topological insulators yew san hor 1 department of chemistry and j. g. checkelsky 2, a. richardella...
TRANSCRIPT
Topological InsulatorsYew San Hor
1Department of Chemistryand
J. G. Checkelsky2, A. Richardella2, J. Seo2, P. Roushan2, D. Hsieh2, Y. Xia2, M. Z. Hasan2, A.
Yazdani2, N. P. Ong2, and R. J. Cava1
2Department of PhysicsPrinceton University
NSF-MRSEC DMR 0819860
TAR College, Kuala Lumpur, Malaysia13 July 2010
Albert Einstein
E = mc2
Photo by Ch’ng Ping Choon
Einstein’s house at Princeton 1935-55
Princeton Campus
Princeton Chemistry Department
Spring 2009
Princeton Physics Department
Ch’ng Ping Choon
Richard Feymann
Princeton Science Library
Princeton Condensed Matter GroupPhysics & Chemistry
NSF-MRSEC
Robert J. Cava
Matthias Prize for New Superconducting Materials 1996
Chemistry
Nai Phuan Ong
• Director of NSF MRSEC DMR 081986
• 2006 Kamerlingh Onnes Prize (For research accomplishments in HTc superconductor)
Physics
Zahid HasanDavid Hsieh
Bob Cava
Yew San Hor
t = 10-32 sec
Dirac equation (μ∂ μ + mc)ψ = 0
Relativistic energy
E2 = p2c2 + m2c4
E
k
E ~ k
Elementary particles
t ~ 300,000 years
t ~ 300,000 years
Condensed Matter
Non-relativistic energy
E~k2
E
k
Schroedinger Equation:Schroedinger Equation:
t ~ 1.5 × 1010 years
t ~ 1.5 × 1010 years
source: spie.org
LLss
EE
kk
Bulk InsulatorBulk Insulator
Strong Spin-OrbitCoupling
Strong Spin-OrbitCoupling
E~k2E~k2
BCBBCB
BVBBVB
LLss
EE
kk
Bulk InsulatorBulk Insulator
Strong Spin-OrbitCoupling
Strong Spin-OrbitCoupling
E~k2E~k2
BCBBCB
BVBBVB
EE
kkSVBSVB
SCBSCB
E~kE~kSurface ConductorSurface Conductor
…is a band insulator which is characterized by a topological
number and has Dirac-like excitations at its boundaries.
Topology…is the mathematical study of the
spatial properties that are preserved under continuous deformations of objects, for examples, twisting and stretching, but no tearing or gluing.
Topology
=
sphere ellipsoid
Topology
=
Topologyin condensed matter electronic phases…
Electron spin property plays an important role.
Example:
AA BB
Insulatormaterial does not conduct electric current
1. Band Insulator (valence band completely filled).2. Peierls Insulator (lattice deformation).3. Mott Insulator (Coulomb repulsion).4. Anderson Insulator (impurity scattering).
A new class of insulator
Topological Insulator
Topological Insulators• Bulk band insulators.
Ingredients:Strong spin-orbit coupling.Time reversal symmetry.
E
k
E
k
Gapless surface state
Gapped bulk insulator
• Gapless Dirac excitations at its boundaries.
E ~ k2
BulkConduction Band
Bulk Valence Band
E ~ k
SurfaceConduction Band
SurfaceValence Band
Consider a simpler system 2D electron gas as an analogy
2D electron gas
No boundary
Applied B-field out of plane
When boundary is created, interface with vacuum state→ Edge state.
Electron charge → Quantum Hall effect
Conducting edge state
Insulator
Vacuum
…but this breaks Time Reversal Symmetry.
Electron charge → Quantum Hall effect
Broken Time Reversal Symmetry
Conducting edge state (Reversed with T operator)
Electron charge → Quantum Hall effect
Hall effect “charge”Electron charge → Quantum
Quantum Hall EffectClassical Hall Effect
Lorentz ForceF = -e x B
Hall conductancexy = -ne/B
Quantization of Hall conductance
xy = ie2/h
h/e2 = 25812.807
(Klaus von Klitzing, 1980)
1985 Nobel Prize in Physics
Fractional Quantum Hall Effect
Quantization of Hall conductance
xy = ie2/h
i = 1/3, 1/5, 5/2, 12/5 ..
