Wednesday, 5 June 2019
[1906.00971] Strong and Weak Many-Body Localizations
[1906.00983] Landau-Ginzburg Theories of Non-Abelian Quantum Hall States from Non-Abelian Bosonization
[1906.01283] Two-dimensional topological materials discovery by symmetry-indicator method
[1906.01628] Spectroscopy of spinons in Coulomb quantum spin liquids
[1906.00983] Landau-Ginzburg Theories of Non-Abelian Quantum Hall States from Non-Abelian Bosonization
[1906.01283] Two-dimensional topological materials discovery by symmetry-indicator method
[1906.01628] Spectroscopy of spinons in Coulomb quantum spin liquids
[1906.00883] A genuine realization of the spinless 4D topological insulator by electric circuits
[1906.00807] Spin chain network construction of chiral spin liquids
[1906.00708] Observations of zero electrical resistance of Au-Ag thin films near room temperature
[1906.00218] $\mathbb{Z}_Q$ Berry Phase for Higher-Order Symmetry-Protected Topological Phases
[1906.00210] Theory of skyrmion, meron, anti-skyrmion and anti-meron in chiral magnets
[1906.00807] Spin chain network construction of chiral spin liquids
[1906.00708] Observations of zero electrical resistance of Au-Ag thin films near room temperature
[1906.00218] $\mathbb{Z}_Q$ Berry Phase for Higher-Order Symmetry-Protected Topological Phases
[1906.00210] Theory of skyrmion, meron, anti-skyrmion and anti-meron in chiral magnets
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