Metallic magnetism and Invar M. Acet Experimentalphysik, Universität Duisburg-Essen.

Slides:



Advertisements
Similar presentations
Acero 2000 PHYSICAL METALLURGY AND THERMAL PROCESSING OF STEEL
Advertisements

Basics of Phases and Phase Transformations W. Püschl University of Vienna.
X-ray Imaging and Spectroscopy of Individual Nanoparticles A. Fraile Rodríguez, F. Nolting Swiss Light Source Paul Scherrer Institut, Switzerland J. Bansmann.
Electromagnetics (ENGR 367) Magnetic Materials & Magnetization.
Metals: Bonding, Conductivity, and Magnetism (Ch. 6)
Diluted Magnetic Semiconductors Diluted Magnetic Semoconductor (DMS) - A ferromagnetic material that can be made by doping of impurities, especially transition.
Chapter 3 -1 ISSUES TO ADDRESS... How do atoms assemble into solid structures? How does the density of a material depend on its structure? When do material.
Chapter 3 The Structure of Crystalline Solids Session I
Electronic structure of La2-xSrxCuO4 calculated by the
UCSD. Tailoring spin interactions in artificial structures Joaquín Fernández-Rossier Work supported by and Spanish Ministry of Education.
Temperature Simulations of Magnetism in Iron R.E. Cohen and S. Pella Carnegie Institution of Washington Methods LAPW:  Spin polarized DFT (collinear)
Computational Materials Science Magnetism and LSDA Peter Mohn Center for Computational Materials Science Vienna University of Technology Vienna, Austria.
Theory of magnetostriction in Invar materials. S. Khmelevskyi Center for Computational Materials Science, Vienna University of Technology P. Mohn, A. V.
Magnetism III: Magnetic Ordering
Honors Biology Mr. Luis A. Velázquez
Magnetic Properties of Materials
Howard H. Liebermann, Ph.D..  Structure of Metals  On atomic level, regular arrangement of atoms immersed in “sea” of “free electrons”.  Results of.
CH 23: METALS. METALS Chapter 23 © 2014 Pearson Education, Inc. Opaque Good conductors of ______ and __________ High ___________ and __________ Metallic.
LEFT CLICK OR PRESS SPACE BAR TO ADVANCE, PRESS P BUTTON TO GO BACK, PRESS ESC BUTTON TO END LEFT CLICK OR PRESS SPACE BAR TO ADVANCE, PRESS P BUTTON.
Chapter 7 Ionic & Metallic Bonding Anything in black letters = write it in your notes (‘knowts’)
Chapter 3 - Algebra and Physics Connections Program for TEA fellows 2015 Feb. 19 & March 5, 9:30 – 11:30 AM, Sims 207 BY Ponn Maheswaranathan, PhD Physics.
NAN ZHENG COURSE: SOLID STATE II INSTRUCTOR: ELBIO DAGOTTO SEMESTER: SPRING 2008 DEPARTMENT OF PHYSICS AND ASTRONOMY THE UNIVERSITY OF TENNESSEE KNOXVILLE.
Colossal Magnetoresistance of Me x Mn 1-x S (Me = Fe, Cr) Sulfides G. A. Petrakovskii et al., JETP Lett. 72, 70 (2000) Y. Morimoto et al., Nature 380,
Magnetism in ultrathin films W. Weber IPCMS Strasbourg.
Byeong-Joo Lee cmse.postech.ac.kr Semi-Empirical Atomistic Simulations in Materials Science and Engineering Byeong-Joo Lee Pohang University of Science.
H. Giefers, University of Paderborn Introduction EHPRG-40 in Edinburgh 7. September 2002 Pressure and Temperature Dependence of the Phonon Density-of-States.
Daresbury Laboratory Ferromagnetism of Transition Metal doped TiN S.C. Lee 1,2, K.R. Lee 1, K.H. Lee 1, Z. Szotek 2, W. Temmerman 2 1 Future Technology.
Starter S-53 Mole Day!. Starter S-55 What is the value of a mole? What is that number used for?
Chapter 3: The Structure of Crystalline Solids
Introduction to Molecular Magnets Jason T. Haraldsen Advanced Solid State II 4/17/2007.
Chapter 3: The Structure of Crystalline Solids
전이금속이 포함된 GaN의 전자구조 및 자기적 특성해석
Crystal Structure of Solids
§2.4 Crystal Structure and Complex Lattice
First Principle Design of Diluted Magnetic Semiconductor: Cu doped GaN
From an Atom to a Solid Photoemission spectra of negative copper clusters versus number of atoms in the cluster. The highest energy peak corres- ponds.
Complex magnetism of small clusters on surfaces An approach from first principles Phivos Mavropoulos IFF, Forschungszentrum Jülich Collaboration: S. Lounis,
1 U N C L A S S I F I E D LANS Company Sensitive — unauthorized release or dissemination prohibited Operated by Los Alamos National Security, LLC for NNSA.
GETTING TO KNOW THE PERDIODIC TABLE. In the periodic table, each row is called period. –There are 7 periods –You sit in rows in your periods. The elements.
2/06/2015PHY 752 Spring Lecture 101 PHY 752 Solid State Physics 11-11:50 AM MWF Olin 107 Plan for Lecture 10: Reading: Chapter in MPM;
Solids  Solids retain their shapes because they have rigid crystal structures.  Based on the attractive forces that hold tem together or on the arrangement.
CHEMICAL BONDING What forces hold atoms and molecules together?
Materials Science Chapter 4 Disorder in solid Phases.
Magnetic properties of (III,Mn)As diluted magnetic semiconductors
Plastic deformation Extension of solid under stress becomes
Topic: Families of Elements PSSA: A/S8.C.1.1.
Kintetic Molecular Theory
Metals & Alloys.
THE SPACE LATTICE AND UNIT CELLS CRYSTAL SYSTEMS AND BRAVAIS LATTICES.
Electromagnetics (ENGR 367)
Basic Metallurgy Tomotsugu Sawai Director
S.-C. Lee*, K.-R. Lee, and K.-H. Lee Computational Science Center
Chapter 19 Coordination Complexes (Nov. 8 and 10)
Chapter 10 Magnetic Properties Introduction 10
Elements Pg Elements Pg Elements Element: __________________________________________________________________________ The number of.
3.14/3.40J/22.71J Recap Basic Crystallography and Miller Indices
Atomic Bonding Primary Bonding: Ionic Bonding, non-directional
Crystallography and Structure
THE BIGGER PICTURE - TRENDS IN REAL SYSTEMS
Quantum complexity in condensed matter physics
Quantum Mechanical Considerations
Starter S-53 Mole Day!.
MATERIALS SCIENCE Materials science investigates the relationships between the structures and properties of materials.
Growth Behavior of Co on Al(001) substrate
METALS Bonds and Properties Alloys Pure Elements.
Litmus lab Get Ready for Bellwork!!!.
Litmus lab Get Ready for Bellwork!!!.
Litmus lab Get Ready for Bellwork!!!.
Chemical Reactivity.
Crystalline Solids (고체의 결정구조)
Presentation transcript:

