description of galvanomagnetic transport using kubo's ......electric field fictitious field ......
TRANSCRIPT
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Description of galvanomagnetic transport using Kubo's linear response formalism
S. Wimmer, D. Ködderitzsch and H. Ebert(J. Minar)
M
E
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SFB 689
SPP 1538
LMU – AKHE
Hubert Ebert
Kristina ChadovaStephan LowitzerSebastian Wimmer
Financial support
Acknowledgments
Spinphänomene in reduzierten Dimensionen
Spin Caloric Transport
University of Warwick
Julie StauntionPaul Tulip
Martin-Luther-UniHalle-Wittenberg
Martin GradhandIngrid Mertig
Uni Regensburg
Christian BackGeorg Woltersdorf
WMI Garching
Sebastian Gönnenwein
Sven BornemannJürgen BraunGerhard KuhnJán MinárSergei MankowskyMartin OffenbergerSvitlana PolesyaMarius Schulte
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Outline
● A zoo of transport phenomena
● Transport formalism from first principles – Boltzmann
● Transport formalism from first principles – Kubo
● longitudinal● transverse● thermogalvanic
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Electronic transport – Ohm's law (linear resp.)
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Introduction
Transport phenomena in linear response regime
● electrical
● spin
● heat
● Electric field
● Fictitious field coupling to spin
● Temperature gradient
current density
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Introduction
Anomalous Hall e ect (AHE)ffAnisotropic Magneto-Resistance (AMR)
Anisotropy of Seebeck e ect (ASE)ffAnomalous Nernst e ect (ANE)ff
Spin Seebeck e ect (SSE)ffSpin Nernst e ect (SNE)ff
Spin Hall e ect (SHE)ff
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Semi-classical approach – Boltzmann transport theory –
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Electronic structure of solids
Schrödinger equation within local (spin) density theory (LSDA)
Periodic potential
Dispersion relation
Bloch theorem
Density of states Fermi surface
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Boltzmann transport equation I
total rate in change for distribution function
external term due to the electric field
group velocity
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Boltzmann transport equation II
scattering term
Transition propability
andwith
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Boltzmann transport equation III
linear ansatz
vector mean free path
relaxation time
conductivity tensor element
Mertig et al., Teubner (1987)
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Ni with 3-d Transition Metal impurities (1%)
Spin projected residual resistivity based on:
Experiment: A. Fert et al., PRL 21, 1190 (1968)Theory: I. Mertig et al., PRB 47, 16178 (1993)
● Two-current model of Mott
● Boltzmann transport formalism
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Full quantum mechanical approach– Kubo formalism –
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Kubo's formalism
Expectation value of operator
with density matrix
To first order w.r.t. the perturbation one has
To get the response to a time-dependent perturbationsolve equation of motion for
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Kubo formalism applied to electric transport
perturbation
electric dipole moment
Kubo's identity
to electric field
induced electric current density
leads for the conductivity tensor to:
represents coupling of
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Hierarchy of transport equations
Kubo
Bastin
Kubo-Středa
Kubo-Greenwood
Independent electron approximation, ω = 0
T = 0K
Retaining symmetric part only
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Transport from first-principles – various ingredients –
(a little detour)
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Multiple scattering representation of G in KKR
scattering path operator
numerical,relativistic
radial solutions&
rel. spin-angular-functions
Muffin-Tin-Potential
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Dyson–Equation
Reference system
Stepanyuk et.al, PRB 68,205410 (2003)
● intuitive, physically transparent
● construction: Hierarchy of Dyson-Equations
● Korringa-Kohn-Rostoker (KKR)-GF method
● spherical waves
● accurate minimal basis set method
● efficient treatment of
● impurities
● surfaces and interfaces
● disorder (CPA, NL-CPA)
Review: Ebert, Ködderitzsch, Minár, Rep. Prog. Phys. 74, 096501 (2011)
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Theory of effective media – CPA
Best single-site theory:
