AND WORKSHOP ON ELECTRONIC CRYSTALS ECRYS2011 ID: 796828
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Slide1
INTERNATIONAL RESEACH SCHOOL AND WORKSHOP ON ELECTRONIC CRYSTALS ECRYS2011 August 15 -27, 2011 Cargèse, France
Slide2Dirac electrons in solid Hidetoshi Fukuyama Tokyo Univ. of Science
Slide3AcknowledgementBiYuki Fuseya (Osaka Univ.)Masao Ogata (Tokyo Univ.)α-ET2I3Akito Kobayashi(Nagoya Univ.)Yoshikazu Suzumura (Nagoya Univ.)
Slide4Dirac electrons in solidscontents“elementary particles” in solids <= band structure , locally in k-spaceBand structure similar to Dirac electrons Examples: bismuth, graphite-graphene molecular solids αET2I3, FePn, Ca3PbO 4x4 (spin-orbit interaction), 2x2 (Weyl eq.)Particular features of Dirac electrons
small band gap
=> inter-band effects of magnetic field effects
Hall effect, magnetic susceptibility
Slide5Dirac equations for electrons in vacuumEquivalently,In special cases of m=0,
Weyl
equation for neutrino
4x4 matrix
2x2 matrix
Slide6“Elementary particles in solids”band structures, locally in k-spaceSi
InSb
electrons
holes
Semiconductors ,
Carrier doping
electron
doping ->n
type
hole
doping -> p
type
Dispersion relation
=>
effective masses and g-factors
“
elementary particles
”
Luttinger
-Kohn
representation (k
・
p approximation)
Slide7LK vs. Bloch representationBloch representation: energy eigen-states Ψnk(r)= eikrunk(r) : unk(r+a)=unk(r) Luttinger –Kohn representation [ Phys. Rev. 97, 869 (1955) ] Χnk(r)= eikru
nk0
(r)
k
0
= some special point of
interest
If
ε
n
(k) has
extremum
at k
0
Spin-orbit interaction
“k
・
p
method”
Hamiltonian is essentially a matrix
Slide8LK vs. Bloch * LK forms complete set and are related to Bloch by unitary transformation * k-dependences are completely different,* in Bloch, both eikr and unk(r) , the latter being very complicated, while in LK only in eikr as for free electrons.* just replace k=> k+eA/c in Hamiltonian matrix
once in the presence of magnetic field
Slide9Dirac types of energy dispersion(1)*Graphite [ P. R. Wallace (1947),J.W. McClure(1957)] semimetal(ne=nh≠0) *graphene: special case of graphite
(
n
e
=
n
h
=
0
)
Geim
H = v(
k
x
σ
x
+ kyσy ) Weyl eq. for neutrino
Isotropic velocity
McClure(1957)
Slide10Dirac types of energy dispersion(2)*Bi, Bi-Sb [M. H. Cohen and E. I. Blount (1960), P.A. Wolf(1964)]:semimetals strong spin-orbit interaction This term is negligible *α-ET2I3:
molecular solids
S. Katayama et al.[2006]
A. Kobayashi et al.(2006)
H = k
・
V
ρ
σ
ρ
σ
0
= 1,
σα α= x,y,z Tilted Weyl eq.
Tilted Dirac eq.
Anisotropic velocity
Anisotropic masses and g-factors
Slide11*FePnHosono(2008)Ishibashi-Terakura(2008) DFT in AF states
HF : JPSJ
Online
—News and Comments [May 12, 2008
]
* Ca
3
PbO :
Kariyado
-Ogata(2011)JPSJ
Dirac types of energy
dispersion(3)
Slide12Dirac electrons in solidsBulk*Bi*graphite-graphene*ET2I3*FePn*Ca3PbO cf. topological insulators at surfacesEffective Hamiltonian
Slide13Characteristics of energy bands of Dirac electrons*narrow band gap, if any*linear dependence on k (except very near k0) Gapless (Weyl 2x2) negligible s-o => effects of spins additive
Finite gap(mass)(4x4)
s-o => spin effects are essential
Slide14Essence of Luttinger-Kohn representationHamiltonian is a matrix H nn’ = [εn(k0)+ k2/2m] δ n,n’ + kαpαnn’ /me.g. 2x2 Eg/2 + k2/2m kp
/m
H=
kp
/m -
Eg
/2
+
k
2
/2m
E= k
2
/2m
(Eg/2 )2 +(kp)2
if (Eg/2 )
2
>> (
kp
)
2
, E
=
Eg
/2 + k
2
/2 m*
=1/2m
Effective mass approximation Effective g-factors as well
precise determination of parameters to describe
electronic state
=> foundations of present semiconductor technology
Luttinger-Kohn representationE= k2/2m (Eg/2 )2 +(kp)2 On the other hand, if (Eg/2 )2 << (kp)2 E ~ |kp| k-linear
Particular features of Dirac electronsNarrow band gaps =>Inter-band coupling “ Inter-band effects”Different features form effective mass approximation in transport and thermodynamic properties. Especially , in magnetic field Hall effects, orbital magnetic susceptibility
Slide1710th ICPS (1970)- corresponds to the Peierls phase in the tight-binding approx.
