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Finite-temperature spin and charge transport in integrable one-dimensional Mott-Hubbard insulators
J M P Carmelo1,2, P D Sacramento2
1Center of Physics of University of Minho and University of Porto, LaPMET, Oporto P-4169-007, Portugal.
The one-dimensional Hubbard model exhibits normal diffusive charge transport at all temperatures, contrary to previous anomalous superdiffusive predictions. This correction arises from accounting for U(1) symmetry beyond the assumed SO(4) symmetry at the h=μ=0 point.
Area of Science:
- Condensed Matter Physics
- Quantum Mechanics
- Statistical Mechanics
Background:
- The one-dimensional (1D) Hubbard model is a key system for understanding Mott-Hubbard insulators.
- Previous studies suggested anomalous superdiffusive spin and charge transport at T>0 for the 1D Hubbard model at h=μ=0.
- These predictions relied on hydrodynamic theory and Kardar-Parisi-Zhang (KPZ) scaling.
Purpose of the Study:
- To review recent findings that correct the understanding of charge transport in the 1D Hubbard model.
- To address the discrepancy between hydrodynamic theory/KPZ scaling predictions and actual behavior.
- To identify the source of the failure in previous theoretical models.
Main Methods:
- Review of recent theoretical results.
- Analysis of symmetry properties at the h=μ=0 point.
- Comparison of hydrodynamic theory and KPZ scaling with corrected models.
Main Results:
- Finite-temperature charge transport in the 1D Hubbard model at h=μ=0 is normal diffusive, not anomalous superdiffusive.
- The previous theoretical failure stemmed from incorrectly assuming an SO(4) symmetry.
- The correct analysis must include the quantum effects of the τ-translational U(1) symmetry beyond SO(4).
Conclusions:
- Hydrodynamic theory and KPZ scaling predictions for charge transport are inaccurate for the 1D Hubbard model at the h=μ=0 point.
- The correct description of transport requires acknowledging the full [SO(4)×U(1)]/Z2 symmetry.
- This work highlights the importance of subtle symmetry considerations in strongly correlated electron systems.
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