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Presentation transcript:

The Landscape of the Hubbard model HARVARD Talk online: sachdev.physics.harvard.edu Subir Sachdev Highly Frustrated Magnetism 2010 Johns Hopkins University August 1

The Hubbard Model Will study the honeycomb and square lattices.

1. Honeycomb lattice: semi-metal and antiferromagnetism Dirac fermions and the Gross-Neveu model 2. Spin liquids Unified formulation as a SO(4) gauge theory 3. Instabilities of spin liquids Geometric phases, valence bond solids, and other competing orders Outline

Cenke Xu Harvard UCSB Liang Fu Harvard Physical Review Letters 105, (2010) and to appear

Outline 1. Honeycomb lattice: semi-metal and antiferromagnetism Dirac fermions and the Gross-Neveu model 2. Spin liquids Unified formulation as a SO(4) gauge theory 3. Instabilities of spin liquids Geometric phases, valence bond solids, and other competing orders

The Hubbard Model

Graphene

Semi-metal with massless Dirac fermions Brilluoin zone

Graphene Dirac semi-metal Insulating antiferromagnet with Neel order

Brilluoin zone

Outline 1. Honeycomb lattice: semi-metal and antiferromagnetism Dirac fermions and the Gross-Neveu model 2. Spin liquids Unified formulation as a SO(4) gauge theory 3. Instabilities of spin liquids Geometric phases, valence bond solids, and other competing orders

Outline 1. Honeycomb lattice: semi-metal and antiferromagnetism Dirac fermions and the Gross-Neveu model 2. Spin liquids Unified formulation as a SO(4) gauge theory 3. Instabilities of spin liquids Geometric phases, valence bond solids, and other competing orders

Quantum “disordering” magnetic order

S. Sachdev, M. A. Metlitski, Y. Qi, and S. Sachdev Phys. Rev. B 80, (2009)

Quantum “disordering” magnetic order

Projected fermion wavefunctions (Fisher, Wen, Lee, Kim,Senthil)

Projected fermion wavefunctions neutral fermionic spinons (Fisher, Wen, Lee, Kim,Senthil)

Projected fermion wavefunctions charged slave boson/rotor (Fisher, Wen, Lee, Kim,Senthil)

Projected fermion wavefunctions (Fisher, Wen, Lee, Kim,Senthil)

Projected fermion wavefunctions (Fisher, Wen, Lee, Kim,Senthil)

Projected fermion wavefunctions (Fisher, Wen, Lee, Kim,Senthil)

Unified spin liquid theory

By breaking SO(4) gauge with different Higgs fields, we can reproduce essentially all earlier theories of spin liquids. We also find many new spin liquid phases, some with Majorana fermion excitations which carry neither spin nor charge

Quantum “disordering” magnetic order

Phase diagram “Frustration”

Phase diagram “Frustration”

Phase diagram “Frustration” Semi-metal

Phase diagram “Frustration” Semi-metal Insulator with Neel order

Phase diagram “Frustration” Semi-metal Insulator with Neel order

Phase diagram “Frustration” Semi-metal Insulator with Neel order Spin liquid: CFT of SU(2) QCD with N f =4 massless Dirac quarks

Phase diagram “Frustration” Semi-metal Insulator with Neel order Spin liquid: CFT of SU(2) QCD with N f =4 massless Dirac quarks

Phase diagram “Frustration” Semi-metal Insulator with Neel order Spin liquid: CFT of SU(2) QCD with N f =4 massless Dirac quarks Confining insulator with VBS (kekule) order

Outline 1. Honeycomb lattice: semi-metal and antiferromagnetism Dirac fermions and the Gross-Neveu model 2. Spin liquids Unified formulation as a SO(4) gauge theory 3. Instabilities of spin liquids Geometric phases, valence bond solids, and other competing orders

Outline 1. Honeycomb lattice: semi-metal and antiferromagnetism Dirac fermions and the Gross-Neveu model 2. Spin liquids Unified formulation as a SO(4) gauge theory 3. Instabilities of spin liquids Geometric phases, valence bond solids, and other competing orders

“Frustration” S=1/2 square lattice antiferromagnetic insulator

Phase diagram “Frustration” Semi-metal Insulator with Neel order Spin liquid: CFT of SU(2) QCD with N f =4 massless Dirac quarks Confining insulator with VBS (kekule) order