Title: Effects of spinorbit coupling on the electronic structure of surfaces
1Effects of spin-orbit coupling on the electronic
structure of surfaces
- Jürgen Henk
- Theory Department
- Max Planck Institute of Microstructure Physics
- Halle (Saale), Germany
2Outline
- Spin-orbit coupling (SOC)
- Effects of SOC on the electronic structure
- Band structure and magnetic dichroism of Fe
- Ab-initio theory
- Electronic structure calculations
- Photoemission calculations
- SOC at surfaces
- Rashba-Bychkov effect in 2DEGs
- Au(111)
- Bi/Ag(111)
- Summary and outlook
3Spin-orbit coupling
Electron in a magnetic field
Relativistic motion ? spin precession
Magnetic moment
Hamiltonian
Why spin-orbit coupling? Central potential
Angular momentum (orbital motion)
Spin
4Effect of SOC on the band structure
Fe, 110 direction
Without SOC
With SOC
Lifting of degeneracies -depends on the
magnetization direction
Exchange splitting
Origin of the magneto-crystalline anisotropy (MCA)
Pure spin states
Spin mixing
Tiny changes ? very accurate computations
5Effect of SOC on the band structure
Without SOC
With SOC
6Magnetic linear dichroism
Probing hybridization by angle-resolved
photoemission MD Change of the photocurrent
upon reversal of the magnetization
MLD in normal emission
Fe(110)
- Rampe, G. Güntherodt, D. Hartmann, JH, T.
Scheunemann, R. Feder - Phys. Rev. B 57 (1998) 14370
7Magnetic linear dichroism
Hot spots in Fe(110) Hybridization
and
D
B
D
B
C
A
Change of the character SOC
Valence-band structure
8Magnetic linear dichroism
Energy dependence _at_ Eb 0.5 eV
PE spectra
Theory
Experiment
B
B
Photon energy
Identification of SOC-induced hybridization (hot
spots)
9Summary Spin-orbit coupling
- Electronic structure
- Band gaps
- Hybridization of both orbital and spin
components - ? Magneto-crystalline anisotropy
- Electron spectroscopies
- Spin-polarized low-energy electron diffraction
(SPLEED) - Mott scattering
- Photoemission
- Spin polarization of photoelectrons
- Magnetic dichroism
What about SOC at surfaces? Are there special
effects being not present in the bulk?
10Electronic-structure calculations
- Description of the electronic structure
- Solution of the many-body problem
- Density-functional theory (DFT)
- Local spin-density approximation (LSDA)
- Parameter-free (ab initio)
- Reduction to a single-particle problem
- Effective potential contains many-particle
effects - Kohn-Sham equations (self-consistent)
- Correlation better described than in Hartree-Fock
approximation - Quantities ground state
- Total energy
- Electron density
- Magnetization density
Walter Kohn Nobel prize 1998
11Spin-orbit coupling
- Relativistic calculations
- Dirac equation instead of the Schrödinger
equation - SOC and magnetism treated on equal footing
- Basis for the photoemission calculations
12Multiple-scattering theory
- Successive computation of the scattering
properties - Free electrons - atom - layer stack of layers -
solid - Flexible low-dimensional systems
- Surfaces, thin films, adatoms,
- Numerical realization layer Korringa-Kohn-Rostoke
r method - Computer program package omni2k for electron
spectroscopies
13Photoemission theory
- One-step model Excitation and transport are
coherent processes - Spin-density matrix
- ?? time-reversed SPLEED state (electron
diffraction) - Photocurrent and spin
polarization - Golden rule
- Sudden approximation Interaction of the
photoelectron with the remaining system is
neglected
Feynman diagram
14Summary Ab-initio theory
- Electronic structure calculations
- Density-functional theory (DFT)
- Local spin-density approximation (LSDA)
- Spin-polarized relativistic layer KKR method
- ? SOC and magnetism treated on equal footing
- Photoemisison calculations
- Spin- and angle-resolved photoelectron
spectroscopy (SPARPES) - One-step model
- Input from the DFTLSDA calculations
Application to Au(111) and Bi/Ag(111)
15Rashba-Bychkov effect in a 2DEG
Rashba-Bychkov effect spin splitting due to
spin-orbit coupling (SOC) in a two-dimensional
electron gas (2DEG)
- Interface
- Band bending
- Asymmetric confinement of the 2DEG
- Spin splitting due to SOC
Interface in a semiconductor heterostructure
2DEG
- Structural inversion asymmetry (SIA)
- Non-centrosymmetric solids
- Interfaces
Asymmetric confinement
Rashba-Bychkov effect at a metal surface?