ε
n
(k) => ε
n
(k+eA/c)
Landau-Peierls Formula
χ
LP
= 0 if DOS at Fermi energy =0
p
・
A :
p
has matrix elements between Bloch bands
Slide19Orbital Magnetism in Bi
Landau-Peierls formula (in textbooks) is totally invalid !!
Expt. Indicate
importance of
inter-band
effects of magnetic field.
Landau-
Peierls
Formula
χ
LP
= 0 if DOS at Fermi energy =0
Slide20HF-Kubo: JPSJ 28 (1970) 570
Diamagetism of Bi
P.A. Wolff
J. Phys. Chem. Solids (1964)
Dirac electrons in solids!
Strong spin-orbit interaction
Slide21Exact
Formula of Orbital
Susceptibility in General Cases
In Bloch representation
Slide22With Gregory Wannier @Eugene, Oregon (1973)
Slide23Weak field Hall conductivity, σxyOne-band approximation based on Boltzmann transport equation,General formula based on Kubo formula: HF-Ebisawa-Wada PTP 42 (1969) 494.
Inter-band effects
have been taken into account
=> Existence of contributions with not only f’(ε) but also f(ε)
HF for
graphene
(2007)
Weyl
eq
.
A. Kobayashi et al., for α-ET
2
I
3
(2008)
Tilted
Weyl
eq.
Y.
Fuseya
et al., for Bi (2009)
Tilted Dirac eq.
Slide24Slide25BiWolf(1964)Assumption = isotropy of velocity“Isotropic Wolf”
Δ=E
G
/2
= original Dirac
Slide26In weak magnetic fieldR=0 , but not 1/R=0
Fuseya
-Ogata-HF, PRL102,066601(2009)
Slide27Isotropic Wolf model (original Dirac)
Under magnetic field, k=> π=
k+eA
/c
* Reduction of cyclotron mass = enhancement of g-factor
=> Landau splitting = Zeeman splitting both can be 100 times those of free electrons
* Energy levels are characterized by j=n+1/2 +σ/2
orbital and spin angular momenta contribute equally to magnetization
* Spin currents can be generated by light absorption
Fuseya
–Ogata-HF, JPSJ
Under strong magnetic field
Slide28Molecular Solids ET2Xlayered structureET layers Anions layers
S
S
S
S
S
S
S
S
ET
molecule
(ET=BEDTTTF)
ET
2
X
-
=> ET
+1/2
ET layers conducting
X- closed shell
Slide29Degree of dimerization
(effectively ¼-filled for weak, ½ for strong)
and
degree of anisotropy of triangular lattice, t’/t
Hotta,JPSJ
(2003),
Seo,Hotta,HF:Chemical
Review 104 (2004) 5005.
ET
2
X Systems
ET=BEDT-TTF
S
S
S
S
S
S
S
S
α
Spin Liquid
Dirac cones
Slide30α-ET2I3
JPSJ 69(2000)Tajima-Kajita
T-indep. R under high pressure
Kajita (1991,1993)
p =19Kbar
μ
eff
deduced by
weak field Hall coefficient
has
very strong T-dep.
n
eff
is also
, since
σ=
neμ
μ
eff
α-ET
2
I
3
b
y charge order
Slide31Hall coefficient in weak magnetic field depends on
samples,
some
change signs
at low
temperature.
