Principle of Maximum Entanglement Entropy and Local Physics of Correlated many-body Electron-Systems
arXiv:1310.7520 · doi:10.1103/PhysRevLett.113.036402
Abstract
We argue that, because of the quantum-entanglement, the local physics of the strongly-correlated materials at zero temperature is described in very good approximation by a simple generalized Gibbs distribution, which depends on a relatively small number local quantum thermodynamical potentials. We demonstrate that our statement is exact in certain limits, and we perform numerical calculations of the iron compounds FeSe and FeTe and of the elemental cerium by employing the Gutzwiller Approximation (GA) that strongly support our theory in general.
Manuscript: 5 pages, 3 figures. Supplemental material: 1 page, 1 figure
References in corpus (9)
- Quantum ESPRESSO: a modular and open-source software project for quantum simulations of materials
- Thermalization and its mechanism for generic isolated quantum systems
- Quantum Quench in the Transverse Field Ising Chain
- Ballistic spreading of entanglement in a diffusive nonintegrable system
- The Luttinger model following a sudden interaction switch-on
- Aspects of generic entanglement
- What is the valence of a correlated solid? The double life of delta-plutonium
- Statistical distribution of quantum entanglement for a random bipartite state
- The - iso-structural Transition in Cerium, a Critical Element
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