Orbital-active honeycomb materials
Congjun Wu
Department of Physics, UC San Diego
Berkeley, 04/30/2019
K Kโ
๐ช
Yi Li (UCSD Princeton Johns Hopkins)
Gufeng Zhang (UCSD experiment)
Shenglong Xu (UCSD Univ. Maryland)
S. Das Sarma (University of Maryland)
L. Balents (UCSB)
Chuanwei Zhang (Washington state UT Dallas)
Gang Li (Shanghai Tech.)
Werner Hanke (Wuerzburg Univ.)
2
Collaborators
Orbital-active
honeycomb(๐๐๐๐), (๐ ๐๐, ๐ ๐๐)
(๐ ๐๐โ๐๐,
๐ ๐๐โ๐๐)
Large gap topo-insulator
Frustrated orbital exchange -120โ model
f-wave supercond.
Flat band: Wigner crystal, ferromagnetism
Bismuthene, Stanene
Polariton lattice
Twisted bilayer graphene
transition metal oxides
K Kโ
๐ช
The dual version (px, py) to graphene (pz)
Orbital-inactiveOrbital-active: degeneracy
E: (px, py)
A2 (๐๐ง) graphene
Recent foci:
bilayer twisted graphene(Paballo),
trilayer graphene: gate tunable Mott states (Feng Wang)
How to find orbital-active honeycomb system?
1/r-like potential
โข Need to passivate the ๐ and ๐๐ง-orbitals. 5
2s
2px 2py
1s
+ +
โข Graphene is not orbital-acitive
๐ ๐2-hybridization 2๐ , 2๐๐ฅ, 2๐๐ฆ, strong ๐ -bonds.
๐ -bands away from Fermi surface.
Flat band ferromagnetism,
Wigner crystal
Flat band and Dirac cones (orbital-enriched)
C. Wu, D. Bergman, L. Balents, and S. Das Sarma, PRL 99, 70401 (2007).C. Wu, PRL 101, 186107 (2008).
Dirac cones: orbital structure large gap topo-insulator
6
KKโ
๐ช
W. C. Lee, C. Wu, S. Das Sarma, PRA 2010; G.F. Zhang, Y. Li, C. Wu, PRB 90 (2014).
S. Z. Zhang, H. h. Hung, C. Wu, PRA 82, 053818 (2010).
Topology and frustration
QAHI(I)
QAHI(II)
Mott Insulator
120โ model
Doping (?)
semi-metal
f-wave SC๐/๐ก
๐/๐ก
CW, PRL.100, 200406 (2008). Lee, CW, Das Sarma, PRA (2010).
arxiv1807.02528, Cava, Broholm et al.
NaNi2BiO6
Orbital-active
honeycomb(๐๐๐๐), (๐ ๐๐, ๐ ๐๐)
(๐ ๐๐โ๐๐,
๐ ๐๐โ๐๐)
Large gap topo-insulator
Frustrated orbital exchange -120โ model
f-wave supercond.
Flat band: Wigner crystal, ferromagnetism
Bismuthene, Stanene
Polariton lattice
Twisted bilayer graphene
transition metal oxides
K Kโ
๐ช
Minimal Hamiltonian (๐ -bonding)
yx ppp2
1
2
3
1 yx ppp2
1
2
3
2 y
pp 3
1e
2e
3e
].)ห()([
].)ห()([
.].)ห()([
333
222
111//
cherprp
cherprp
cherprptHAr
t
โข p-bonding neglected โ good approx. in transition metal oxide. Not good in semiconductor.
p-bondtC. Wu, D. Bergman, L. Balents, and S. Das Sarma, PRL 99, 70401 (2007)
10
Flat bands -- localized eigenstates
โข If ๐กโฅ is included, flat bands narrow bands .
C. Wu, D. Bergman, L. Balents, and S. Das Sarma, PRL 99, 70401 (2007).
11
Observed! (polariton in the ๐๐ฅ-๐๐ฆ bands of the
honeycomb lattice)
โDirect Observation of Dirac Cones and a flatband in a honeycomb lattice for Polaritonsโ,
T. Jacqmin, I. Carusotto, et al. PRL 112, 116402 (2014)
xpyp
s
+-
+-
โข Wigner crystal (spinlessfermions or bosons).