Slide32Tight-binding approximation
Slide33fastest
slowest
エネルギー
(eV)
Energy dispersion
Massless Dirac fermion in α-(BEDT-TTF)
2
I
3
Katayama et al. (2006)
Tilted Dirac cone
Confirmed by DFT
: Kino et al. (2006)
Ishibashi
(2006)
NMR
:
Takahashi et al. (2006)
Kanoda
et al.
(
2007
)
Shimizu et al.(2008)
Interlayer
Magnetoresistance
Osada
et al.(2008)
Tajima et al.(2008)
Morinari
et al. (2008)
Tilted
Weyl
Hamiltonian
Kobayashi et at. (2007)
Hall effect
:
Tajima et al. (2008)
Kobayashi et al. (2008)
Slide34The conventional relation RH∝1/n is invalid. ------ typically, RH=0 at μ=0 (
n
eff
=0 for
semicoductors
)
sharp μ-dependence in narrow enegy range of the order of Γ.
1/
Γ
: elastic scattering time
extremely sensitive probe!
Orbital
susceptibility
conductivity
Hall conductivity
X=μ/Γ
Transport properties:
Hall effect
Kobayashi et al., JPSJ 77(08)064718
σ
μν
=σ
0
K
μν
μ:chemical potential
2d model Without tilting=
graphene
Slide35Effect
of Tilting
Kobayashi-
Suzumura
-HF,JPSJ 77, 064718(2008)
Based on exact gauge-invariant formula
X=ε/Γ
Slide36speculations on T-dep. with μ=0 for T/Γ>1σxx= Kxx
σ
xx
(T)
=-
∫
dεf
’(ε
)
σ(ε
)~
Γ/T
weak T dep. of σ => Γ ~ T,
Then σxy=
~ 1/T
2
R ~
1/T
2
K
xy
σ=
neμ
n~ T
2
μ
~1/T
2
α= 0
Stronger T-
dep
In
expts
?
Slide37Possible sign change of Hall coefficient;
A. Kobayashi et al., JPSJ 77(2008) 064718.
Asymmetry of DOS
relative to the crossing energy, ε
0.
Chemical potential crosses ε
0
as T->0
if I
3
- ions are deficient of the order of 10
-6
(hole-doped)
Hall coefficient can
change sign,
in accordance with expt.
by Tajima et al. as below.
Prediction,
diamagnetism will be maximum,
when Hall coefficient
changes
sign
.
Bulk 3d effects
Cf. specific heat
Slide38Under strong perpendicular magnetic field
p=18kbar
α-(BEDT-TTF)
2
I
3
N. Tajima et al. (2006)
T
0
T
1
*For
tilted-cones,
inter-valley scattering
plays important roles.
*Mean-filed phase transition(T
0
) to pseudo-spin
XY ferromagnetic state.
*Possible
BKT
transition
at lower temperature.
A.Kobayashi
et al,
JPSJ78(2009)114711
T
0
T
1
Slide39Landau quantizationMassless Dirac fermions under magnetic field
At H=10T
T
0
With
tilting
M. O.
Goerbig
et al. (2008)
T.
Morinari
et al. (2008
)
Electron correlation can play important roles!
Effective Coulomb interaction
Zeeman energy
Slide40Kosterlitz-Thouless Transition in Strong Magnetic Field
Long-range Coulomb interaction
:spin
↑、↓
:
pseudo-spin
(
valley)
R,L
Tilted Weyl Hamiltonian
v:
cone velocity
pseudo-spin
(
valley)
Katayama et al.
(2006)
Zeeman term
w: tilting velocity
Kobayashi et at. (2007)
Slide41Wave function of N=0 states (Landau gauge)
Å
X-direction: localized
Y-direction: plane wave
Magetic length
magnetic unit cell :
a flux quantum
Φ
0
|Φ|
2
Wannier functions (ortho-normal) can be defined
on magnetic lattice
Fukuyama (1977, in Japanese)
To treat interaction effects,
“
Wannier
function” for N=0 states
Slide42Effective Hamiltonian on the magnetic latticeLandau quantization (N=0)+Zeeman energy+long-range Coulomb interaction
Effective Hamiltonian
SU(4)
symmetric
independent of tilting
Breaking SU(4) symmetry
Induced by Tilting!
V
term
:
intra-valley scattering
W
term
:
inter-valley scattering
for α-(BEDT-TTF)
2
I
3
H=10T
:tilting parameter
Slide43Ground state of the effective Hamiltonian
In the absence of tilting
Spin-polarized state
the phase transition can occur at finite T
in the mean-field approximation.
