topological insulators
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Topological Insulators. 组员:马润泽 金佳霖 孙晋茹 宋化鼎 罗巍 申攀攀 沈齐欣 生冀明 刘易. Introduction Brief history of topological insulators Band theory Quantum Hall effect Superconducting proximity effect. Outline. Close relation between topological insulators and several kinds of Hall effects. introduction. - PowerPoint PPT PresentationTRANSCRIPT
Topological Insulators
Topological Insulators
OutlineIntroductionBrief history of topological insulatorsBand theoryQuantum Hall effectSuperconducting proximity effectintroductionClose relation between topological insulators and several kinds of Hall effects.Brief history of topological insulatorsThe History of Topological InsulatorQHEQSHE3D TI2005 Kane & Mele 2006 HgTe / CdTe2007 Molenkamp 2007 FuKane Bi1-xSbx 3D TI2008 Hasan ARPES2009 Bi2Se3Bi2Te3Sb2Te32009 ARPES Hasan Bi2Se3 Bi2Te3 Hasan Sb2Te3
1980 1982 5
2D topological insulator
Shou-Cheng Zhang Group. Science 314, 1757 (2006)
2D topological insulatorMolenkamp Group. Science 318, 766 (2007)3D topological insulator
Liang Fu and C. L. Kane Physical Review B, 2007, 76(4): 045302.3D topological insulatorHasan Group. Nature, 2008, 452(7190): 970-974.
Band theory
Figure 1: the band structures of four kinds of material (a) conductors, (b) ordinary insulators, (c) quantum Hall insulators, (d) T invariant topological insulators
Band structuresThe Chern invariant n
Berry phase
Berry flux
The Chern invariant is the total Berry flux in the Brillouin zone
TKNN showed that xy, computed using the Kubo formula, has the same form, so that N in Eq.(1) is identical to n in Eq.(2).
Chern number n is a topological invariant in the sense that it cannot change when the Hamiltonian varies smoothly.
For topological insulators, n0, while for ordinary ones(such as vacuum), n=0.Haldane model
tight-binding model of hexagonal lattice a quantum Hall state with introduces a mass to the Dirac points
Edge states skipping motion electrons bounce off the edgechiral:propagate in one direction only along the edgeinsensitive to disorder :no states available for backscatteringdeeply related to the topology of the bulk quantum Hall state.
Z2 topological insulatorT symmetry operator:
Sy is the spin operator and K is complex conjugation
for spin 1/2 electrons:
A T invariant Bloch Hamiltonian must satisfy
Z2 topological insulator for this constraint,there is an invariant with two possible values: =0 or 1 two topological classes can be understood,is called Z2 invariant. define a unitary matrix:
There are four special points in the bulk 2D Brillouin zone.define:
Z2 topological insulatorthe Z2 invariant is:
if the 2D system conserves the perpendicular spin SzChern integers n, nare independent,the difference
defines a quantized spin Hall conductivity.The Z2 invariant is then simply
Z2 topological insulator
Surface quantum Hall effect
19Integer Quantized Hall Effect
20The explanation for the integer quantized Hall effect can be found in solid state physics textbooks. Here we will use a video for illustration
21**-422
Fig c A thin magnetic film can induce an energy gap at the surface. d A domain wall in the surface magnetization exhibits a chiral fermion mode.b180dbb//pptfor a single surface23Superconducting proximity effect and majorana fermionsMajorana 1937 Ettore Majorana Majorana
when a superconductor (S) is placed in contact with a "normal" (N) non-superconductor. Typically thecritical temperatureof the superconductor is suppressed and signs of weak superconductivity are observed in the normal material overmesoscopicdistances.
Majorana Majorana
Majorana
Majorana
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