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トポロジカル絶縁体・超伝導体
古崎
昭
(理化学研究所)
topological insulators (3d and 2d)July 9, 2009
Outline• イントロダクション
バンド絶縁体, トポロジカル絶縁体・超伝導体
• トポロジカル絶縁体・超伝導体の例:
整数量子ホール系
p+ip 超伝導体
Z2
トポロジカル絶縁体: 2d & 3d
• トポロジカル絶縁体・超伝導体の分類
絶縁体 Insulator
• 電気を流さない物質
絶縁体
Band theory of electrons in solids
• Schroedinger equation
ion (+ charge)
electron Electrons moving in the lattice of ions
( ) ( ) ( )rErrVm
ψψ =⎥⎦
⎤⎢⎣
⎡+∇− 2
2
2h
( ) ( )rVarV =+
Periodic electrostatic potential from ions and other electrons (mean‐field)
Bloch’s theorem:( ) ( ) ( ) ( )ruaru
ak
aruer knknkn
ikr,,, , , =+<<−=
ππψ
( )kEn Energy band dispersion :n band index
例:一次元格子模型
ε2A A A A AB B B B B
t−
n 1+n1−n
( ) ⎟⎟⎠
⎞⎜⎜⎝
⎛=
B
Aikn
uu
enψ ⎟⎟⎠
⎞⎜⎜⎝
⎛=⎟⎟
⎠
⎞⎜⎜⎝
⎛⎟⎟⎠
⎞⎜⎜⎝
⎛+−
−−
B
A
B
A
uu
Euu
ktkt
εε
)2/cos(2)2/cos(2
222 )2/(cos4 ε+±= ktE
k
E
ππ− 0
ε2
Metal and insulator in the band theory
k
E
aπ
aπ− 0
Interactions between electronsare ignored. (free fermion)
Each state (n,k) can accommodateup to two electrons (up, down spins).
Pauli principle
Band Insulator
k
E
aπ
aπ− 0
Band gap
All the states in the lower band are completely filled. (2 electrons per unit cell)
Electric current does not flow under (weak) electric field.
ε2
ε2
Topological (band) insulators
Condensed-matter realization of domain wall fermions
Examples: integer quantum Hall effect,
quantum spin Hall effect, Z2
topological insulator, ….
• バンド絶縁体
• トポロジカル数をもつ
• 端にgapless励起(Dirac fermion)をもつstable
Topological (band) insulators
Condensed-matter realization of domain wall fermions
Examples: integer quantum Hall effect,
quantum spin Hall effect, Z2
topological insulator, ….
• バンド絶縁体
• トポロジカル数をもつ
• 端にgapless励起(Dirac fermion)をもつ
Topological superconductorsBCS超伝導体
(Dirac or Majorana) をもつ
p+ip superconductor, 3He
stable
Example 1: Integer QHE
Prominent example: quantum Hall effect
• Classical
Hall effect
Br
e− −−−−−−
++++++
Er
vr
W
:n electron density
Electric current nevWI −=
BcvE =Electric field
Hall voltage IneBEWVH −
==
Hall resistanceneBRH −
=
Hall conductanceH
xy R1
=σBveFrrr
×−=Lorentz force
Integer quantum Hall effect
(von Klitzing 1980)
Hxy ρρ =
xxρ Quantization of Hall conductance
heixy
2
=σ
Ω= 807.258122eh
exact, robust against disorder etc.
Integer quantum Hall effect• Electrons are confined in a two-dimensional plane.
(ex. AlGaAs/GaAs interface)
• Strong magnetic field is applied(perpendicular to the plane)
Landau levels:
( ) ,...2,1,0 , ,21 ==+= n
mceBnE ccn ωωh
AlGaAs GaAsBr
cyclotron motion
k
E
ππ−
TKNN number (Thouless‐Kohmoto‐Nightingale‐den Nijs)TKNN (1982); Kohmoto (1985)
Che
xy
2
−=σ
Chern number (topological invariant)
∫∫ ⎟⎟⎠
⎞⎜⎜⎝
⎛
∂∂
∂∂
−∂∂
∂∂
=yxxy k
uku
ku
kurdkd
iC
**22
21π
( )yxk kkAkdi
, 21 2
rr×∇= ∫π
filled band
( ) kkkyx uukkA rrrr∇=,
integer valued
)(rue krki r
rrr⋅=ψ
Topological insulators: band insulators characterized by a topological number
Best known example:IQHE in 2DEG
Quantized Hall conductance
he
xy
2
×Ζ∈σ
Edge states
GS0=xyσ 1+=xyσ 2+=xyσ2−=xyσ 1−=xyσ
Quantum phase transitions
Space of gapped groundstates is partitioned intotopological sectors.
