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Superdiffusion, normal diffusion, and chaos in semiclassical Bose-Hubbard chains
Dragan Marković1,2, Mihailo Čubrović2
1Friedrich-Alexander-Universität Erlangen-Nürnberg, Department of Mathematics, Cauerstr. 11, D-91058 Erlangen, Germany.
The one-dimensional Bose-Hubbard model exhibits early-time superdiffusion, independent of system parameters. This phenomenon, driven by scaling symmetry, transitions to normal diffusion over time.
Area of Science:
- Quantum many-body physics
- Statistical mechanics
- Condensed matter theory
Background:
- The Bose-Hubbard model describes interacting bosons in a lattice.
- Understanding correlation function dynamics is crucial for characterizing quantum systems.
- Semiclassical approximations offer insights into complex quantum behavior.
Purpose of the Study:
- To investigate the evolution of two-point correlation functions in the 1D Bose-Hubbard model.
- To analyze the role of superdiffusion and its dependence on initial conditions and system parameters.
- To explore the transition from superdiffusion to normal diffusion and its relation to nonintegrability and chaos.
Main Methods:
- Utilizing the truncated Wigner approximation (TWA).
- Incorporating quantum jumps as first-order corrections to TWA.
- Analyzing the semiclassical regime of the Bose-Hubbard model.
Main Results:
- Observed strong superdiffusion at early times with universal integer exponents.
- Demonstrated that superdiffusion is insensitive to system parameters and chaos.
- Identified a crossover to normal diffusion at later times, robust under strong nonintegrability.
- Found that strong nonintegrability leads to a homogeneous state, while weak nonintegrability preserves oscillations.
Conclusions:
- The observed superdiffusion is an early-time phenomenon, not related to prethermalization or thermalization.
- Superdiffusion is linked to a specific scaling symmetry of the Bose-Hubbard Hamiltonian.
- System behavior at later times depends on the degree of nonintegrability, with chaos playing a significant role.
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