W-term :
Pseudo-spins are bound to XY-plane.
V-term
:
symmetric
in the spin and pseudo-spin space
In the presence of tilting
Pseudo-spin ferromagnetic state
Only E
z
-term
breaks the symmetry
If the interaction is larger than E
z
,
Slide44Mean field theory (finite T)
:Pseudo-spin operator
:
interactions between pseudo-spins
Taking fluctuations of pseudo-spins in XY-plane,
Spin-polarized state
Pseudo-spin XY ferro
Effective “spin model” on the magnetic lattice
Tc ~ 0.5 I
Slide45Kosterlitz-Thouless transitionExpanding the free energy from long-wavelength limit,
The fluctuations are described by the XY model
Berenzinskii-Kosterlitz-Thouless
transition
(J. M.
Kosterlitz
, J. Phys. C7 (1974) 1046. )
(in the present case)
vortex and anti-vortex excitations
Tc~ 0.5
I
n
earest-neighbor
interaction
nearly
isotropic
if
I
00
=I
Slide46Under strong perpendicular magnetic field
p=18kbar
α-(BEDT-TTF)
2
I
3
N. Tajima et al. (2006)
T
0
T
1
*For
tilted-cones,
inter-valley scattering
plays important roles.
*Mean-filed phase transition(T
0
) to pseudo-spin
XY ferromagnetic state.
*Possible
BKT
transition
at lower temperature.
A.Kobayashi
et al,
JPSJ78(2009)114711
T
0
T
1
Slide47GraphenesCheckelsky-Ong,PRB 79(2009)115434
BKT
transition T=0.3K at 30T
K. Nomura, S. Ryu, and D-H Lee, cond-mat/0906.0159
Without tilting (W=0) : electron-lattice coupling
Slide48Massless Dirac electrons in α-ET2X*Described by Tilted Weyl equation*Unusual responses to weak magnetic field Hall coefficient Inter-band effects of magnetic field (vector potential, A) are crucial.*Under strong magnetic field possible Berezinskii-Kosterlitz-Thouless transition* Further many-body effects ?
Slide49Massless Dirac electrons in α-ET2X*Described by Tilted Weyl equation*Unusual responses to weak magnetic field Hall coefficient Inter-band effects of magnetic field (vector potential, A) are crucial.*Under strong magnetic field possible Berezinskii-Kosterlitz-Thouless transition* Further many-body effects ?
Slide50Ca3PbO
Synthesis not yet.
Similarity to and differences from Bi
Kariyado
-Ogata to appear in JPSJ
Dirac electrons in solidsSummary* Examples: bismuth, graphite-graphene molecular solids αET2I3, FePn, Ca3PbO 4x4 (spin-orbit interaction), 2x2 (Weyl eq.)* Particular features are “small band gap” => inter-band effects of magnetic field effects
Hall effect, magnetic susceptibility
~~
Targets
Effects of boundary( surfaces, interfaces)
Slide52SupplementFePn Superconductivity
Slide53Year 2008: New High-Tc “Fever” derived from Hosono’s DiscoveryPbNb
NbC
NbN
Nb
3
Ge
MgB
2
Hg
Year
T
c
(K)
Onnes
1913
Physics
1911
LaBaCuO
LaSrCuO
YBaCuO
BiCaSrCuO
HgCaBaCuO
HgCaBaCuO
(High-Pressure)
1986
Bednorz
Muller
1987
Physics
2001
Akimitsu
LaFePO
LaFeAsO
LaFeAsO
(High-Pressure)
SmFeAsO
Hosono
1
st
International Symposium
June 27-28, Tokyo
1
st
Proceedings
Vol. 77 (2008) Supplement C
November 28
1
st
Focused Funding Program
T
ransformative
R
esearch-Project
on
I
ron
P
nictides
Call for proposal: July-August
Start: October (till March 2012)
TlCaBaCuO
2008
Prepared by JST
Slide54World-wide Competition and Collaboration triggered by TRIP
Oct 2008 – Mar 2012
Leader:
Hide Fukuyama
24 Research Subjects
0.3-0.8 M$/ 3.5
Yrs
Collaboration
Leader:
Hideo Hosono