TKNN
Ζ∈#stable against disorder
Edge states• There is a gapless chiral edge mode along the sample
boundary.Br
xk
E
ππ−Number of edge modes C
hexy =
−=
/2
σ
Robust against disorder (chiral fermions cannot be backscattered)
Bulk: (2+1)d Chern-Simons theoryEdge: (1+1)d CFT
( )xm
x
Effective field theory
( ) ( ) zyyxx xmivH σσσ +∂+∂−=
( ) zyyxx mivH σσσ +∂+∂−=
parity anomaly ( )mxy sgn21
=σ
Domain wall fermion
( ) ( ) ⎟⎟⎠
⎞⎜⎜⎝
⎛−⎥⎦
⎤⎢⎣⎡ −= ∫ i
dxxmv
ikyyxx
y
1''1exp,
0σψ
vkE −= 0>m 0<m
Example 2: chiral p-wave superconductor
BCS理論
(平均場理論)
( ) ( ) ( )
( ) ( ) ( ) ( ) ( ) ( )[ ]∑∫
∑∫
↓=↑
++
↓=↑
+
Δ+Δ+
⎥⎦
⎤⎢⎣
⎡−−∇−=
,,
*,,
,
22
'','','21
2
βαβαβαβαβα
σσσ
ψψψψ
ψμψ
rrrrrrrrrrdd
rAiem
rrdH
dd
drrh
( ) ( ) ( ) ( )''',, rrrrVrr βαβα ψψ−=Δ 超伝導秩序変数
S‐wave (singlet) ( ) ( ) ( ) ( )rrrrr Ψ↑↓−↓↑−=Δ 2
1'',, δβα
0ξ
P‐wave (triplet)
+
( ) ( ) ( )rrrr
rr Ψ↑↑−∂∂
=Δ ''
',, δβα
xkk kk 0)( Δ∝∝Δ −ψψr
高温超伝導体22)( yxkk kkk −∝∝Δ −ψψ
r22 yx
d−
Integrating outGinzburg‐Landau
σψ
Spinless
px
+ipy
superconductor in 2 dim.• Order parameter
• Chiral (Majorana) edge state
)()( 0 yxkk ikkk +Δ∝∝Δ −ψψr
k
E
Δ
Ψ⋅Ψ=Ψ⎟⎟⎠
⎞⎜⎜⎝
⎛
−−−Δ+Δ−
Ψ= ++ 21
2)()()(2)(
21
22
22
σrr
kFFyx
FyxF hmkkkikk
kikkmkkH
Hamiltonian density ⎟⎟⎠
⎞⎜⎜⎝
⎛=Ψ +
−k
k
ψψ
⎟⎟⎠
⎞⎜⎜⎝
⎛ −+Δ−
Δ=
mkkk
kk
kkh Fyx
F
y
F
xk 2
222r
khEr
±=Gapped fermion spectrum22 : SS
hh
k
k →r
r
1=zL
( ) ( )[ ]ψψψψψμψ yxyxF
iik
im
H ∂−∂+∂+∂Δ
−⎟⎟⎠
⎞⎜⎜⎝
⎛−∇−= +++
222
2h
( )( )
( )( )⎟⎟⎠
⎞⎜⎜⎝
⎛=⎟⎟
⎠
⎞⎜⎜⎝
⎛ −+ rv
rue
trtr iEt h/
,,
ψψ
( )( ) ⎟⎟
⎠
⎞⎜⎜⎝
⎛=⎟⎟
⎠
⎞⎜⎜⎝
⎛⎟⎟⎠
⎞⎜⎜⎝
⎛−∂−∂Δ−
∂+∂Δ−
vu
Evu
hiiiih
yx
yx
0
0
Hamiltonian density
Bogoliubov-de Gennes equation
⎟⎟⎠
⎞⎜⎜⎝
⎛→⎟⎟
⎠
⎞⎜⎜⎝
⎛−→ *
*
,uv
vu
EE Particle-hole symmetry (charge conjugation)
zeromode: Majorana fermion
[ ]Ht
i ,ψψ=
∂∂
Majorana edge state
( ) ( )
( ) ( ) ⎟⎟⎠
⎞⎜⎜⎝
⎛=⎟⎟
⎠
⎞⎜⎜⎝
⎛
⎟⎟⎟⎟
⎠
⎞
⎜⎜⎜⎜
⎝
⎛
+∂+∂∂−∂Δ
−
∂+∂Δ
−+∂+∂−
vu
Evu
km
ik
i
ik
ikm
FyxyxF
yxF
Fyx
222
222
21
21
Δ<E
px
+ipy
superconductor: vacuum:0>y 0<y 0=⎟⎟⎠
⎞⎜⎜⎝
⎛∂∂
vu
y
( ) ⎟⎟⎠
⎞⎜⎜⎝
⎛−⎟⎟
⎠
⎞⎜⎜⎝
⎛ Δ+=⎟⎟
⎠
⎞⎜⎜⎝
⎛11
cosexp 22 ykkykmikx
vu
FFk
k
FkkE Δ=
k
E
Δ2
( ) ( ) ( )( )∫ +Δ−−Δ− +=F
FF
k
kktxik
kktxik eedktx
0
//
4, γγ
πψ
+=ψψ
( ) ( )∫∫ ∂Δ
−=Δ
= + yydyk
ikkdkH y
F
k
kkF
F
ψψγγ0
edge
• Majorana bound state in a quantum vortex
vortex ehc
=φ
Fn En / , 2000 Δ≈= ωωε
Bogoliubov-de Gennes equation
⎟⎟⎠
⎞⎜⎜⎝
⎛=⎟⎟
⎠
⎞⎜⎜⎝
⎛⎟⎟⎠
⎞⎜⎜⎝
⎛
−ΔΔ
− vu
vu
heeh
i
i
εϕ
ϕ
*0
0 ( ) FEAepm
h −+=2
0 21 rr
zero mode
phase⎟⎟⎠
⎞⎜⎜⎝
⎛⇒⎟⎟
⎠
⎞⎜⎜⎝
⎛− 2/
2/
ϕ
ϕ
i
i
veue
vu
⎟⎟⎠
⎞⎜⎜⎝
⎛⇔⎟⎟
⎠
⎞⎜⎜⎝
⎛ΨΨ+ v
u
00 =ε )( γ=Ψ=Ψ + Majorana (real) fermion!