Strong correlations in the flat-band
C. Wu, D. Bergman, L. Balents, and S.
Das Sarma, PRL 99, 70401 (2007).
S
โข Flat-band FM for spinfulfermions.
โข Large entropy good for cold
atom expt.
โข Skyrmion texture.
S. Z. Zhang, H. h. Hung, C. Wu, PRA 82, 053818 (2010).
33
13
Orbital ordering with strong repulsions
10/ // tU2
1n
โข Various orbital ordering insulating states at commensurate fillings.
Kekule pattern
14
How to make ๐๐ฅ /๐๐ฆ -orbital active?
G. Grynberg et al., Phys. Rev. Lett. 70, 2249 (1993).
also recent works from K. Sengstock, Esslinger, Blochโs groups.
โข px /py-orbital bands well separated from s.
โข Strong confinement along z-direction pz pushed to high energy
s
pharmonic-like potential
optical lattices
Transition metal oxide bilayer (111) LaNiO3
15D. Xiao, et,al., Nat.Comm. (2011); Ying Ran, et al, PRB, (2011).
๐๐2โ3๐ง2, ๐๐ฅ2โ๐ฆ2
๐๐ : 2d rep
Flat-band in โKagome grapheneโ
+โ
๐
โ๐
+
๐+
โ
Y. P. Chen, S. L. Xu, Y. Xie, C. Zhong, CW,
S. B. Zhang, PRB 98,035135 (2018).
Ferromagnetism and spontaneous quantum anomalous Hall state
LDA: dope holes:half-filled flat-band
Mean-field: Spontaneous generation of orbital moment โจ๐ฟ๐งโฉ = 0.004โ
Sun, Yao, Fradkin, Kivelson, PRL 2009
Y. P. Chen, S. L. Xu, Y. Xie, C. Zhong,
CW, S. B. Zhang, PRB 98,035135
(2018).
Wannier orbitals in twisted bilayer graphene
Liang Fu et al, PRX 8,
031087 (2018).
๐ = ๐๐๐๐ ๐
๐ ๐
๐๐
11i
i
Orbital-active
honeycomb(๐๐๐๐), (๐ ๐๐, ๐ ๐๐)
(๐ ๐๐โ๐๐,
๐ ๐๐โ๐๐)
FM , Wigner crystal in flat band
Frustrated orbital exchange -120โ model
f-wave supercond.
large topo-gap at the atomic SO energy scale
Bismuthene, Stanene
Polariton lattice
Twisted bilayer graphene
transition metal oxides
๐ ๐ -band inversion -- small gap
)(
)()(
kp
ksk
iyx
)(
)()(
kp
ksk
iyx
โข InAs/GaSb type II quantum well
s and p spatially separated, inversion controlled by gate potential.
C. X. Liu et al, PRL 100, 2336601 (2008),
R. R. Duโs group, PRL 115 136804 (2015) .
s
p
p
ss
p
โข HgTe/HgCdTe: s-p hybridization. Bernevig, Hughs, Zhang Science 314, 1757 (2006); Molenkampโs group, Science. 318 766โ770 (2007)
ฮ๐๐๐ฃ ฮ๐ก๐๐๐/ฮ๐๐๐ฃโ ๐ฟ๐๐0
๐ฟ๐
Orbital-active honeycomb systems
Real materials Bismuthene on SiC
Gap at the atomic SO coupling (1eV)
Topo-gap boosting mechanism
C. Wu, PRL 101, 186807 (2008)
M. Zhang, H. Hung, C. W. Zhang, C. Wu, PRA 83, 023615 (2011)
G. F. Zhang, Y. Li, C. Wu, PRB 90, 075114 (2014).
F. Reis, G. Li, L. Dudy, M. Bauernfeind, S. Glass, W. Hanke, R.
Thomale, J. Schafer, and R. Claessen, Science (2017).
