Proliferation Transitions for Non-Abelian Anyons

Organisé par

Institut Henri Poincaré

Phases of matter and the transitions between them are famously characterized within the Landau paradigm and Landau–Ginzburg theory: phases are labeled by broken or unbroken symmetries, while phase transitions are described in terms of scalar order parameters. There are, however, phases beyond the standard Landau paradigm that are distinguished not by the realization of ordinary symmetries, but by

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