ϕ
energy spectrum of vortex bound states
2N vortices GS degeneracy = 2N
phase winding:π2 γγ −→
interchanging vortices braid groups, non-Abelian statistics
i i+11+→ ii γγ
ii γγ −→+1
D.A. Ivanov, PRL (2001)
Fractional quantum Hall effect at
• 2nd
Landau level• Even denominator (cf. Laughlin states: odd denominator)• Moore-Read (Pfaffian) state
25
=ν
jjj iyxz +=
( ) ∑−Π⎟⎟⎠
⎞⎜⎜⎝
⎛
−= −
<
4/2MR
21Pf izjiji
ji
ezzzz
ψ ( ) ijij AA det Pf =
Pf( ) is equal to the BCS wave function of px
+ipy
pairing state.
Excitations above the Moore-Read state obey non-Abelian statistics.
Effective field theory: level-2 SU(2) Chern-Simons theory
G. Moore & N. Read (1991); C. Nayak & F. Wilczek (1996)
Example 3: Z2
topological insulator
Quantum spin Hall effect
Quantum spin Hall effect (Z2
top. Insulator)
• Time-reversal invariant band insulator• Strong spin-orbit
interaction
• Gapless helical edge mode (Kramers pair)
Kane & Mele (2005, 2006); Bernevig & Zhang (2006)
Br
Br
−
up-spin electrons
down-spin electrons
σλ rr⋅L
No spin rotation symmetry
kykx
E
K
K’
K’
K’
K
K
Kane-Mele model (PRL, 2005)
( )∑ ∑ ∑∑ ++++ +×++=ij ij i
iiivij
jzijiRjz
iijSOji cccdscicscicctH ξλλνλrr
t
SOiλ
SOiλ−
i j
ijdr
A B( ) ( )( ) ↓=↑=Ψ ⋅ , ,, skke sBsA
rkirrrr
φφ
( ) ( ) zv
yxxyR
zzSOy
yx
xK sssivHK σλσσλσλσσ +−+−∂+∂=
2333 :
(B) 1 (A), 1 −+=iξ
( ) ( ) zv
yxxyR
zzSOy
yx
xK sssivHK σλσσλσλσσ ++++∂+∂−=
2333 :' '
'*
Ky
Ky HisHis =− time reversal symmetry
• Quantum spin Hall insulator is characterized by Z2
topological index ν1=ν an odd
number of helical edge modes; Z2
topological insulator
an even (0)
number of helical edge modes0=ν1 0
Kane-Mele modelgraphene + SOI[PRL 95, 146802 (2005)]
Quantum spin Hall effectπ
σ2es
xy =
(if Sz
is conserved)
0=Rλ
Edge states stable against disorder (and interactions)
Z2
: stability of gapless edge states
(1) A single Kramers doublet
zzyyx
xxz sVsVsVVivsH ++++∂= 0 HisHis yy =− *
(2) Two Kramers doublets
( ) ( )zzyyx
xy
xz sVsVsVVsIivH ++⊗++∂⊗= τ0
remain to be gapless
opens a gap
Odd number of Kramers doublet (1)
Even number of Kramers doublet (2)
ExperimentHgTe/(Hg,Cd)Te quantum wells
Konig et al. [Science 318, 766 (2007)]
CdTeHgCdTeCdTe
Example 4: 3-dimensional Z2
topological insulator
3‐dimensional Z2
topological insulatorMoore & Balents; Roy; Fu, Kane & Mele (2006, 2007)
bulkinsulator
surface Dirac fermion(strong) topological insulatorbulk: band insulatorsurface: an odd
number of surface Dirac modes
characterized by Z2
topological numbers
