lecture notes introduction to strongly correlated electron ......iii. pressure effect on the ground...
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Lecture Notes
Introduction to Strongly Correlated Electron
Systems
Mohsen Abd-Elmeguid
II. Institute of Physics, University of Cologne, Germany
WS 2014/ 2015
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II. Classes of strongly correlated electron systems
(a) Transition metal compounds: 3d-electrons
- Hubbard model, Mott insulator, metal-insulator transition
- Spin, charge, and orbital degrees of freedom and ordering phenomena, selected materials
(b) Heavy fermion systems: 4f (5f) – electrons
- The Kondo effect, heavy fermion systems, non-Fermi liquid behavior,
- Quantum phase transitions, unconventional superconductivity, selected materials
(c) Nanoscale structures:
- Quantum confinement, unusual properties for potential applications
III. Pressure effect on the ground state properties: - Recent experimental results on heavy fermions and transition metal compounds
IV. Summary and open discussion
I. Introduction
Brief summary of electrons in solids, origin of strong electron correlations
Introduction to strongly correlated electron systems
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selected materials
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Layered structure quasi-2D system MO2-planes
Re: La3+, A: Sr2+, M: Cu,Ni,Mn,Co
Example: (Re,A)2MO4
Hole doping
-Quite large doping required to overcome charge/spin/orbital Long range order -Doped carriers can self assemble some examples!
Doped Mott insulators
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In the cuprates with large doping, charges are found to segregate in stripes running along the Cu–O bonds and are therefore called horizontal (or vertical) stripes. In the nickelates stripes are observed to run along the diagonals (diagonal stripes) as it is also reported for low-doped La2-xSrxCuO4
H. Ulbrich, M. Braden / Physica C 481 (2012) 31–45
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Getting control of the properties in TMO systems
correlation physics here has an energy scale of eV
but decision between metallic vs. insulator, FM vs. AFM is on much lower energy scale!
tiny perturbations of the system lead to a huge change of the properties
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Experimentally Driven 1986-1989; Theoretically Modeled 1989; IT Applications into 1990’s
First Commerical Hard-Disks with GMR Sensors (IBM) 1998
Giant Magnetoresistance (CMR)
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1988: … simultaneously, but independent
Albert Fert Peter Grünberg
Nobel Prize in Physics 2007
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The electrical resistance depends on
the relative magnetic alignment of the ferromagnetic layers
19% for trilayers @RT
80% for multilayers @ RT
Giant magnetoresistance (GMR)
Ferromagnet
Metal
Ferromagnet
Electrical
resistance: RP RAP
GMR RAP RP
RP
GMR is much larger than the anisotropic magnetoresistance (AMR)
only occurs for thin spacers with a thickness of a few nm
observed for many metallic spacer layers
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First observations of GMR
[1] G. Binasch, P. Grünberg et al., Phys. Rev B 39, 4828 (1989)
[2] M.N. Baibich, A. Fert et al., Phys. Rev. Lett. 61, 2472 (1988)
P. Grünberg, FZJ [1] A. Fert, Paris-Sud [2]
GMR
AMR
Both experiments employ antiferromagnetic interlayer coupling to
achieve the antiparallel alignment
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Anisotropic Magnetoresistance (AMR)
Origin: spin-orbit interaction -> coupling adds some orbital contribution
to the spin moment, gives rise to a dependence of the electron scattering
on the angle between the electron wave vector and the magnetization
direction
The largest AMR effect at room temperature is found for Ni1-xCox alloys with x
