Video URL
https://pirsa.org/15030113Universal Aspects of Many-body Localization Phase Transition and Eigenstate Thermalization
APA
Grover, T. (2015). Universal Aspects of Many-body Localization Phase Transition and Eigenstate Thermalization. Perimeter Institute for Theoretical Physics. https://pirsa.org/15030113
MLA
Grover, Tarun. Universal Aspects of Many-body Localization Phase Transition and Eigenstate Thermalization. Perimeter Institute for Theoretical Physics, Mar. 10, 2015, https://pirsa.org/15030113
BibTex
@misc{ scivideos_PIRSA:15030113, doi = {10.48660/15030113}, url = {https://pirsa.org/15030113}, author = {Grover, Tarun}, keywords = {Quantum Matter}, language = {en}, title = {Universal Aspects of Many-body Localization Phase Transition and Eigenstate Thermalization}, publisher = {Perimeter Institute for Theoretical Physics}, year = {2015}, month = {mar}, note = {PIRSA:15030113 see, \url{https://scivideos.org/index.php/pirsa/15030113}} }
Tarun Grover University of California, San Diego
Abstract
Does a generic quantum system necessarily thermalize? Recent developments in disordered many-body quantum systems have provided crucial insights into this long-standing question. It has been found that sufficiently disordered systems may fail to thermalize leading to a 'many-body localized' phase. In this phase, the fundamental assumption underlying equilibrium statistical mechanics, namely, the equal likelihood for all states at the same energy, breaks down. A fundamental question is: what happens as the disorder becomes weaker so that one approaches the localization-delocalization transition? For example, does the system thermalize *at* the transition?
In this talk, I will show that very general considerations on the scaling of entanglement entropy close to the transition imply that at a continuous many-body localization transition, the system is necessarily ergodic.
Finally, I will present recent results on "eigenstate thermalization", a long standing hypothesis which posits that a single eigenstate hides within itself a thermal ensemble. In particular, I will discuss which class of operators do or do not satisfy eigenstate thermalization.