Mar 2010 – Mar 2013
Outcome
New priority program
‘
High-temp
. superconductivity
in iron pnictides’
(SPP 1458)
From 2010; 6
Yrs
(3Yrs + 3Yrs)
Collaboration
Collaboration
JST-EU Strategic Int. Cooperative
Program
on
‘Superconductivity’
(3-Yrs period)
Under
ex ante
evaluation
International Workshop on the Search for New SCs
Co-sponsored by
JST-DOE-NSF-AFOSR
May 12-16, 2009, Shonan
Collaboration
Frontiers in
Crystalline
Matter
Reported by
National
Academy of
Sciences
Oct 2009
P108-109 Box 3.1
Iron-Based Pnictide Materials: Important New Class of Materials Discovered Outside the United States
Prepared by JST
Slide55A15-MgB2-Cuprates-FePn*A15 : BCS, structural change*MgB2 : BCS, strong ele-phonon, 2bands*Cuprates: strong correlation in a single band, Doped Mott, t-J model*FePn: strong correlation in multi bands structural change
Slide56Journal of the Physical Society of JapanVol. 77 (2008) Supplement CProceedings of the International Symposium on Fe-Pnictide Superconductors Published in JPSJ online November 27, 2008 PrefaceOutline*Layered Iron Pnictide Superconductors: Discovery and Current Status Hideo Hosono *A New Road to Higher Temperature Superconductivity S. Uchida *Doping Dependence of Superconductivity and Lattice Constants in Hole Doped La1-xSrxFeAsO Gang Mu, Lei Fang, Huan Yang, Xiyu Zhu, Peng Cheng, and Hai-Hu Wen *Se and Te Doping Study of the FeSe
Superconductors
K. W.
Yeh
, H. C. Hsu, T. W. Huang, P. M. Wu, Y. L. Huang, T. K. Chen, J. Y.
Luo
, and M. K. Wu
Total ~50 papers
Slide57In 2011,Special Issue : Solid State Communications, to appear.
Slide58S. Nandi et al.: Phys. Rev. Lett. 104 (2010) 0570061111R. Parker et al.: Phys. Rev. Lett. 104 (2010) 057007111
FePn
Phase diagram
Tet
Ort
T
S
>
T
N
for
x
>0
T-W Huang
et al
.: Phys. Rev. B82 (2010) 104502
Tet
Ort
J. Zhao
et al
.: Nature Mater. 7 (2008) 953
122
No
T
N
11
Courtesy: Ono
Slide591111Tet
Ort
J. Zhao
et al
.: Nature Mater. 7 (2008) 953
Courtesy: Ono
Basic difference from
cuprates
Parent compound
Cuprates
: Mott insulator (odd) 1 band
FePn
: semimetal (even)
multi-band
Importance of magnetism : spin-fluctuations
Roles of many bands
:
Mazin
, Kuroki
Effects of crystal structure: Lee plot (
Pn
height-Kuroki)
film
MKWu
Electronic inhomogeneity
Phase separation
Slide60MinimumCourtesy: Yoshizawa
Ba122Co
Slide61Analysis for softening in C66 of Ba(Fe1-xCox)2As2
Co ( % )
Θ
(
K )
Δ
( K )
3.7
%
75.5
5.4
6 %
17.2
8.3
10 %
- 30
15.6
M.Yoshizawa
et al
., arXiv:
1008
.
1479v3
(Aug 2010)
Increasing of Co doping in
Ba(Fe
1-x
Co
x
)
2
As
2
reduces
Θ
and enhances
Δ
.
C
66
of
Ba
(
Fe
1-x
Co
x
)
2
As
2
Constant
Θ
changes its
sigh
from + to – over
q
uantum critical point.
Slide62Temperature dependence in elastic constants of Ba(Fe0.9Co0.1)2As2C66 reveals huge softening of 28% from room temperature down to Tsc=23K.No sigh of softening in (C
11
–
C
12
)
/ 2
and
C
44
.
Electric
quadrupole
of
O
u
is relevant
Courtesy:
Goto
little change by H
Slide631d bands Labbe-Friedel:band Jahn Teller Gorkov:dimerization along chains3d bands <= band calc. by Mattheiss Bhatt-McMillan, Bhatt: 2 close-lying saddle points based on dx2-y2 band Matheiss dz2Tc Klein ele-phonon A15
Slide64FePn: Coulomb interaction +el-ph interaction due to multi-orbit(multi-band)
Slide65END