Quantum entanglement in condensed matter systems (2/4)

Grégoire Misguich

IPhT

Fri, May. 29th 2015, 10:00-12:00

Salle Claude Itzykson, Bât. 774, Orme des Merisiers

Quantum entanglement has become a central subject of research in the field of quantum many-body physics. In the last ten years, concepts of quantum information theory have found conceptual and practical applications to condensed-matter problems, from lattice spin models to the fractional quantum Hall effect. \par In particular, an important discovery is that the low-energy states of short-ranged Hamiltonians are much less entangled than states picked at random in the Hilbert space, or than highly excited eigenstate of the same Hamiltonians. This is known as the area law (or boundary law): the entropy of a large subsystem scales like its surface, whereas an extensive termal entropy would scale like the volume and therefore grow much faster as a function of the size. The entanglement entropy then encodes many important low-energy and long-distance physical properties of many-body systems, such as long-range order, spontaneous symmetry breaking, algebraic correlations, and the nature of elementary excitations. \par These lectures will start by introducing some basic definitions and concepts: \\ - the reduced density matrix, \\ - the Schmidt decomposition, \\ - the Von-Neumann and Rényi entropies, \\ - the boundary law. \par Then, we will describe and explain a selection of key ideas and results in the field: \\ - entanglement in free fermion systems and Fermi seas, \\ - logarithmic divergence of the entanglement entropy in critical 1d systems, \\ - matrix-product states, \\ - bulk-edge correspondence and the entanglement spectrum in 2d, \\ - the topological entanglement entropy.

Contact : Sylvain
RIBAULT