| Tue, July-30-2013 |
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| Superconductivity, superfluidity |
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| 09:30-10:15 | Yip | Order parameter and surface states for superconducting Cu:Bi2Se3 |
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| 10:15-10:45 | Pollet | Lattice modulation of a two-dimensional superfluid: could it be … the Higgs particle? |
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| 10:45-11:15 | | Coffee break |
| Disordered systems |
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| 11:15-12:00 | Rieger | The two-dimensional disordered Bose-Hubbard model: phase diagrams and new applications |
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| 12:00-12:30 | Iglói | Random quantum magnets in d >= 2 dimensions: critical behavior and entanglement entropy |
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| 12:30-14:00 | | Lunch |
| Deconfined quantum-criticality |
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| 14:00-14:45 | Kawashima | Quantum phase transition in SU(N) J-Q Heisenberg model |
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| 14:45-15:15 | Sen | Low-energy excitations of near-critical 2D antiferromagnets |
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| 15:15-15:45 | | Coffee break |
| 15:45-16:30 | Kaul | Fate of CP(N-1) fixed points with q-monopoles | | |
| 16:30-17:00 | Beach | Resonating-valence-bond trial wave functions (and beyond) for frustrated quantum magnets |
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| Wed, July-31-2013 |
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| Topological states, fractionalization |
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| 09:30-10:15 | Assaad | Phase diagram of the Kane-Mele Hubbard model |
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| 10:15-10:45 | Schuch | Characterizing topological order in Projected Entangled Pair States |
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| 10:45-11:15 | | Coffee break |
| 11:15-12:00 | Singh | Yb2Ti2O7 a model Quantum Spin Ice |
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| 12:00-12:30 | Pollmann | Topological phases in gapped edges of fractionalized systems |
| 12:30-14:00 | | Lunch |
| Quantum computing, dissipation |
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| 14:00-14:45 | Poulin | The search for a new, self-correcting phase of matter | |  |
| 14:45-15:15 | Wei | Universal quantum computation with AKLT states |
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| 15:15-15:30 | | Coffee break |
| 15:30-16:15 | Cugliandolo | From Brownian dynamics to impurity motion in 1D quantum liquids |
| 16:15-17:00 | Young | Mind the Gap -- Could a quantum computer solve optimization problems efficiently? |
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