Ex: tight‐binding model with SO int. on the diamond lattice[Fu, Kane, & Mele; PRL 98, 106803 (2007)]
trivial insulator
Z2
topologicalinsulator
trivial band insulator: 0 or an even
number of
surface Dirac modes
Surface Dirac fermions
• A “half”
of graphene
• An odd number of Dirac fermions in 2 dimensionscf. Nielsen-Ninomiya’s no-go theorem
kykx
E
K
K’
K’
K’
K
K
topologicalinsulator
Experiments• Angle-resolved photoemission spectroscopy (ARPES)
Bi1‐x
Sbx
p, Ephoton
Hsieh et al., Nature 452, 970 (2008)
An odd (5) number of surface Dirac modes were observed.
Experiments II
Bi2
Se3
Band calculations (theory)
Xia et al.,Nature Physics 5, 398 (2009)
“hydrogen atom”
of top. ins.
a single Dirac cone
ARPES experiment
トポロジカル絶縁体・超伝導体の分類
Schnyder, Ryu, AF, and Ludwig, PRB 78, 195125 (2008)
arXiv:0905.2029 (Landau100)
Classification oftopological insulators/superconductors
Schnyder, Ryu, AF, and Ludwig, PRB (2008)
Kitaev, arXiv:0901.2686
Zoo of topological insulators/superconductors
Topological insulators are stable against (weak) perturbations.
Classification of topological insulators/SCs
Random deformation of Hamiltonian
Natural framework: random matrix theory (Wigner, Dyson, Altland & Zirnbauer)
Assume only basic discrete symmetries:
(1) time-reversal symmetry
HTTH =−1*0 no TRS
TRS = +1 TRS with‐1 TRS with
TT +=Τ
TT −=Τ(integer spin)
(half‐odd integer spin)
(2) particle-hole symmetry
HCCH −=−Τ 10 no PHS
PHS = +1 PHS with‐1 PHS with
CC +=Τ
CC −=Τ(odd parity: p‐wave)
(even parity: s‐wave)
( ) HTCTCH −=−110133 =+×
(3) TRS PHS chiral symmetry [sublattice symmetry (SLS)]× =
yisT =
(2) particle-hole symmetry Bogoliubov-de Gennes
( ) ( ) zkyyxxkk
kkkk kkh
cc
hccH σεσσ ++Δ=⎟⎟⎠
⎞⎜⎜⎝
⎛= +
−−
+ 21
px
+ipy
Txkxkx CChh ==−=− σσσ *
dx2-y2
+idxy
( ) ( )[ ] zkyyyxyxkk
kkkk kkkkh
cc
hccH σεσσ ++−Δ=⎟⎟⎠
⎞⎜⎜⎝
⎛= +
↓−
↑↓−
+↑
22 21
Tykyky CiChh ==−=− σσσ *
10 random matrix ensembles
IQHE
Z2
TPI
px
+ipy
Examples of topological insulators in 2 spatial dimensionsInteger quantum Hall EffectZ2
topological insulator (quantum spin Hall effect) also in 3DMoore-Read Pfaffian state (spinless p+ip superconductor)
dx2‐y2
+idxy
Table of topological insulators in 1, 2, 3 dim. Schnyder, Ryu, Furusaki & Ludwig, PRB (2008)
Examples:(a)Integer Quantum Hall Insulator, (b) Quantum Spin Hall Insulator,(c) 3d Z2
Topological Insulator, (d) Spinless chiral p‐wave (p+ip) superconductor (Moore‐Read),(e)Chiral d‐wave superconductor, (f)
superconductor,
(g) 3He B phase.
