Hilbert-Glass Transition: New Universality of Temperature-Tuned Many-Body Dynamical Quantum Criticality
By D. Pekker, G. Refael, E. Altman, E. Demler, V. Oganesyan. 2013
184 citations recorded by the source corpus.
Conventional phase transitions are usually characterized by a change in a fundamental thermodynamic observable, e.g., in density when liquid changes to vapor. A theoretical study of a one-dimensional disordered quantum spin chain reveals a new class of quantum phase transitions that leave no such signatures and pins down their origin.
Subfields: Atomic and Molecular Physics, and Optics, Condensed Matter Physics, Statistical and Nonlinear Physics
View Paper: https://www.semanticscholar.org/paper/c7be3819d07465f5fb6583f06ede5890d448c52a
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In Atomic and Molecular Physics, and Optics
In Condensed Matter Physics
In Statistical and Nonlinear Physics
Citations in the corpus
- Local integrals of motion in many‐body localized systems (2016, methodology): “Moreover, it allows to access to the dynamical properties in the MBL phase adapting computational approaches originally designed for the ground-state physics, such as the strong disorder renormalization group exploited in [82] to construct approximate many-body eigenstates, and in [101, 102] to desc”
- Ergodicity breaking transition in finite disordered spin chains (2020, background): “This scenario predicts an eigenstate quantum phase transition from an ergodic to a nonergodic phase [36–39], the latter named many-body localization (MBL) [40–44].”
- Pre-thermal phases of matter protected by time-translation symmetry (2016, background): “43 we introduced a formal definition of time-translation symmetry-breaking in MBL systems in terms of eigenstates (two equivalent formulations of which we called TTSB-1 and TTSB-2.)”
- Avalanches and many-body resonances in many-body localized systems (2021, background): “[14] David Pekker, Gil Refael, Ehud Altman, Eugene Demler, and Vadim Oganesyan, “Hilbert-glass transition: New universality of temperature-tuned many-body dynamical quantum criticality,” Phys.”
- Random Quantum Circuits (2022, background): “This example is reminiscent of a ground state phase transition from a paramagnet to a symmetry-broken ferromagnet, although a closer analogy may be the eigenstate phase transition between spin-glass ordered and paramagnetic states in many-body localized systems (265, 266).”
- Colloquium : Many-body localization, thermalization, and entanglement (2018, methodology): “excited states (RSRG-X) uses an approximate succession of local unitary transformations to construct eigenstates of the system at all energies (Pekker et al., 2014).”
- Low-frequency conductivity in many-body localized systems (2015, background): “It is not presently clear whether or not the stretched-exponential effective interactions that occur at putative critical points within the MBL phase [9,14,20,21] substantially modify the above story.”
- Gapless Symmetry-Protected Topological Order (2017, background): “[86] David Pekker, Gil Refael, Ehud Altman, Eugene Dem-”
- Integrals of motion in the many-body localized phase (2014, background): “Many-body localization opens the interesting possibilities of protection of topological order at finite temperature or of phase transitions below the equilibrium lower critical dimension [18, 19, 20, 21, 22, 23]).”
- Operator Spreading and the Emergence of Dissipative Hydrodynamics under Unitary Evolution with Conservation Laws (2017, background): “On the theory side, research in the field of many-body localization (MBL) [4–9] has revealed the existence of classes of generically interacting systems that do not obey quantum statistical mechanics, and understanding the nature of different MBL phases [10,11] and the transition(s) between MBL and ”