G. Li, W. Hanke, E. M. Hankiewicz, F. Reis, J. Schaefer, R.
Claessen, C. Wu, R. Thomale, PRB 98, 165146 (2018).
K Kโ
๐ชStanene (Theory Xu, S. C. Zhang, Exp: Xue, Jia, He):
Topo-gap: solids v.s. AMO
))()(( rLrLH zr
zSO
โข Solids: ionic core soft pseudo-potential
zzyyxx LLLL
G. F. Zhang, Y. Li C. Wu, PRB 90 (2014).
(6s 6p no longer degenerate)
s
p
SO coupling: quantum spin Hall
โข AMO: Rotate each site around its own center.
)(rLHr
zzmn
C. Wu, PRL 101, 186107 (2008);
M. Zhang, Hung, C. Zhang, C. Wu, PRA (2011).
โข A/B sublattices decouple due to destructive interference๏ผnon-bonding states at K (Kโ)
B
1
2
B
B
K Kโฮ๐ธ = 2๐
๐ = ๐๐23๐ A
1
2
A
A
๐๐ฅ ยฑ ๐๐๐ฆ
Topological gap = Atomic level spacing
๐ป๐๐ = ๐๐ฟ๐ง๐๐ง โ ฮ๐ธ = 2๐
G. F. Zhang, Y. Li, CW,
PRB 90 (2014).
Bismuthene on the SiC substrate
G. F. Zhang, Y. Li, C. Wu, PRB 90, 075114 (2014).
F. Reis, et al, Science 2017.
Gang Li, W. Hanke, Ewelina, M. Hankiewicz, J. Schafer, R. Claessen, C. Wu, and R. Thomale, PRB (2018).
๐๐ฅ, ๐๐ฆ orbital-active
honeycomb materials
weak s-p hybridization
๐๐ง-orbital passivated
by the SiC
large topo-gap 2D materials
Strong SO coupling
โข Monolayer โ no buckling
โข Large topo-gap ~0.67eV (STM)
Double group: Rashba splitting
Spectra of Bismuthene on SiC
+ + โ
1 + 1 โ1
2=3
2โก โ
3
2(๐๐๐ 3)
โกโ+ +
๐๐ง = ยฑ5
2โก โ
1
2
1. F. Reis, G. Li, et al Science (2017).
2. Gang Li, W. Hanke, Ewelina, M.
Hankiewicz, J. Schafer, R.
Claessen, C. Wu, and R. Thomale,
PRB (2018).
)(, rLHr
zSO
AB
AB
Unification: Stanene - ฮ -point
G. F. Zhang, Y. Li, C. Wu, PRB 90 (2014).
๐ช
Y. Xu, et, al., PRL (2013) S. Chen, et, al., PRB (2014)
ฮ๐ธ = 2๐
Experiments: Menghan Liao, et al,
arxiv1712.03695,
Yunyi Zang, et al, arXiv1711.07035
Fengfeng Zhang et al, Mature
Materials 14, 1020 (2015).
Orbital-active
honeycomb(๐๐๐๐), (๐ ๐๐, ๐ ๐๐)
(๐ ๐๐โ๐๐,
๐ ๐๐โ๐๐)
FM , Wigner crystal in flat band
Frustrated orbital exchange -120โ model
f-wave supercond.
large topo-gap at the atomic SO energy scale
Bismuthene, Stanene
Polariton lattice
Twisted bilayer graphene
transition metal oxides
band topology, orbital frustration
QAHI(I)
QAHI(II)
Mott Insulator
120โ model
Doping (?)
semi-metal
f-wave SC๐/๐ก
๐/๐ก
CW, PRL.100, 200406 (2008). Lee, CW, Das Sarma, PRA (2010).
arxiv1807.02528, Cava, Broholm et al.
NaNi2BiO6
Mott insulator of SPINLESS fermions: orbital exchange
U
29
โข Pseudo-spin representation.
)(2
11 yyxx pppp )(
2
12 xyyx pppp )(
23 xyyxi pppp
โข Orbital exchange: no orbital flipping process.
