Burnett coefficients in quantum many-body systems
arXiv:1302.4879 · doi:10.1103/PhysRevE.87.050103
Abstract
The Burnett coefficient B is investigated for transport in one-dimensional quantum many-body systems. Extensive numerical computations in spin-1/2 chains suggest a linear growth with time, B(t) \sim t, for non-integrable chains exhibiting diffusive transport. For integrable spin chains in the metallic regime, on the other hand, we find a cubic growth with time, B(t) \sim -D_m^2 t^3, with the proportionality constant being simply a square of the Drude weight D_m. The results are corroborated with additional studies in non-interacting quantum chains and in the classical limit of large-spin chains.
5 pages, 4 figures
References in corpus (7)
- Open XXZ spin chain: Nonequilibrium steady state and strict bound on ballistic transport
- Spin transport in a one-dimensional anisotropic Heisenberg model
- Thermodyamic bounds on Drude weights in terms of almost-conserved quantities
- Transport in open spin chains: A Monte Carlo wave-function approach
- Decay of currents for strong interactions
- Transition from diffusive to ballistic dynamics for a class of finite quantum models
- Spin transport in the XXZ model at high temperatures: Classical dynamics versus quantum S=1/2 autocorrelations
Cited by in corpus (5)
- Finite-temperature transport in one-dimensional quantum lattice models
- Scaling of diffusion constants in the spin-1/2 XX ladder
- Hydrodynamic gauge fixing and higher order hydrodynamic expansion
- Exponential damping induced by random and realistic perturbations
- Modeling the Impact of Hamiltonian Perturbations on Expectation Value Dynamics