[1801.04935] On the Structure of Edge State Inner Products in the Fractional Quantum Hall Effect
[1801.04936] Loop Models, Modular Invariance, and Three Dimensional Bosonization
[1801.05020] Ultrathin Films of Superconducting Metals as a Platform for Topological Superconductivity
[1801.05438] Do the surface Fermi arcs in Weyl semimetals survive disorder?
[1801.05698] Engineering Quantum Spin Liquids and Many-Body Majorana States with a Driven Superconducting Box Circuit
[1801.05811] Topological energy conversion through bulk/boundary of driven systems
[1801.06177] Entanglement signatures of emergent Dirac fermions: kagome spin liquid & quantum criticality
[1801.06178] Translationally invariant non-Fermi liquid metals with critical Fermi-surfaces: Solvable models
[1801.04936] Loop Models, Modular Invariance, and Three Dimensional Bosonization
[1801.05020] Ultrathin Films of Superconducting Metals as a Platform for Topological Superconductivity
[1801.05438] Do the surface Fermi arcs in Weyl semimetals survive disorder?
[1801.05698] Engineering Quantum Spin Liquids and Many-Body Majorana States with a Driven Superconducting Box Circuit
[1801.05811] Topological energy conversion through bulk/boundary of driven systems
[1801.06177] Entanglement signatures of emergent Dirac fermions: kagome spin liquid & quantum criticality
[1801.06178] Translationally invariant non-Fermi liquid metals with critical Fermi-surfaces: Solvable models
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