volta,” Università di Pavia, Pavia, (Italy) ║ Max Planck Institute for Chemical Physics of Solids, Dresden,
FZU Comparison of Mn doped GaAs, ZnSe, and LiZnAs dilute magnetic semiconductors J.Mašek, J. Kudrnovský, F. Máca, and T. Jungwirth.
 Nature of nuclear forces, cont.  Nuclear Models lecture 3&4.
Drude weight and optical conductivity of doped graphene Giovanni Vignale, University of Missouri-Columbia, DMR The frequency of long wavelength.
Hψ = E ψ Hamiltonian for the H atom. The wave function is usually represented by ψ.
Exchange splitting in electronic states of single atoms and magnetic coupling in single dimers and trimers on a surface Mats Persson (1), Hyo-June Lee.
Wigner molecules in carbon-nanotube quantum dots Massimo Rontani and Andrea Secchi S3, Istituto di Nanoscienze – CNR, Modena, Italy.
Fujian Provincial Key Subject of Condensed Matter Physics * Corresponding author: Prof. Zhigao Huang First-principles study of the.
Title: Multiferroics 台灣大學物理系 胡崇德 (C. D. Hu) Abstract
Ferroelectricity induced by collinear magnetic order in Ising spin chain Yoshida lab Ryota Omichi.
The Electronic Structure of the Ti4O7 Magneli Phase
Helical Spin Order in SrFeO 3 and BaFeO 3 Zhi Li Yukawa Institute for Theoretical Physics (YITP) Collaborator: Robert Laskowski (Vienna Univ.) Toshiaki.
The Structure and Dynamics of Solids
鄭弘泰 國家理論中心 (清華大學) 28 Aug, 2003, 東華大學
Magnetism and Magnetic Materials DTU (10313) – 10 ECTS KU – 7.5 ECTS Sub-atomic – pm-nm With some surrounding environment and a first step towards the.
Complex magnetism of small clusters on surfaces An approach from first principles Phivos Mavropoulos IFF, Forschungszentrum Jülich Collaboration: S. Lounis,
The Quantum Theory of Magnetism Carlo Maria Canali Linnaeus University 7 December 2011 – Lecture 21.
Flat Band Nanostructures Vito Scarola
Evolution of the orbital Peierls state with doping
Correlation in graphene and graphite: electrons and phonons C. Attaccalite, M. Lazzeri, L. Wirtz, F. Mauri, and A. Rubio.
Electron-Phonon Coupling in graphene Claudio Attaccalite Trieste 10/01/2009.
At first Hww is neglected, for each electron we get a hydrogen problem
The role of isospin symmetry in medium-mass N ~ Z nuclei
Orbitals and Quantum Numbers
Structure and dynamics from the time-dependent Hartree-Fock model
CHAPTER 12 The Atomic Nucleus
Half-Metallic Ferromagnetism in Fe-doped Zn3P2 From First-Principles Calculations G. JAI GANESH and S. MATHI JAYA Materials Science Group, Indira Gandhi.
Effects of Si on the Electronic Properties of the Clathrates
Bumsoo Kyung, Vasyl Hankevych, and André-Marie Tremblay
Novel quantum states in spin-orbit coupled quantum gases
Hydrogen relativistic effects II
Carbon Nanotube Diode Design
S.Li (李晟) and Z.Q.Yang (杨中芹)
Theory of Magnetic Moment in Iron Pnictides (LaOFeAs) Jiansheng Wu (UIUC), Philip Phillips (UIUC) and A.H.Castro Neto (BU) arxiv:
Consider the He atom. The Hamiltonian is
Ⅱ HOMO-LUMO gap and dispersion of HOMO
Pressure-induced spin-state and insulator-metal transition in Sr2CoO3F by first principles Xue-dong Ou and Hua Wu We have studied the electronic structure.
Multielectron Atoms The quantum mechanics approach for treating multielectrom atoms is one of successive approximations The first approximation is to treat.
Status of FEL Physics Research Worldwide  Claudio Pellegrini, UCLA April 23, 2002 Review of Basic FEL physical properties and definition of important.
Spin-orbit coupling and coupled charge-spin-orbital state in iridates
Deformation of the Fermi surface in the
Better approximations:
Presentation transcript:

Crucial interactions in BaIrO 3 : Spin-orbit coupling and Coulomb correlation W.W. Ju ( 琚伟伟 ) and Z. Q. Yang*( 杨中芹 ) Abstract The electronic structures of perovskite-like BaIrO 3 are investigated using local spin density approximation (LSDA) as well as the LSDA plus Hubbard U (LSDA+U) scheme. The ferromagnetic ground state can be obtained only when the on-site Coulomb interaction is considered. The spin-orbit coupling (SOC) can not be neglected due to the existence of orbital angular momentum on Ir 5d electrons, as have been found recently (PRL105, (2010)). The calculations including SOC and on-site Coulomb interaction can give the proper spin and orbital magnetic moments, in agreement with the experimental results. Crystal structure and Method Space group: C2/m (No.12) Unit cell parameters: a= Å b=5.7514Å c= Å β= o Feature: Two kinds nonequivalent Ir 3 O 12 clusters made of face-sharing IrO 6 octahedra, connected by corner sharing and long axis are tilted by about 12 o Magnetic property: Ferromagnetic ground state Method: Local spin density approximation (LSDA) On-site Coulomb interaction U on Ir 5d orbital Spin-orbit coupling (SOC) Results The upper table presents the relative values of total energies for ferromagnetic (FM) state and nonmagnetic (NM) state based on L(S)DA and L(S)DA+U method. The L(S)DA+U calculations give relatively large energy difference stabilizing the FM ground state of BaIrO 3. The energy difference becomes larger with the U value increasing, which distinctly suggests on-site Coulomb interaction is indispensable in correctly describing the electronic structures of BaIrO 3. The spin and orbital magnetic moments of each Ir atom within different calculation methods are presented in the lower table. The spin magnetic moments of each Ir atom remarkably decrease after SOC effect is considered. When on-site Coulomb interaction (U=1.5 eV) and SOC are synchronously considered, spin and orbital magnetic moments of Ir atoms can almost accord with the experimental results. Discussion The comparison of PDOS with and without SOC may shed light on the question why SOC can produce notable influence on the magnetism of Ir atoms. The SOC influences DOS distribution of Ir-5d orbitals, making them become broader in the vicinity of the fermi level. The extended electron distributions not only strengthen direct Ir-Ir interaction but also enhance hybridization between the Ir 5d and O 2p, leading to the decrease of spin magnetic moments of Ir atoms. Strong 5d-2p hybridization and a small exchange splitting on 5d orbitals were believed to be the reasons of small Ir moments in previous study, but our results indicate they are also suppressed by SOC effect and direct Ir-Ir interaction. Conclusions I. The electronic structures of BaIrO 3 have been studied by first-principles calculations within LSDA+U+SOC method. II. The On-site Coulomb interaction is important to obtain the magnetic ground state of BaIrO 3. III. The SOC effect play an important role in the investigation on the magnetic properties of this compound. References (1) M. A. Laguna-Marco, D. Haskel, et. al.,Phys. Rev. Lett. 105, (2010). (2) G. Cao, J. E. Crow, el. al.,Solid State Commun. 113, 657 (2000).