0J
UtJ /2 2
UtJ /2 2
)ห()( 11 xrrJH ex
โข Ising quantization axis depends on bond orientation.
xp
: eigen-states of yxe 2sin2cosห2
2e
)ห)ห()(ห)(( 22 eererJH ex
Hexagon lattice: quantum model120
)ห)(()ห)((,
ijjiji
rr
ex ererJH
โข Transformation: the Ising quantization axes bond orientations.
A B
B
B
11 ))(( 22
3
12
1
22
3
12
1
))(( 22
3
12
1
22
3
12
1
ypyx pp ,
30
C. Wu et al, arxiv0701711v1; C. Wu, PRL
100, 200406 (2008). E. Zhao, and W. V.
Liu, Phys. Rev. Lett. 100, 160403 (2008)
From the Kitaev model to 120 degree model
A B
B
B
xxyy
zz
โข cf. Kitaev model: Ising quantization axes form an orthogonal triad.
))()(
)()()()((
3
21
err
errerrJH
zz
yyxx
Ar
kitaev
Kitaev
cos02
1
120
31
120
32
Large S picture: heavy-frustration of classic ground states
โข Ground states: the two -vectors have the same projection along the bond orientation.
or
rzrr
rrex rJerrJH )(}ห)]()({[( 22
,
โข Ferro-orbital configurations. โข Loop config: -vectors along the tangential directions.
Heavy-degeneracy of the classic ground states
โข General loop configurations
33
34
Global rotation degree of freedom
โข Each loop config remains in the ground state manifold by a suitable arrangement of clockwise/anticlockwise rotation patterns.
35
โOrder from disorderโ: 1/S orbital-wave correction
36
Zero energy orbital wave fluctuations
4
22
)(
)cos1(6
JSE
โข Each loop has a local zero energy mode.
โข The closest packed config. contains the maximal number of zero modes selected by quantum fluctuations.
f-wave structure from conventional interaction
โข Bisector lines are nodal lines: no interaction between TR pairs.
โข The TR pair at K and Kโ has the largest pairing.
nodal lines
)()()()(int rnrnUrnrnUHyxyxyx ipp
rippp
rp
K K
yxipp
yxipp
yxipp
yxipp
k
k
A
B
A
B
A
B
A
B
38
Orbital-assisted f-wave superconductivity
inkout
k
Zero energy Majorana boundary modes
W. C. Lee, CW, S. Das Sarma, PRA 2010;
39
A unified framework for bismuthen, stanene, and more โฆ
โข ๐๐ฅ and ๐๐ฆ orbital-active honeycomb lattice
โข Large topo gap to the scale of atomic spin-orbit coupling (1eV)
โข Novel many-body physics: flat-band ferromagnetism, orbital frustration, f-wave superconductivity etc.
Back up!
Orbital configuration (Dirac band)
โข Complex eigen-orbitals at K (Kโ) large topo-gap with SO
coupling.
C. Wu PRL 101, 2008; W. C. Lee, C. Wu, S. Das Sarma, PRA 2010; G. F. Zhang, Y. Li C. Wu, PRB 90 (2014).
M
K K
k
k
M
โข Real eigen-orbitals along the M-ฮ -M- line f-wave pairing.
๐ต site
A
1
2
A
A
B
1
2B
B
+
-
+
-
+
-
+
-
+
-
+
-
๐๐ฅ ยฑ ๐๐๐ฆ
Add interactions (spinless fermions)
)()(int rnrnUHyx p
rp
U
)(0 rLHHr
zt
///t
///tU
QAHI(I)
QAHI(II)
semi-metal
Mott Insulator
120 model
(Quantum) anomalous Hall state
โข Van Vleck (inter-band) response.
B
1
2B
B
E
K Kโ
A
1
2
A
A
โข k-space Berry curvature.
โข Anomalous velocity. Luttinger, PR, 112 793 (1958), Xiao, Chang, Niu, RMP 82, 1959 (2010).
