The insulating state of matter: a geometrical theory
Raffaele Resta (Instituto Officina dei Materiali, CNR, Trieste, Italy)
Abstract: The insulating versus conducting behavior of condensed matter is commonly addressed in terms of electronic excitations and/or conductivity. At variance with such wisdom, W. Kohn hinted in 1964 that the insulating state of matter reflects a peculiar organization of the electrons in their ground state, and does not require an energy gap. Kohn’s “theory of the insulating state” got a fresh restart in 1999; at the root of these developments is the modern theory of polarization, developed in the early 1990s, and based on a geometrical concept (Berry phase). Since insulators and metals polarize in a qualitatively different way, quantum geometry also discriminates insulators from conductors. A common geometrical “marker”, based on the quantum metric, caracterizes all insulators (band insulators, Anderson insulators, Mott insulators, quantum Hall insulators. . . ); such marker diverges in conductors.
condensed mattermathematical physics
Audience: researchers in the topic
( video )
Quantum Matter meets Maths (IST, Lisbon)
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