Classification of 3d topological insulators/SCs
strategy (bulk boundary)• Bulk topological invariants
integer topological numbers:
3 random matrix ensembles
(AIII, CI, DIII)
• Classification of 2d Dirac fermions
Bernard & LeClair (‘02)
13
classes
(13=10+3) AIII, CI, DIII AII, CII
• Anderson delocalization in 2dnonlinear sigma models
Z2
topological term (2)
or
WZW term (3)
BZ: Brillouin zone
Topological distinction of ground states
m filledbands
n
empty
bands
xk
ykmap from BZ to Grassmannian
( ) ( ) ( )[ ] Ζ=×+ nUmUnmU2π IQHE (2 dim.)
homotopy class
deformed “Hamiltonian”
In classes AIII, BDI, CII, CI, DIII, Hamiltonian can be made off‐diagonal.
Projection operator is also off‐diagonal.
( )[ ] Ζ=nU3π topological insulators labeled by an integer
[ ] ( )( )( )[ ]∫ ∂∂∂= −−− qqqqqqkdq νμλλμνε
πν 111
2
3
tr24
Discrete symmetries limit possible values of [ ]qν
Z2
insulators in CII (chiral symplectic)
The integer number # of surface Dirac (Majorana) fermions( )qν
bulkinsulator
surfaceDiracfermion
(3+1)D 4-component Dirac Hamiltonian
( ) ⎟⎟⎠
⎞⎜⎜⎝
⎛
−⋅⋅
=+⊗=mk
kmmkkH x σστστ μμμ rrrr
AII: ( ) ( )kHikHi yy −=− σσ * TRS
DIII: ( ) ( )kHkH yyyy −−=⊗⊗ στστ * PHS
AIII: ( ) ( )kHkH yy −=ττ chS
[ ] ( )mq sgn21
=ν
( )zm
z
(3+1)D 8-component Dirac Hamiltonian⎟⎟⎠
⎞⎜⎜⎝
⎛= + 0
0D
DH
( ) ( ) ( )imkikikD yyy −⊗−=−= μμμμ σστγαβσ 5CI:
( ) ( )kDkDT −=
CII: ( ) ( )kDmkkD +=+= βαμμ ( ) ( )kDikDi yy −=− σσ *
[ ] ( ) 2sgn21
×= mqν
[ ] 0=qν
( )zm
z
Classification of 3d topological insulators
strategy (bulk boundary)
• Bulk topological invariants
integer topological numbers:
3 random matrix ensembles
(AIII, CI, DIII)
• Classification of 2d Dirac fermions
Bernard & LeClair (‘02)
13
classes
(13=10+3) AIII, CI, DIII AII, CII
• Anderson delocalization in 2dnonlinear sigma models
Z2
topological term (2)
or
WZW term (3)
Nonlinear sigma approach to Anderson localization• (fermionic) replica• Matrix field Q describing diffusion• Localization massive• Extended or critical massless topological Z2
termor WZW term
Wegner, Efetov, Larkin, Hikami, ….
( ) 22 ZM =π
( ) ZM =3π
Table of topological insulators in 1, 2, 3 dim. Schnyder, Ryu, Furusaki & Ludwig, PRB (2008)
arXiv:0905.2029
Examples:(a)Integer Quantum Hall Insulator, (b) Quantum Spin Hall Insulator,(c) 3d Z2
Topological Insulator, (d) Spinless chiral p‐wave (p+ip) superconductor (Moore‐Read),(e)Chiral d‐wave superconductor, (f)
superconductor,
(g) 3He B phase.
Reordered TableKitaev, arXiv:0901.2686
Periodic table of topological insulators
Classification in any dimension
Classification oftopological insulators/superconductors
Schnyder, Ryu, AF, and Ludwig, PRB (2008)
Kitaev, arXiv:0901.2686
Summary• Many topological insulators of non-interacting fermions
have been found.interacting fermions??
• Gapless boundary modes (Dirac or Majorana)stable against any (weak) perturbation disorder
• Majorana
fermionsto be found experimentally in solid-state devices
Z2
T.I. + s-wave SC Majorana
bound state (Fu & Kane)
Z2
T.I. + test charge Dyon
(Qi, Li, Zang, & S.-C. Zhang)
∫ ⋅= BExdtdhceS
rr3
2
2πθ
θ