16Rashba-Bychkov effect at a surface
Structural inversion asymmetry
- Surface
- Band gap surface barrier
- Asymmetric confinement of the surface state
- Spin splitting due to SOC
Metal surface
Surface state
Band gap
- Ingredients
- Asymmetric confinement (SIA)
- Strong atomic SOC
- Free-electron like surface state
Paradigm Au(111)
Also W(110), Gd(0001),
Surface potential Additional SOC
Atomic potential Strong SOC
17Analytical calculation - model
- Hamiltonian
- Hamiltonian for an isotropic 2DEG
- Ansatz for the wave function
- Relation
- ? 2 wave functions, indexed by
SOC
Rashba terms
Pauli spinor
18Analytical calculation - dispersion
Dispersion without SOC
Inner ()
Dispersion with SOC
Outer (-)
splitting
SOC ? effective B-field in the electrons
restframe
Time-reversal symmetry
19Analytical calculation spin polarization
Time-reversal symmetry System remains nonmagnetic
- Spin polarization
-
- Complete (100)
- Within the surface plane
- Perpendicular to the wave vector
20Isotropic 2DEG versus Au(111)
2DEG isotropic parabolic complete in-plane
Au(111) threefold parabolic? complete? in-plane?
Symmetry Dispersion Spin polarization
Three-fold rotational symmetry
Value and sign of a, ß and ??
Probes
Theory Electronic-structure calculations Photoemis
sion calculations
Experiment Spin-resolved photoemission
(Osterwalder et al.) Dichroism (Carbone, Rossi et
al.)
21Au(111) - Dispersion
Experiment
Ab-initio theory
J. Osterwalder et al. (Zürich)
L
L
Momentum distribution at EF
Dispersion
Splitting
L
L
- Parabolic dispersion
- Circular momentum distribution
No significant signature of the threefold symmetry
22Au(111) Normal-emission spectra
Determination of free parameters (optical
potential) ? unique parameter set
Ab-initio theory
Experiment
J. Osterwalder et al.
Intensity
Spin polarization
Spin polarization due to SOC
(Tamura-Henk-Feder)
23Au(111) Off-normal-emission spectra
Linear dichroism in spin-integrated spectra
Ab-initio theory
Experiment
J. Osterwalder et al. (Zürich)
Dichroism due to surface symmetry
3.6º
Signature of the threefold symmetry
0º
-3.6º
24Au(111) - Choosing the right set-up
- Goal
- Determine the initial-state ESP from that of the
photoelectrons - Good set-ups
- Photoelectron spin polarization aligned with that
of the initial state - Set-up for linearly polarized light
- P-polarized light
- ESP normal to the scattering plane
- COmplete PHotoEmission Experiment
- Used in Zürich/PSI (Zürich set-up)
- Set-up for circularly polarized light
- Strong dichroism?
- Used in Trieste/ELETTRA (Trieste set-up)
due to SOC
25Au(111) Spin polarization
Zürich set-up
Binding energy 0.17 eV
Pz
Prad
Ptan
6
60
4
-60
Ab-initio theory
-4
-6
Threefold symmetry
Experiment
40
L
-40
26Au(111) Dichroism
Is there a magnetic or spin-related circular
dichroism?
Spin asymmetry or left-right asymmetry?
Trieste set-up
s
s-
Spectral density _at_ EF
Intensity _at_ EF
Wave vector
Wave vector
Left-right asymmetry in experiment, too?
27Au(111) Dichroism
Dichroism s - s-
K. Menon et al.
Experiment
Trieste set-up
Energy
- Left-right asymmetry
- No magnetic dichroism
- Circular dichroism (CDAD)
Wave vector
28Summary Spin-orbit coupling in Au(111)
- Electronic structure
- Parabolic dispersion, split into two bands
- Spin polarization
- Almost complete
- In-plane
- Normal to the wavevector
- No significant effects of the threefold
rotational symmetry - Photoemission
- Energy- and momentum distributions
- Good set-ups
- Strong reduction of the photoelectron spin
polarization - Dichroism
- Signature of the surface symmetry
29Spin-orbit coupling at Bi/Ag(111)
Surface alloy v3xv3R30-Bi/Ag(111)
Bi
Work in progress
Ag
Giant splitting
sp bands
Chr. Ast et al., cond-mat/0509509
30Spin-orbit coupling at Bi/Ag(111)
Experiment
Free-electron model
DFT calculations
1st band
2nd band
31Spin-orbit coupling at Bi/Ag(111)
2nd band
1st band
2nd band
32Summary Spin-orbit coupling in Bi/AgAu(111)
- Findings so far
- Giant spin splitting of the Bi sp states
- Agreement between experiment and ab initio
theory - Open questions
- Hybridization of the 1st and the 2nd band
- Effect of the threefold-rotational symmetry (Ag
sites surrounding Bi sites) - Degree and orientation of the spin polarization
33Summary and outlook
- Summary
- Spin-orbit coupling
- Effects of SOC on the electronic structure
- Ab-initio theory
- SOC at surfaces
- Rashba-Bychkov effect in 2DEGs
- Au(111)
- Bi/Ag(111)
- Work in progress
- Effect of electronic correlations Gd(0001)
- Effect of magnetization reversal at surfaces
Ni(111)
34Thanks
- MPI-MSP Halle
- Patrick Bruno, Arthur Ernst
- University Zürich
- Moritz Hoesch, Jürg Osterwalder
- Elettra/TASC, Trieste
- Carlo Carbone, Krishna Menon, Mattia Mulazzi,
Giorgio Rossi - EFL Lausanne
- Marco Grioni
- MPI-FKF Stuttgart
- Christian Ast, Klaus Kern