(discovered in 1982)
Daniel Tsui Horst Stormer
Robert Laughlin
1998 Nobel Prize in Physics
Devices utilize electron charge property: Semiconductor
Transistor, AT&T Bell Labs (1947).Single Crystal Germanium (1952).Single Crystal Silicon (1954).IC device, Texas Instrument (1958).IC Product, Fairchild Camera (1961).Microprocessor, Intel (1971).Personal Computer (1975).
Semiconductor crisisGorden Moore (co-founder of Intel 1964):
Number of transistors doubled every 12 months while price unchanged.
In 1980s, number of transistors doubled every 18 months.
*Size limit*Heat dissipation
So, we need to find a new material
New materials utilize electron spin property:
Topological Insulators
Topological Insulators
Spintronic devices
- apply electron spin property.
Quantum computer
- apply quantum mechanical phenomena.
- use qubit (quantum bit) instead of bit.
Topological Insulator
is also important for…
1. Quantum Spin Hall Effect.2. The search of Majorana fermion.3. Axion electrodynamic study.4. Magnetic monopole.
3D Topological Insulator
Bulk insulator
L
s
Strong spin-orbit couplingL
s
L
s
L
s
L
s
L
s
Large atomic number → Large orbital moment, L
No boundary
3D Topological Insulator
Bulk insulator
L
s
Strong spin-orbit coupling
L
s
L
s
3D Topological Insulator
Bulk insulator
L
s
Strong spin-orbit coupling
Etrap
Etrap
s
s
k1k2
k x Etrap ~ B
3D Topological Insulator
L
s
Etrap Etrap
s
s-k2 -k1
Time Reversal Symmetry
Invariant!
Bulk insulator
Strong spin-orbit coupling
When T-operator is applied…
3D Topological Insulator
Bulk insulator
L
s
Strong spin-orbit coupling
L
s
L
s
Electron spin Quantum spin Hall effect
Surface Dirac-like spin current.Zero net current, but spin-polarization,protected by Time Reversal Symmetry
• Bi • Bi1-xSbx • Sb• Bi2Se3 • Bi2Te3
• Sb2Te3• will look for more…
Nature 452, 970 (2008)
Science 321, 547 (2008)
Nature Physics 5, 398 (2009)
Bi
Bi2Se3
Bi0.9Sb0.1
Bi1-xSbx
Topological insulators
Basics of ARPES
ARPES is surface sensitive
Can measure E vs k of bulk and surface states separately
Damascelli et al. RMP 2003
h
(Angle-resolved photoemission spectroscopy)
EE
EE
kkSVBSVB
SCBSCB
E~kE~kDirac surface stateDirac surface state
ARPES
Surface Dirac-like spin current.Zero net current, but spin-polarization,protected by Time Reversal Symmetry
k
E
Gaplesssurfacestate
EF
Challenging problem for
Dirac surface state transport measurements
Why not bulk insulator?
Bulk electron is measured
BCB
Imperfect World
Defect chemistry in Bi2Se3
SeSe → VSe●● + Se (gas) + 2 e-
defect
n-type Bi2Se3
10 nm
e-e-
STM
Bi
Se
Se
Bi
Se
Se
Se
Se
Se
Se
Bi
Bi
Bi
Ca-doped in Bi2Se3
2Ca
defect
n-type Bi2Se3
10 nm
e-e- → 2CaBi’ + 2h•
p-type Bi2Se3 STM
Bi
Se
Se
Bi
Se
Se
Se
Se
Se
Se
Bi
Bi
Bi
Bi2-xCaxSe3 Crystal growth
1st step: (i) stoichiometric mixture of Bi and Se in vacuum quartz tube. (ii) melting at 800 oC for 16 hours. (iii) air-quenching to room temperature.
2nd step: (i) add Ca to Bi2-xSe3 and sealed in vacuum quartz tube. (ii) 400 oC for 16 hours. (iii) 800 oC for 1 day. (iv) 1 day slow cooling
to 550 oC. (v) stay at 550 oC for 3 days.
PRB 79 195208 (2009)
n- to p-type Bi2-xCaxSe3 topological insulator
X=0
X=0.02
X = 0
X=0.02k
E
k
E
PRB 79 195208 (2009)
x = 0x = 0.005, 0.02, 0.05
Fine tuning in Bi2-xCaxSe3
Bi2Se3 Bi1.9975Ca0.0025Se3 Bi1.99Ca0.01Se3
Nature 460, 1101 (2009)
Metallic behavior.
