gauge field of bloch electrons in dual space first considered in context of qhe kohmoto 1985...

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Page 1: Gauge Field of Bloch Electrons in dual space First considered in context of QHE Kohmoto 1985 Principle of Quantum Mechanics Eigenstate does

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Page 2: Gauge Field of Bloch Electrons in dual space First considered in context of QHE Kohmoto 1985 Principle of Quantum Mechanics Eigenstate does

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Page 4: Gauge Field of Bloch Electrons in dual space First considered in context of QHE Kohmoto 1985 Principle of Quantum Mechanics Eigenstate does

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Page 5: Gauge Field of Bloch Electrons in dual space First considered in context of QHE Kohmoto 1985 Principle of Quantum Mechanics Eigenstate does

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Page 6: Gauge Field of Bloch Electrons in dual space First considered in context of QHE Kohmoto 1985 Principle of Quantum Mechanics Eigenstate does

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Page 7: Gauge Field of Bloch Electrons in dual space First considered in context of QHE Kohmoto 1985 Principle of Quantum Mechanics Eigenstate does

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Page 8: Gauge Field of Bloch Electrons in dual space First considered in context of QHE Kohmoto 1985 Principle of Quantum Mechanics Eigenstate does

Gauge Field of Bloch Electrons in dual space

First considered in context of QHEKohmoto 1985

Principle of Quantum MechanicsEigenstate does not depend on overall phase factor

Gauge invariant magnetic field in dual space

Page 9: Gauge Field of Bloch Electrons in dual space First considered in context of QHE Kohmoto 1985 Principle of Quantum Mechanics Eigenstate does

Superconductivity and Quantized Flux

ratio of wave functions on sublattice A and B

write

U(1) field

Page 10: Gauge Field of Bloch Electrons in dual space First considered in context of QHE Kohmoto 1985 Principle of Quantum Mechanics Eigenstate does

Meissner effect

Hall conductanceKohmoto 1985

but if C contain Dirac point

no magnetic fieldtime reversal symmetry is not brokenHall conductance has to be zerosum of fluxes is zero monopole-antimonopole confinement

Page 11: Gauge Field of Bloch Electrons in dual space First considered in context of QHE Kohmoto 1985 Principle of Quantum Mechanics Eigenstate does

Dual Space of Honeycomb lattice

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Page 12: Gauge Field of Bloch Electrons in dual space First considered in context of QHE Kohmoto 1985 Principle of Quantum Mechanics Eigenstate does

Quantum Hall Effect

magnetic field induces breaking of the timereversal symmetry

Jx = σxyEy

•Laughlin•TKNN

Key advantages:magnetic fieldDissipationless response, sincetopological origin, due to gauge field in momentum spaceKohmoto (1985)also appear in Berry phase expression (k->adiabatic parameter)

Gauge field does not related to external magnetic field explicitly

Page 13: Gauge Field of Bloch Electrons in dual space First considered in context of QHE Kohmoto 1985 Principle of Quantum Mechanics Eigenstate does

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Hofstadter Butterfly

nonzero TKNN Hall conductance

Page 14: Gauge Field of Bloch Electrons in dual space First considered in context of QHE Kohmoto 1985 Principle of Quantum Mechanics Eigenstate does

nonzero TKNN Hall conductance

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Page 15: Gauge Field of Bloch Electrons in dual space First considered in context of QHE Kohmoto 1985 Principle of Quantum Mechanics Eigenstate does

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Page 16: Gauge Field of Bloch Electrons in dual space First considered in context of QHE Kohmoto 1985 Principle of Quantum Mechanics Eigenstate does
Page 17: Gauge Field of Bloch Electrons in dual space First considered in context of QHE Kohmoto 1985 Principle of Quantum Mechanics Eigenstate does

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Page 18: Gauge Field of Bloch Electrons in dual space First considered in context of QHE Kohmoto 1985 Principle of Quantum Mechanics Eigenstate does

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Page 19: Gauge Field of Bloch Electrons in dual space First considered in context of QHE Kohmoto 1985 Principle of Quantum Mechanics Eigenstate does

Jahn-Teller Theorem

Localized Object(molecule, impurity)If a molecule has degeneracy in electronic energy, there is at least one instability mode of symmetry breaking

CrystalBand Jahn-Teller effectPeirerls instability of one-dimensional half-filled band(dimerization)

Dirac Mode

massive massless

doubly degenerateNon degenerate

Page 20: Gauge Field of Bloch Electrons in dual space First considered in context of QHE Kohmoto 1985 Principle of Quantum Mechanics Eigenstate does

Jahn-Teller instability mode

K-K’

period 3 direction

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Page 21: Gauge Field of Bloch Electrons in dual space First considered in context of QHE Kohmoto 1985 Principle of Quantum Mechanics Eigenstate does

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tA tB 5%

Period 2 modulation

Period 3 modulation

Page 22: Gauge Field of Bloch Electrons in dual space First considered in context of QHE Kohmoto 1985 Principle of Quantum Mechanics Eigenstate does

SummaryHoneycomb Lattice: sublattice A and B, non-Bravais latticetopological dual space:

Dirac zero mode: break down of Bloch’s theoremground state degeneracy-> Jahn-Teller period 3 lattice modulation in

U(1) gauge field of Bloch electrons in dual space

Type II superconductor, Abrikosov quantized vortex, +1, -1

Magnetic monopole: non-Abelian gauge theory broken to U(1), cf ‘t Hooft

Page 23: Gauge Field of Bloch Electrons in dual space First considered in context of QHE Kohmoto 1985 Principle of Quantum Mechanics Eigenstate does

No magnetic fieldTime reversal symmetry -> zero Hall conductance -> monopole confinement

With a magnetic fieldHofstadter mechanism, 2q dual subspaces, nonzero TKNN Hall conductancemonopole deconfinement