Inti Sodemann (MIT) Séptima Escuela de Física Matemática, Universidad de Los Andes, Bogotá, Mayo 25, 2015
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1 Inti Sodemann (MIT) Séptima Escuela de Física Matemática, Universidad de Los Andes, Bogotá, Mayo 25, 2015
2 Contents Why are the fractional quantum Hall liquids amazing! Abelian quantum Hall liquids: Laughlin and the Composite Fermions Quantum Hall states in the sphere and the Shift The old story at filling for The surprise we found at for and : Ground states in torus and sphere, which are and singlets, are not composite fermion states! Summary
3 The A team
4 The A team Thierry Jolicoeur Universite Paris-Sud Fengcheng Wu Grad Student U Texas Soon to be in postdoc market!
5 Why fractional quantum Hall is amazing Electrons in two-dimensions and super strong magnetic fields B Landau levels: B
6 Why fractional quantum Hall is amazing The number of states available equals the number of magnetic flux quanta: B B Filling fraction:
7 Why fractional quantum Hall is amazing Stormer, Tsui, & Gossard, RMP (1999) A zoo of correlated liquids At certain rational fillings: B
8 Laughlin state as a paradigm A very stable correlated state at B B Laughlin, PRL (1983)
9 Composite Fermions Hierarchy Typically most robust states show up at Jain s sequence: Integer quantum Hall states bound to 2 flux quanta: Jain, PRL (1989)
10 Composite Fermions Hierarchy Composite Fermions describe abelian topological states. Topological properties of composite fermions agree with other Hierarchy constructions and with Chern-Simons. They represent the same phase. I believe the Hierarchy is a form of spontaneous symmetry breaking of indistinguishability (permutation symmetry).
11 Quantum Hall States on curved surfaces A sphere with a magnetic charge (monopoles): Haldane, PRL (1983)
12 Quantum Hall States on curved surfaces Aharonov-Bohm phase of electric test charge on surface:
13 Quantum Hall States on curved surfaces Aharonov-Bohm phase of electric test charge on surface:
14 Quantum Hall States on curved surfaces Aharonov-Bohm phase of electric test charge on surface:
15 Quantum Hall States on curved surfaces Aharonov-Bohm like phase of spinning particles on curved surface: Gauss-Bonnet
16 Quantum Hall States on curved surfaces Aharonov-Bohm like phase of spinning particles on curved surface: Gauss-Bonnet
17 Quantum Hall States on curved surfaces Aharonov-Bohm like phase of spinning particles on curved surface: Gauss-Bonnet
18 Quantum Hall States on curved surfaces Laughlin state on torus: Laughlin state on sphere: Emergent orbital spin of composite boson Wen & Zee, PRL (1992)
19 Shift (S) of states on sphere State on torus: State on sphere: Emergent orbital spin Wen & Zee, PRL (1992)
20 SU(2) states at 2/3 ( old news ) Two states compete: ferromagnet and a 2-component singlet. Singlet from composite fermions
21 SU(2) states at 2/3 ( old news ) Two states compete: ferromagnet and a 2-component singlet. Ferromagnet from composite fermions
22 SU(3) & SU(4) composite fermions at 2/3 No new states are expected: Ferromagnet 2-component singlet
23 Surprise for SU(3) at 2/3 Exact diagonalization on torus Three colors of electrons: B Electrons spontaneously choose an SU(3) singlet occupying all colors!!!
24 Surprise for SU(4) at 2/3 Exact diagonalization on torus Four colors of electrons: B Electrons spontaneously choose an SU(4) singlet occupying all colors!!!
25 SU(3) and SU(4) in sphere
26 Unexpected pattern in correlations Maybe the whole story at needs to be re-thougth?
27 Summary Fractional quantum Hall states are liquids with particle-like excitations which are a fraction of bare electrons and have fractional statistics: topological order. Abelian fractional quantum Hall liquids are condensates of composite bosons (Chern-Simons boson) with an emergent orbital spin which couples to the curvature of space. Composite fermions do not describe the new SU(3) and SU(4) singlet states we have discovered at. Microscopic understanding is missing.
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