close to 0.2, for which %6~SRA
For permalloy Ni80Fe20 %4~SRA
Spontaneous resistivity anisotropy ratio generally defined as
Effect disappears above Tc
323||
||
SRA
SRA
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First observations of GMR
[1] G. Binasch, P. Grünberg et al., Phys. Rev B 39, 4828 (1989)
[2] M.N. Baibich, A. Fert et al., Phys. Rev. Lett. 61, 2472 (1988)
P. Grünberg, FZJ [1] A. Fert, Paris-Sud [2]
GMR
AMR
Both experiments employ antiferromagnetic interlayer coupling to
achieve the antiparallel alignment
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Clossal Magnetoresistance in doped TMO (CMR)
Example:
The Ca-doped series : La1-xCaxMnO3
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Doped manganites
O2-
Mn3+ A = La3+, Y3+…
B = Sr2+, Ca2+…
Perovskite structure
A1-x Bx MnO3
A = trivalent alkaline ion
B = divalent rare earth
Mn mixed valence :
Mn4+
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The Ca-doped series : La1-xCaxMnO3
LaMnO3 CaMnO3
Mn3+ Mn4+
Jahn-Teller active ion Non Jahn-Teller active
xCa
Regular
octahedron
Axially elongated
octahedron
• La3+ and Ca2+ are subsitutional
• La1-xCaxMnO3 solid solution can be obtained with 0 ≤ x ≤ 1 :
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La1-xCaxMnO3
xCa
T(K)
paramagnetic
insulating
350
300
250
200
150
100
50
00 0.2 0.4 0.6 0.8 1
LaMnO3 CaMnO3
Temperaturevs doping phase diagram
Doped manganites
have complex
phase diagram
FM = FerroMagnetic
AF = AntiFerromagnetic
CAF = Canted AF
FI = FM Insulator
CO = Charge Ordered
Maximum MR at x = 0.25
FM-MR
conductive
phase
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(
MW
· cm
)
M/Ms
T (K)
magneto-transport properties
Magnetic
transition (TC)
Metal-to-Insulator
transition (TMI)
Structural
transition (TS)
(TC ~ TMI ~ TS)
Local structure :
• Mn-O bond lengths
• Mn-O-Mn bond angles
ferromagnetic
conductive
reduced distortion
paramagnetic
insulating
enhanced distortion
TC ~ 260 K
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A.P. Ramirez, J. Phys.: Condens. Matter., 9 (1997) 8171
CMR (colossal magnetoresistance) La0.75Ca0.25MnO3
Tc
)(
)()0(
HR
HRHRR
Magnetoresistance is defined as the relative change of resistances at different magnetic fields
Tc
Ferromagnetic Metal
Paramagnetic Insulator
Conduction is by hopping of electrons between Mn3+ and Mn4+ sites, magnetic moments must be parallel ! ferromagnetic state is needed
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- reduced on-site Coulomb
interaction strength
- sensitive to lattice distortion,
magnetic order, etc.
- spin-orbit (SO) coupling much
stronger! (mainly 5d comounds)
Why interesting?
Examples!
correlated 4d and 5d transition metal oxides
4d and 5d orbitals are more extended than 3d’s
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3.2 Dzyaloshinskii-Moriya interaction
2D square lattice (Jeff =1/2 moments) with large JSE
similar to undoped high-TC cuperates
• Dzyaloshinskii-Moriya interaction: favors non-colinear spin arrangement
C. Cosio-Castaneda et al. J. Phys.: Condens. Matter 19 (2007)
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Ruddlesden-Popper (RP) series (Sr,Ca)n+1RunO3n+1
n=1,Sr2RuO4(SC),
Ca2RuO4(AF insulator);
n=2,Sr3Ru2O7,Ca3Ru2O7;
n=3,Sr4Ru3O10
Crystal structures for various n. T site
is Ru.
G. Cao et al. Matl. Sci. Eng. B 63,76 (1999)
Ruthenates
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Ru electronic configuration: [Kr]4d75s1
Rutherate (Ru4+)
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phase diagram of Ca2-xSrxRuO4
P: paramagnetic,
CAF: canted antiferromagnetic,
M: magnetic,
SC: superconducting,
-M: metallic phase,
–I : insulating phase.
S. Nakatsuji et al Phys. Rev. Lett. 84, 2666 (2000)
(I) (0≤x<0.2) AF insulating
ground state;
(II) (0.2≤x<0.5) Magnetic
metallic (M-M) region;
(III) (0.5≤x≤2) Paramagnetic
metal.
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Steffens et al. PRB 72,094104 (2005).
