scholarly journals Many-body localization from a one-particle perspective in the disordered one-dimensional Bose-Hubbard model

2020 ◽  
Vol 101 (6) ◽  
Author(s):  
Miroslav Hopjan ◽  
Fabian Heidrich-Meisner
1991 ◽  
Vol 05 (10) ◽  
pp. 1791-1800 ◽  
Author(s):  
C. Stephen Hellberg ◽  
E. J. Mele

We study a general class of variational wavefunctions for strongly correlated lattice fermions. The wavefunctions considered here automatically satisfy local constraints of no double occupancy and include correlations between opposite spin particles in a very physical way. We calculate the energy and correlation functions for the one dimensional U=∞ Hubbard model, where a comparison with exact results is made. We briefly report on preliminary results for the t-J model.


2020 ◽  
Vol 102 (5) ◽  
Author(s):  
Guo-Qing Zhang ◽  
Dan-Wei Zhang ◽  
Zhi Li ◽  
Z. D. Wang ◽  
Shi-Liang Zhu

AIP Advances ◽  
2020 ◽  
Vol 10 (12) ◽  
pp. 125127
Author(s):  
Václav Janiš ◽  
Antonín Klíč ◽  
Jiawei Yan

2021 ◽  
Vol 12 (1) ◽  
Author(s):  
Naoto Shiraishi ◽  
Keiji Matsumoto

AbstractThe investigation of thermalization in isolated quantum many-body systems has a long history, dating back to the time of developing statistical mechanics. Most quantum many-body systems in nature are considered to thermalize, while some never achieve thermal equilibrium. The central problem is to clarify whether a given system thermalizes, which has been addressed previously, but not resolved. Here, we show that this problem is undecidable. The resulting undecidability even applies when the system is restricted to one-dimensional shift-invariant systems with nearest-neighbour interaction, and the initial state is a fixed product state. We construct a family of Hamiltonians encoding dynamics of a reversible universal Turing machine, where the fate of a relaxation process changes considerably depending on whether the Turing machine halts. Our result indicates that there is no general theorem, algorithm, or systematic procedure determining the presence or absence of thermalization in any given Hamiltonian.


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