Coherent potential approximation (CPA)
self-consistent construction of the medium:
embedding of A- or B-atoms in effectiv mediumdoes not cause – on average – scattering
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Theory of relativity and quantum mechanics
Westminster Abbey
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Longitudinal charge transport
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Band structure of disordered alloys
Fermi surfacein Γ-X-W-plane
along Γ-Xalong Γ-X
Dispersion relationof pure Cu
Bloch spectral function of Cu0.80Pd0.20
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Band structure of disordered alloys
Fermi surfacein Γ-X-W-plane
along Γ-Xalong Γ-X
Dispersion relationof pure Cu
Bloch spectral function of Cu0.80Pd0.20
group velocity life time
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Boltzmann-formalism applied to AgxPd1-x
Fermi surface of AgxPd
1-xResidual resistivity (T=0K)
(110)-plane (001)-plane
Ag0.2Pd0.8
Ag0.5Pd0.5
Ag0.8Pd0.2
W. H. Butler et al., PRB 29, 4217 (1984)
Neglecting scattering-in term
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Kubo-Greenwood (KG) Equation Part I
conductivity tensor within linear response (Kubo) formalism given ascurrent density–current density correlation function
= average over alloy configurations
current density operator
with:
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Kubo-Greenwood Equation Part II
with and the quantum numbers
Implementation within KKR-CPA
Butler, PRB 31, 3260 (1985) (non-relativistic)Banhart et al., SSC 77, 107 (1991) (fully-relativistic)Turek et al., PRB 65, 125101 (2002) (LMTO-CPA)
Vertex corrections (VC)
account for scattering-in processes
vertex correction
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Application to non-magnetic alloys
small large
Expt: Guénault, Phil. Mag. 30, 641, (1974)Theo: Tulip et al., PRB 77, 165116 (2008)
Residual resistivity (T=0K)
impact of vertex corrections (VC)
depending on alloy system and character of wave functions at Fermi level
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Symmetry breaking due to magnetism
G = m3m G = 4/mm'm'
Point group for bcc-structure
1': time reversal
paramagnetic ferromagnetic
reduced symmetry due to magnetism AND spin-orbit coupling
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Structure of the conductivity tensor σ
Von Neumann's Principle
paramagnetic ferromagnetic
Isotropic conductivityor resistivity
Galvano-magnetic effectsAnomalous Hall effect
Anisotropic magnetoresistance AMR
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The Dirac Equation for magnetic solids
effective magnetic field
is determined by the spin magnetisation within spin density functional theory (SDFT)
Within an atomic cell one can choose to have:
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Bloch spectral function of Fe0.2Ni0.8
minority spin majority spin
along Γ-X
Fermi surfacein Γ-X-W-plane
Ebert et al., SSC 104, 243 (1997)
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Residual resistivity of ferro-magnetic alloys
see also :Banhart et al., PRB 56, 10165 (1997)Khmelevskyi et al., PRB 68, 012402 (2003)Turek et al., JPCS 200, 052029 (2010)
Isotropic residual resistivity Anisotropic magnetoresistance AMR
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Ni with 3d Transition Metal impurities (1%)
Spin projected longitudinal residual resistivity
● Boltzmann transport formalism
● Two-current model of Mott
● Kubo-Středa formalism
● Spin current operatorversus
● I Mertig et al., PRB 47, 16178 (1993) non-relativistic two current model● S Lowitzer, DK, H Ebert, PRB 82, 140402(R) (2010), relativistic spin current op.
Theory:
Exp. : A Fert et al., PRL 21, 1190 (1968)
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Transverse currents
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Transverse charge and spin currents
Anomalous Hall Effect (AHE)
Source relativistic spin-orbit interaction
Separating charge (+ spin)
FM
M
E
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Transverse charge and spin currents
Anomalous Hall Effect (AHE)Spin Hall Effect (SHE)
Source relativistic spin-orbit interaction
Separating charge (+ spin)
PM
“Spintronics without magnetism”
M
E
spin
in both cases
FM
E
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Anomalous Hall effect (AHE)
electrical conductivity tensor for a ferromagnetic cubic system with magnetization direction along the z-axis
M
E
● Spin-orbit coupling as defining component
● Intrinsic component – interpreted in terms of Berry phase
● Extrinsic components – e.g.