Detailed structural studies (Braden s Group)
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Continuous research activities in Cologne
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- reduced on-site Coulomb
interaction strength
-sensitive to lattice distortion,
magnetic order
- spin-orbit (SO) coupling much
stronger! (mainly 5d compounds)
Why interesting?
Example: SO-assisted Mott transition
correlated 4d and 5d transition metal oxides
in Sr2IrO4
4d and 5d orbitals are more extended than 3d’s
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spin-orbit coupling
• interaction of angular momentum around nucleus L and spin S
of electron:
total angular moment:
coupling strength:
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SO-coupling is a fast growing effect:
spin-orbit coupling
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extended 5d orbitals reduced Coulomb repulsion U (U~ W).
strength of SO coupling λ and U become comparable.
Systems with correlation + strong SO coupling
Hubbard model with strong SO coupling (mean-field):
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Spin-Orbit- assisted Mott insulators: SrIr2O4
Systems with correlation + strong SO coupling
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5d5 transition metal oxide
Perovskite
Rock salt Ir
O
?
magnetic frustration
along c-axis
B.J. Kim et al. Science 323 (2009)
Sr2IrO4
K2NiF4-structure
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• insulating behavior
Similar to Sr2
2+Rh4+O42-:
• 4d5 TMO with metallic ground state
expected behavior using LDA observed behavior
B.J. Kim et al. Science 323 (2009)
Sr2IrO4
insulating ground state metallic ground state
weak ferromagnetism
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Fig. 2 (Color online.) Temperature dependence of the magnetization M ( T ) measured under (a) 0.2 T and 1 T; (b) 0.001 T and 0.002 T. The inset of (a) shows <math altimg="si0001.gif" overflow="scroll"> <mi> χ</mi> <mo stretchy="false"> (</mo> <mi> T</mi> ...
Min Ge , Shun Tan , Yuanjie Huang , Lei Zhang , Wei Tong , Li Pi , Yuheng Zhang
Magnetism of insulator Sr2IrO4 with strong spin–orbit coupling
Journal of Magnetism and Magnetic Materials, Volume 345, 2013, 13 - 17
http://dx.doi.org/10.1016/j.jmmm.2013.05.022
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Orbital degeneracy and crystal field in Sr2IrO4:
octahedra stretched along z-axis
orbital degeneracy is lifted
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Orbital degeneracy and crystal field in Sr2IrO4
• assumption of a small CF: Hund´s rule: High spin, S=5/2
• electron configuration in Sr2IrO4:
large CF
Hund´s rule broken:
low spin state (S=1/2), eg orbitals empty
small:
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Leff=1:
1) angular part of wave function described by spherical harmonics , with :
all d-orbitls real for all individual d-orbitals:
orbital momentum is quenched
2) for degenerate orbitals, orbital momet is partially restored:
a. consider 1 electron in triply degenerate t2g orbitals:
degenerate t2g orbitals behave like effective p-orbitals with Leff=1
degenerate t2g orbitals behave like effective p-orbitals with Leff=1
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How strong spin-orbit coupling drives a Mott insulating state? see Board!
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The SO-assisted Mott state
• Leff=1 with S=1/2
Jeff =1/2 doublet and Jeff=3/2 quartet band
with energy difference
still metallic
B.J. Kim et al. PRL 101 (2008)
B.J. Kim et al. PRL 101 (2008) B.J. Kim et al. PRL 101 (2008)
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U
Leff =1 with S=1/2, Jeff =1/2 doublet and Jeff=3/2 quartet bands
By a strong Spin-Orbit coupling the t2g band splits into effective total angular momentum Jeff=1/2 doublet and Jeff=3/2 quartet bands. Splitting
The Jeff=1/2 spin-orbit states form a narrow band so that even small U opens a Mott gap, making it a Mott insulator.
The SO-assisted Mott state in Sr2IrO4
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narrow Jeff=1/2 band with Hubbard U Jeff=1/2 Mott ground state
Theory: LDA+SO+U insulating ground state
B. J. Kim, PRL 101, 076402 (2008)