Diffusive charge transport in the gapped 1D Hubbard model at all finite temperatures
arXiv:2507.02753 · doi:10.1103/5smb-xkt4
Abstract
Studies relying on hydrodynamic theory and Kardar-Parisi-Zhang (KPZ) scaling have found that in the one-dimensional Hubbard model spin and charge transport are for all temperatures T > 0 anomalous superdiffusive at zero magnetic field, h = 0, and zero chemical potential, μ = 0, respectively. However, this contradicts recent exact results that at very low temperature charge transport rather is normal diffusive. In this Letter we identify the mechanisms that control the different types of temperature dependence of the h = 0 spin and μ = 0 charge transport and find that the latter is normal diffusive for all finite temperatures T > 0, in contrast to the hydrodynamic theory and KPZ scaling predictions.
6 pages, 2 figures plus Supplementary Material
References in corpus (12)
- Kardar-Parisi-Zhang physics in the quantum Heisenberg magnet
- Ballistic transport in the one-dimensional Hubbard model: the hydrodynamic approach
- Ballistic spin transport in a periodically driven integrable quantum system
- Stability of superdiffusion in nearly integrable spin chains
- Spin crossovers and superdiffusion in the one-dimensional Hubbard model
- Absence of Normal Fluctuations in an Integrable Magnet
- Universal Kardar-Parisi-Zhang dynamics in integrable quantum systems
- Non-linear fluctuating hydrodynamics for KPZ scaling in isotropic spin chains
- Kardar-Parisi-Zhang scaling in the Hubbard model
- Temperature dependence of charge transport in the half-filled 1D Hubbard model
- Finite-temperature charge and spin transport in the one-dimensional Hubbard model accounting for its global [SU (2) X SU(2) X U(1)]/Z_2^2$ symmetry
- Tunable surface electron gas and effect of phonons in SrCuO: A first-principles study