● Side-jump
● Skew scattering
● Spin-orbit coupling as defining component
● Intrinsic component – interpreted in terms of Berry phase
● Extrinsic components – e.g.
● Side-jump
● Skew scattering
Mechanisms
skew (Mott-) scattering
side-jump scattering
spin dependent impurity scattering
● Relativistics, i.e. Spin-orbit coupling as defining component
● Intrinsic component – interpreted in terms of Berry phase
● Extrinsic components – e.g.
● Side-jump
● Skew scattering
● Relativistics, i.e. Spin-orbit coupling as defining component
● Intrinsic component – interpreted in terms of Berry phase
● Extrinsic components – e.g.
● Side-jump
● Skew scattering
Yao et al., PRL 92, 037204 (2004)Sinitsyn, JPhys. Cond. Matter, 20,023201 (2008)Nagaosa et al., Rev. Mod. Phys, 82, 1539 (2010)
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Kubo-Středa (KS) Equation (T = 0K)
electronic
spin
with the current density operators
Spinprojektionsop. [1,2,3]
[1] Bargmann & Wigner, Proc. Natl. Acad. Sci. 34, 211 (1948)
[3] Lowitzer, Ködderitzsch, Ebert, PRB 82, 140402(R) (2010)
[2] Vernes, Györffy, Weinberger, PRB 76, 12408 (2007)
Dirac matrix
Advanced / retarded relativistic Green function
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Intrinsic AHE of 3d metals
Berry curvatureYao et al., PRL 92, 037204 (2004)
Fe
SPR-KKR 727 -2115 343481 Berry curvature
753 -2073 492751 -2203
1032 Experiment-646
480
σxy (Ωcm)-1 bcc Fe fcc Ni hcp Co
Kubo-StředaRoman et al. (2009)Yao et al. (2004)Wang et al. (2007)Dheer (1967)Lavine (1961)Miyasato et al. (2007)
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AHE and SHE in alloys
Lowitzer, Ködderitzsch, Ebert,Phys. Rev Lett. 105, 266604 (2010)
Exp.: Matveev et al., Fiz. Met. Metalloved 53, 34 (1982)
FexPd
1-x AuxPt
1-x
Anomalous Hall-Effect Spin-Hall-Effect
Lowitzer, Gradhand, Ködderitzsch, et al. Phys. Rev. Lett. 106, 056601 (2011)
Review: Ködderitzsch, Lowitzer, Staunton, Ebertphys. stat. sol. (b) 248, 2248 (2011) .
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Classification of contributions
Vertex-diagrams
Crepieux, Bruno, PRB 64, 014416 (2001)
side-jump
skew
extrinsic
intrinsic
● intrinsic
● calculation without vertex corrections
● extrinsic
● with vertex corrections
● assume scaling
● extract values
First-principles calculation: KKR-GF-Kubo-Středa
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SHE: Kubo-Středa vs. Boltzmann-Formalism
Comparison of results for
Boltzmann-based calculations: Collaboration with Gradhand, Fedorov, Mertig Uni Halle-Wittenberg
longitudinal conductivity skew scattering
(impurity concentration 1%)
Lowitzer, Gradhand, Ködderitzsch, et al. Phys. Rev. Lett. 106, 056601 (2011)
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Summary
First-principles, parameter-free,material specific electronic structure determination
● Spin-density-functional theory
● KKR-Green function method
● Disorder (CPA)
● relativistic effects
Transport formalisms
● Boltzmann
● semi-classical
● dilute alloys
● Kubo(-Středa)
● full quantum mechanical
Transport phenomena
● Longitudinal
● conductivity● spin-decomposition● AMR● Seebeck
● Transverse
● Spin-Hall● Anomalous Hall● Spin-Nernst● Anomalous Nernst
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Thermogalvanic transport
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Thermogalvanic coefficients
Jonson & Mahan, PRB 21, 4223 (1980); Kontani, PRB 67, 014408 (2003)
Response functions by Kubo formulas in Matsubara notation
Electrical and thermal current in linear response theory
Thomas J. Seebeck(1770-1831)
Seebeck effectFlashback: talk by Ch. Heiliger (yesterday)
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Thermogalvanic coefficients via Mott's rule
● for constant : ,
● S from integral (T-dependence via Fermi distr.)