Non-metallic.Onset at T~130 K.
x = 0.0025x > 0.005x = 0
PRL 103, 246601 (2009)
Bi2-xCaxSe3 transport properties
Bi1.9975Ca0.0025Se3
Quasi-periodic fluctuations
Surface state?
PRL 103 246601 (2009)
Te annealing of Bi2Te3
Annealing temperature: 400 – 440 C (1 week)
Te powder As-grown Bi2Te3 crystal
Transport property of Bi2Te3
kx (Å-1)
EB (
eV)
Fine tuning of Bi2Te3+
As-grown
EF S1S2
S3
S4
Dirac States in topological insulator Bi2Te3
Science (in press)
Non-metallic Metallic
kx
EB
EB
kx
dxx
/dH
HHHH
HH
HH
2D Fermi Surface 3D Bulk State
On the other hand…
Bi2Se3 can be doped to become more conducting…
Superconductor
Cu-intercalated Bi2Se3
By C.Kane (U Penn.)
superconductor
CuxBi2Se3
Cux
Cux
Cux
Cu-doped Bi2Se3 crystal growth
• Mixtures of high purity elements Bi, Cu, Se in sealed vacuum quartz tubes.
• Melt at 850 oC overnight.• Slow cooling: 850 → 620 oC for 24 hours.• Quench in cold water at 620 oC.
STM topography of Cu0.15Bi2Se3
T = 4.2 K
Cu clusters on surface. Cu atoms intercalated between layers
Superconductivity of CuxBi2Se3
Superconductivity only found in 0.1 < x < 0.3
Tc~3.8 K
~20 % SC phase
SC phase is not fully connected.
PRL 104 057001 (2010)
Superconductivity of CuxBi2Se3
Upper critical field Hc2 is anisotropic
Strongly type II superconductor
Bi2Se3 topological insulator+
CuxBi2Se3 superconductor
Majorana Fermionic Physics.
(?)
Topological magnetic insulators
• Motivated by:• Axion electrodynamics theory → E x B.• Magnetic monopole → symmetries of Maxwell’s
equations.• by Zhang group (Stanford), arXiv:0908.1537v1
Ferromagnetism in Bi2-xMnxTe3
For axion electrodynamics
1. Quantum Spin Hall Effect: (b) Transport measurements
Point charge
Vacuum
Topologicalinsulator
Magnetic monopole induced
Surface currentinduced
S. C. Zhang, Science 323 1184 (2009)
Axion electrodynamics
Schematic diagram for the studies of axion electrodynamics
1. Quantum Spin Hall Effect: (b) Transport measurements
Gold-copper alloy contacts
I+ V+ V- I-
Induced surface current
E field
TI crystal
Sharp tip acts as a point charge
Mn-doped Bi2Te3
Mn-substituted Bi2Te3 (Bi2-xMnxTe3)
Bi/Mn
Te
Te
Bi/Mn
Te
Te
Te
Te
Te
Te
Bi/Mn
Bi/Mn
Bi/Mn
STM topography of Bi1.91Mn0.09Te3
Black triangles: substitutional Mn on Bi sites. No Mn-clustering is found.
DC Magnetization of Bi2-xMnxTe3
TC ~ 9 – 12 K for x = 0.04 and 0.09
ARPES
Topological surface state is still present. Dispersion relation of the state is changed in a subtle fashion.
T=15 K
PRB 81,195203 (2010)
Summary● Ca-doped Bi2Se3 → Topological “Insulator”.
suppress bulk conductance to show up Dirac electron surface state.
● Cu-added Bi2Se3 → Superconductor.
interface with Bi2Se3 to have proximity effect, Majorana fermionic physics (?).
● Mn-doped Bi2Te3 → Magnetic topological insulator.
in search for magnetic monopole (?) and
axion electrodynamics studies (?).
AcknowledgementsCava group:
• Professor Robert Cava• Tyrel McQueen (JHU)• Don Vincent West (U Penn)• Anthony Williams• David Grauer (UC Berkeley)• Jared Allred• Shuang Jia• Siân Dutton• Esteban Climent-Pascual• Martin Bremholm• Ni Ni• Ulyana Sorokopoud• Linda Peoples
Funding agencies:
Air Force Office of Scientific Research (AFOSR).
Materials Research Science & Engineering Centers (MRSEC).
Thank you
References:Bernevig, Hughes, Zhang, Science 2006.Fu, Kane, Mele, PRL 2007.Moore, Nature 2010.Bjorken, Relativistic Quantum Mechanics.