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Published on: March 24, 2019
Interaction-Driven Instabilities in the Random-Field XXZ Chain
Jeanne Colbois1, Fabien Alet1, Nicolas Laflorencie1
1<a href="https://ror.org/01w0hda30">Laboratoire de Physique Théorique</a>, <a href="https://ror.org/004raaa70">Université de Toulouse</a>, CNRS, UPS, France.
This study investigates many-body localization (MBL) in Heisenberg spin chains. Researchers found weak interactions cause instability, while strong disorder leads to MBL, with unique spin-correlation behaviors observed.
Area of Science:
- Condensed Matter Physics
- Quantum Mechanics
- Statistical Physics
Background:
- The nature of high-energy behavior in Heisenberg spin chains with random magnetic fields remains debated.
- Understanding many-body localization (MBL) is crucial for quantum systems.
Purpose of the Study:
- To explore the weak interaction limit of Anderson localized (AL) insulators.
- To map the phase diagram of the XXZ model in the disorder-interaction plane.
- To characterize the behavior of spin-spin correlation functions in different regimes.
Main Methods:
- Shift-invert diagonalization was employed.
- The study analyzed the XXZ model in the disorder (h) and interaction (Δ) plane.
- Total magnetization conservation was utilized to analyze correlation functions.
Main Results:
- Below a disorder threshold (h*), weak interactions induce ergodic instability.
- At strong disorder, Anderson localized insulators transition directly to MBL.
- Spin-spin correlation functions exhibit an orientation inversion (ξz > ξx) in the MBL regime.
- Longitudinal correlation length (ξz) indicates ergodic instabilities, increasing with system size near the thermal phase.
Conclusions:
- The study clarifies the transition from Anderson localization to many-body localization.
- A novel indicator for ergodic instabilities, the longitudinal correlation length, was identified.
- The findings contribute to a deeper understanding of quantum phase transitions in disordered spin systems.
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