Mott's formula for the thermoelectric powerwith conductivity calculated via Kubo-Středa
● Seebeck (diagonal)
● Anomalous Nernst conductivity (off-diagonal)
Sommerfeld
(low T)
Variation of
at Fermi energy
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Thermogalvanic coefficients – nomenclature
Anomalous Hall Effect (AHE)Spin Hall Effect (SHE)
PM
M
E FME
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Thermogalvanic coefficients – nomenclature
Anomalous Hall Effect (AHE)Spin Hall Effect (SHE)
PM
M
E FME
Nernst Nernst
T T
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Spin-Hall Effect for Cu-Ir and Cu-Bi
Cu-Bi Cu-Ir
Spin-Hall resistivity versus longitudinal resistivity
Niimi et al., PRL, accepted (2012)
Gigantic SHE Spin Hall angle
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Spin-Hall Effect for Cu-Ir and Cu-Bi
Cu-Bi Cu-Ir
Spin-Hall resistivity versus longitudinal resistivity
Niimi et al., PRL, accepted (2012)
Gigantic SHE
SpinNernst?
Spin Hall angle
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Spin dependent thermogalvanic coefficients
● Linear transport coefficients: ,
● Spin-dependent thermopowers
● Charge Seebeck coefficient
● Spin-polarised Seebeck coefficient:
off-diagonal component:
describes the spin accumulation transverse to a temperature gradient
● Spin Nernst conductivity
Tauber et al., PRL 109, 026601 (2012).
See talk Sebastian Wimmer
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Vielfachstreutheorie
● Traditionelle Lösung
● Schrödingergleichung in I,II,III
● Wellenfunktion anpassen
● Gleichungssystem lösen
Doppel-Delta-Barriere
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Vielfachstreutheorie
Reflexion Transmission
● Traditionelle Lösung
● Schrödingergleichung: I,II,III
● Wellenfunktion anpassen
● Gleichungssystem lösen
Alternative: Vielfachstreuung und Greensche Funktion
Ist es möglich, aus den Eigenschaften der Einzelbarrieren die Lösung zu bestimmen ?
Ja!
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Vielfachstreutheorie und Greensche Funktion G
t – Matrix Operator
Greensche Funktion ohne Barriere (Potential)
(*)
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Vielfachstreutheorie und Greensche Funktion G
t – Matrix Operator
Greensche Funktion ohne Barriere (Potential)
Iteriere (*)
(*)
Reflexion RTransmission T
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Vielfachstreutheorie und Greensche Funktion G
t – Matrix Operator
Greensche Funktion ohne Barriere (Potential)
Iteriere (*)
(*)
Reflexion RTransmission T
Äquivalent: Konstruktion der Greenschen Funktion des Systems mit Barriere
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Vielfachstreutheorie und Greensche Funktion G
Äquivalent: Konstruktion der Greenschen Funktion des Gesamtsystems
Erwartungswert einer Einteilchenobservable (Operator )
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Dyson–Gleichung
Greensche Funktion des Gesamtsystems
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Vielfachstreutheorie und Greensche Funktion
Streupfadoperator
:
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Dyson–Gleichung
Referenzsystem
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Vielfachstreudarstellung von G in der KKR
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Vielfachstreudarstellung von G in der KKR
Muffin-Tin-Potenzial
numerische,relativistischeRadialwellen
&rel. Spin-Winkel-Funktionen
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Vielfachstreudarstellung von G in der KKR
Streupfadoperator
numerische,relativistischeRadialwellen
&rel. Spin-Winkel-Funktionen
Muffin-Tin-Potenzial
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Vielfachstreudarstellung