Micromagnetic Simulations of Systems with Shape-Induced Anisotropy

Slides:



Advertisements
Similar presentations
Introduction Landau Theory Many phase transitions exhibit similar behaviors: critical temperature, order parameter… Can one find a rather simple unifying.
Advertisements

2Instituto de Ciencia de Materiales de Madrid,
Some New Geometric Phase Effects in Mn 12 Variants Jonathan Friedman Eduardo H. da Silva Neto Michael Foss-Feig Amherst College Funding: NSF, Research.
Quantum Critical Behavior of Disordered Itinerant Ferromagnets D. Belitz – University of Oregon, USA T.R. Kirkpatrick – University of Maryland, USA M.T.
Optical Control of Magnetization and Modeling Dynamics Tom Ostler Dept. of Physics, The University of York, York, United Kingdom.
Kinetics of ordering and metastable phase of alloys Jun Ni Department of Physics Tsinghua University.
Topics in Magnetism III. Hysteresis and Domains
Temperature Simulations of Magnetism in Iron R.E. Cohen and S. Pella Carnegie Institution of Washington Methods LAPW:  Spin polarized DFT (collinear)
Introduction to Micromagnetic Simulation
Computer Simulations, Scaling and the Prediction of Nucleation Rates
H. C. Siegmann, C. Stamm, I. Tudosa, Y. Acremann ( Stanford ) On the Ultimate Speed of Magnetic Switching Joachim Stöhr Stanford Synchrotron Radiation.
The Scaling of Nucleation Rates Barbara Hale Physics Department and Cloud and Aerosol Sciences Laboratory University of Missouri – Rolla Rolla, MO
Y. Acremann, Sara Gamble, Mark Burkhardt ( SLAC/Stanford ) Exploring Ultrafast Excitations in Solids with Pulsed e-Beams Joachim Stöhr and Hans Siegmann.
Nuclear spin irreversible dynamics in crystals of magnetic molecules Alexander Burin Department of Chemistry, Tulane University.
Physics of Graphene A. M. Tsvelik. Graphene – a sheet of carbon atoms The spectrum is well described by the tight- binding Hamiltonian on a hexagonal.
Topics in Magnetism II. Models of Ferromagnetism Anne Reilly Department of Physics College of William and Mary.
Random Field Ising Model on Small-World Networks Seung Woo Son, Hawoong Jeong 1 and Jae Dong Noh 2 1 Dept. Physics, Korea Advanced Institute Science and.
Christian Stamm Stanford Synchrotron Radiation Laboratory Stanford Linear Accelerator Center I. Tudosa, H.-C. Siegmann, J. Stöhr (SLAC/SSRL) A. Vaterlaus.
Magnetic Data Storage. 5 nm Optimum Hard Disk Reading Head.
Spins, Effective Spins, Spin Relaxation, Non-Radiative Transitions and all that Marshall Stoneham.
ChE 452 Lecture 24 Reactions As Collisions 1. According To Collision Theory 2 (Equation 7.10)
Lecture 12: Domains, nucleation and coarsening Outline: domain walls nucleation coarsening.
Apparent sixfold configurational anisotropy and spatial confinement of ferromagnetic resonances in hexagonal magnetic antidot lattices V. N. Krivoruchko.
Magnetism and Magnetic Materials DTU (10313) – 10 ECTS KU – 7.5 ECTS Module 6 18/02/2011 Micromagnetism I Mesoscale – nm-  m Reference material: Blundell,
An Electron Trapped in A Potential Well Probability densities for an infinite well Solve Schrödinger equation outside the well.
Magnetization dynamics
8. Selected Applications. Applications of Monte Carlo Method Structural and thermodynamic properties of matter [gas, liquid, solid, polymers, (bio)-macro-
Elastic collisions. Spin exchange. Magnetization is conserved. Inelastic collisions. Magnetization is free. Magnetic properties of a dipolar BEC loaded.
LONG-LIVED QUANTUM MEMORY USING NUCLEAR SPINS A. Sinatra, G. Reinaudi, F. Laloë (ENS, Paris) Laboratoire Kastler Brossel A. Dantan, E. Giacobino, M. Pinard.
  Satyendra Prakash Pal DEPARTMENT OF PHYSICAL SCIENCES
Slide # 1 Variation of PL with temperature and doping With increase in temperature: –Lattice spacing increases so bandgap reduces, peak shift to higher.
Meta-stable Sites in Amorphous Carbon Generated by Rapid Quenching of Liquid Diamond Seung-Hyeob Lee, Seung-Cheol Lee, Kwang-Ryeol Lee, Kyu-Hwan Lee, and.
Experimental determination of Universal Thermodynamic Functions for a Unitary Fermi Gas Takashi Mukaiyama Japan Science Technology Agency, ERATO University.
Quasi-1D antiferromagnets in a magnetic field a DMRG study Institute of Theoretical Physics University of Lausanne Switzerland G. Fath.
J.P. Eisenstein, Caltech, DMR If it were not for the Coulomb repulsion between electrons, iron would not be ferromagnetic. It would instead be.
M. Ueda, T. Yamasaki, and S. Maegawa Kyoto University Magnetic resonance of Fe8 at low temperatures in the transverse field.
Korea Institute of Science and Technology Seung-Hyeob Lee, Churl-Seung Lee, Seung-Cheol Lee, Kyu-Hwan Lee, and Kwang-Ryeol Lee Future Technology Research.
Slow Dynamics of Magnetic Nanoparticle Systems: Memory effects P. E. Jönsson, M. Sasaki and H. Takayama ISSP, Tokyo University Co-workers: H. Mamiya and.
Spatial distributions in a cold strontium Rydberg gas Graham Lochead.
Universität Karlsruhe Phys. Rev. Lett. 97, (2006)
Antiferromagnetic Resonances and Lattice & Electronic Anisotropy Effects in Detwinned La 2-x Sr x CuO 4 Crystals Crystals: Yoichi Ando & Seiki Komyia Adrian.
Effects of Arrays arrangements in nano-patterned thin film media
Spin Wave Model to study multilayered magnetic materials Sarah McIntyre.
Muons, Inc. 14 Jan 2010 S. Kahn--IR Quads 1 IR Quadrupoles with Exotic Materials Steve Kahn, Muons Inc. Bob Palmer, BNL Don Summers, Ole Miss.
Eutectic Phase Diagram NOTE: at a given overall composition (say: X), both the relative amounts.
Theory of Nanoscale Friction Theory of Nanoscale Friction Mykhaylo Evstigneev CAP Congress University of Ottawa June 14, 2016.
Atomic Simulation Term Report Thur. POSTECH M.S.E Kim Kyeong-Min.
Spin-Orbit Torques from Interfacial Rashba-Edelstein Effects
Single reservoir heat engine: controlling the spin
Magnetization dynamics in dipolar chromium BECs
Fig. 7 from Soft-error tolerance and energy consumption evaluation of embedded computer with magnetic random access memory in practical systems using computer.
Salle de séminaire, IJL-Vandoeuvre Entrée 2A 4éme Etage
Common features of glassy models
Coarsening dynamics Harry Cheung 2 Nov 2017.
14. TMMC, Flat-Histogram and Wang-Landau Method
Algorithms and Software for Large-Scale Simulation of Reactive Systems
Superparamagnetic limit, where magnetic particles
Novel quantum states in spin-orbit coupled quantum gases
Experiment Experiment: thing ferromagnetic films
Alternating Antisymmetric Interaction in Nanoscale Iron Ring
Compact Modeling of MTJs for use in STT-MRAM
Quantum World at Atomic Scale:
Zacharias G. Fthenakis, Zhen Zhu and David Tománek
Feasibility Study of the Polarized 6Li ion Source
FIG. 7. Simulated edge localized mode magnetization and phase distributions at the 2.4 GHz resonance (top panels) and 3.6 GHz resonance (bottom panels)
Algorithms and Software for Large-Scale Simulation of Reactive Systems
郑 公 平 河南师范大学 第五届全国冷原子物理和量子信息青年学者学术讨论会
Ion-beam, photon and hyperfine methods in nano-structured materials
P. He1,4, X. Ma2, J. W. Zhang4, H. B. Zhao2,3, G. Lupke2, Z
Information Storage and Spintronics 18
Presentation transcript:

Micromagnetic Simulations of Systems with Shape-Induced Anisotropy S. Hill Thompson Florida State University

Manufactured Single-Domain Iron Nanopillars Grown by STM-assisted CVD 1 200 nm 40 nm 1 S. Wirth, M. Field, D. D. Awschalom, and S. von Molnar, Phys. Rev. B 57, R14028 (1998); J. Appl. Phys. 85, 5249 (1999)

Background – A Typical Simulation Time(scaled units) Mz

Metastable Decay Free energy vs. Mz Saddle point Free energy barrier Metastable minimum +Mz Free energy vs. Mz

Lattice Dynamic equation, Landau-Lifshitz-Gilbert (LLG) on a computational lattice

Landau-Lifshitz-Gilbert (LLG) : uniform magnetization density go: electron gyromagnetic ratio, 1.67x107 Hz/Oe a: phenomenological damping parameter, 0.1 : total local field at = z e d a n +

Rescaling M = M/Ms H = H/Ms r = r/le t = γoMst

Dipole interactions Handled by the Fast Multipole Method O(n2) O(n)

Realistic Models – Computational Details 6x6x90 computational lattice -> 3240 sites 10 nm x 10 nm x 150 nm Fe nanopillar dt = 0.083 picoseconds usin first-order Euler integration Temperature = 20 Kelvin Applied Field = 3160 Oe at 75 degrees from the easy axis Fields: dipole-dipole, thermal, exchange, Zeeman 3-4 days on IBM SP3 using 20 processors

Cumulative Distribution Function of the Lifetime t – All Runs

Phase Plot of the Total Magnetization Faster Mode Slower Mode

Phase Plot of the Total Energy Faster Mode Slower Mode

Two Distributions Fast Slow

Thermalization out of the T=0K Metastable State Quenched Slower mode

Thermalization T = 0K T = 20K

Quench/Relax vs Slow Mode Q/R Slow

Projective Dynamics Number of visits, N Growth Probability = G/N Same, N – (G + S) Shrinkage, S Growth, G Mz Growth Probability = G/N Shrinkage Probability = S/N

Projective Dynamics Slower mode Faster mode

Location of Extrema

Choosing the Correct Model 7x7x101 spins 1x1x17 spins Stoner-Wohlfarth 1-D models are not sufficient, full 3-D models are necessary Wirth, et al, J. Appl. Phys. 85, 5249 (1999). Li, et al, J. Appl Phys, 93, 7912 (2003). Li, et al, J. Appl. Phys. Lett 80, 4644 (2002)