Quantum Hall Ferromagnets-I Les Houches June 2006 University of Texas at Austin Ramin Abolfath Luis Brey Anton Burkov Rene Cote Jim Eisenstein Herb Fertig Steve Girvin Charles Hanna Tomas Jungwirth Kentaro Nomura Leo Radzihovksy (Doug) Rajaraman Mark Rasolt Jairo Sinova Kun Yang
A Few Remarks About `Ordinary’ Magnetism
Magnetism in Atomic Physics Electrons are Fermions Magnetism due to Fermi Statistics and spin-independent interactions Make all orbitals in an open shell as similar to each other as possible
Magnetism in Insulators A playground for strongly-correlated electron physics
Magnetism in Metals – Hubbard Picture Doubles - Interaction Energy Cost U Empties Simple model – Sophisticated QF Theory Possible
Itinerant Electron Ferromagnetism Bloch-Stoner Picture E = E 0 + M 2/D(EF) - Δ M 2 xc E Singly Occupied Orbitals
DOS d s E μ μ
Itinerant Electron Ferromagnetism Spin-Density Functional Theory One very successful picture of transition metal ferromagnetism is Density Functional Theory. Hohenberg-Kohn Theorem Kohn-Sham Trick E= E[n, m]= Es[n, m]+Exc[n, m] v = ves + vxc B = D[n, m] m/m Local Spin-Density Approx.
Stoner Criterion - Elements Δ
Itinerant Electron Ferromagnetism Spin-Density Functional Theory of Itinerant Electron Magnetism JÜRGEN KÜBLER, Institute of Solid State Physics Darmstadt University of Technology
Itinerant Electron Ferromagnetism Quasiparticle and Collective Aspects Majority Spins Minority Spins Q Fermi Surface Singly Occupied Orbitals ph spin flip Spin Wave Collective Q E
Micromagnetics Dipole-Dipole Interactions Direction of Magnetization
Micromagnetics
A Few Remarks About Spintronics
SPIN (Elec)TRONICS = Spin-Torques + Spin-Orbit (AHE+Spin-Galvanic) + Magnetic Semiconductors
GMR TMR and Spin Torques Dan Ralph – KITP Spintronics Program Talk www. kitp. ucsb. edu
Hard-disk Technology 10 GByte/(person. year)
A Few Remarks About the Quantum Hall Effect
Quantum Wells Al. Ga. As Al. Ga. As - e- Ga energy As Si 100 A Quantum Well Double Quantum Well
Landau Levels Cyclotron Orbit
Integer Quantum Hall Effect xx xy/(h/e 2)
Incompressible States & Streda Formula Compressibility Edge Current Conductance and LL degeneracy
Integer Quantum Hall Effect xx xy/(h/e 2)
QHF- Stoner-Criterion Landau Band Landau-Level Exchange Energy
QHF- Stoner-Criterion Maude et al. PRB (2005)
Landau Levels - Really! (Ashoori – MIT)
Next Time: • Skyrmions • QHF Anistropy – Ising or XY • QHF in Graphene • Pseudo-spin Transfer Torques