๐ด ๐ = ๐๐ฟ,๐ ๐ ๐๐ ๐๐ฟ,๐ , ฮฉ๐ง ๐ = ๐๐๐ฅ๐ด๐๐ฆ โ ๐๐๐ฆ๐ด๐๐ฅ
๐๐ฅ๐ฆ =๐2
โ
๐2๐
2๐ฮฉ๐ง
=๐2
โ
๐2๐
2๐๐ป ร ๐ด ๐ = ยฑ
๐2
โ
๐๐ ๐ฒ = ๐๐ณ(๐โฒ) ๐ = ๐๐ธ + ๐ ๐ ร ๐ต ( ๐)
๐ = ๐ป๐๐ ๐ โ ๐ ร ฮฉ(๐)
Thouless, Kohmoto, Nightingale, den Nijis, PRL 49, 405 (1982)
Creation of chiral phonon and large momentum exciton
1. Right-handed light exciton at
K-valley
eV15.0
eV65.1
Kv
2. Another right-handed light
hole scattered to Kโ-valley by absorbing phonon and emitting a chiral phonon (K-Kโ=2K=Kโ )
3. Electron and hole are in different valleys large
momentum exciton.
Edge spectra and Berry curvature (spin )
//3.0 t
1C
)1(10 C
1
0
0
1C
45
C. Wu, Phys. Rev. Lett. 101, 186807 (2008).
K Kโ
G
Quantum anomalous Hall (QAH): a triangle relation
โข The 3rd gap mechanism: Neel exchange.
))()(( , r
BzAzN rSrSnH
โข Superpose charge and spin sub-lattice asymmetry.
FM
FM
m
nnm || nm
topo trivial topo non-trivial
spin-up spin-down
โข QAH -- Three players: none should be too large, too small either.
G. F. Zhang, Y. Li, C. Wu, PRB 90
(2014). Q.F. Liang, L.H. Wu, X. Hu, NJP 2013.
โข Gaps around K (Kโ) valley Hall.
Gaps due to sub-lattice asymmetry m > l (cf. MoS2)
)( mE
B
1
2
B
B
B
1
2
B
B
)( mE
ixyyxd
222 22 3zrd
MoS2: upper bands are replaced by
47
))()(( r
BAM rnrnmH
Honeycomb lattice system (graphene)
B
A
)(
)()(
kc
kck
B
A
โข 2-level in a planar pseudo-B field.
K Kโ
1e2e
3e
A
B B
Bโข Symmetry and topology protection:
gapless Dirac cones โ ๐พ = โ ๐พโฒ = 0 .
๐ป ๐ = โ ๐ โ ๐
โ๐ฅ ๐ + ๐โ๐ฆ ๐ =
๐=1
3
๐๐๐โ ๐๐ , โ๐ง ๐ = 0
Selected References
1. G. Li, W. Hanke, E. M. Hankiewicz, F. Reis, J. Schaefer, R. Claessen, C. Wu ,
R. Thomale, PRB 98, 165146 (2018).
2. G. F. Zhang, Yi Li, C. Wu, PRB 90, 075114 (2014).
3. M. Zhang, H. Hung, C.W. Zhang, C. Wu, PRA 83, 023615 (2011).
4. C. Wu, PRL 101, 186807 (2008).
5. C. Wu, PRL 100, 200406 (2008).
6. C. Wu, D. Bergman, L. Balents, and S. Das Sarma, PRL. 99, 70401 (2007).
49
Early work: on-line video
http://online.kitp.ucsb.edu/online/lowdim_c09/wu/
My research webpage
https://wucj.physics.ucsd.edu/research/topo/pQSH.html
https://wucj.physics.ucsd.edu/research/coldatom/pband.html
Large topo-gaps ~ atomic SO coupling strength
KKโ
๐ช
)(rLHr
zso
Little group: ฮฉ=0 ฮฉ>0 degeneracyฮ D6 C6 21+1
K(Kโ) D3 C3 21+1
2
2
1C
0
0
1
50
)(rLHr
z
K Kโ
๐ช