Metallic magnetism and Invar M. Acet Experimentalphysik, Universität Duisburg-Essen

- Structure of transition metals - Magnetism of transition metals - Magnetic instabilities and ‘Invar’ Outline

Band formation

Structure of the transition elements (elements with ‘wrong’ crystal structures) complex cubicbcchcp bccfcc

Allotropy in the 3d elements

The density of states and non-integral magnetic moment N   N   2.2  B  N  8 BCC Fe

Ferro and antiferromagnetic transition temperatures  -Mn

s+d electrons fcc Mn fcc Fe Rigid band model and the Slater-Pauling curve: Valence electron concentration dependence of the magnetic moment

Invar: Fe 65 Ni 35

Measuring the thermal expansion of the Eifel tower

Thermal expansion of solids ‘normal’ metals invar T (K)

Binding energy vs. atomic volume for a “normal” ferromagnet (schematic) Binding energy vs. atomic volume for “normal” and magnetically unstable ferromagnet (schematic) enhanced “negative” anharmonicity T (K)

What are instabilities at all?

Fe-Ni: Invar to Anti-invar

Summary of Magnetovolume Instabilities positive enhanced anharmonicity negative enhanced anharmonicity “anti-Invar” “Invar”

Moruzzi et al, PRB 39 (1989) Anti-invar in fcc-Fe and fcc-Mn

Cu 2 MnAl Cu2MnSn Mn 3 SnC MnBi MnAl Ag 5 MnAl Mn 3 ZnC Au 4 Mn MnSb MnCrSb Pt 3 Mn Ni 3 Mn … Knowledge of magnetostructural properties vital for material design in - Spintronics - Magnetic shape memory - Nanomagnets Ferromagnetic Mn in a cubic environment