2012/11/29 by Chih-Chun Chien, Massimiliano Di Ventra
Physics and Astronomy · #Boson #Cold Atom Physics and Bose-Einstein Condensates #Condensed matter physics #Fermion #Lattice (music) #Observable #Optical lattice #Physics #Quantum #Quantum entanglement #Quantum many-body systems #Quantum mechanics #Quantum tunnelling #Quantum, superfluid, helium dynamics #Superfluidity #Ultracold atom #cond-mat.mes-hall #cond-mat.quant-gas #quant-ph
paper · pdf · doi:10.1103/physreva.87.023609
published as Phys. Rev. A 87, 023609 (2013) · 5 pages, 3 figures
arxiv created 2012/11/29 · openalex publication_date 2013/02/08 · arxiv updated 2013/02/12 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
We show that the recently developed optical lattices with Peierls substitution---which can be modeled as a lattice with a complex tunneling coefficient---may be used to induce controllable quantum transport of ultracold atoms. In particular, we show that by ramping up the phase of the complex tunneling coefficient in a spatially uniform fashion, a finite quasi-steady-state current (QSSC) ensues from the exact dynamics of noninteracting fermions. The direction and magnitude of the current can be controlled by the overall phase difference but not the details of the ramp. The entanglement entropy does not increase when the QSSC lasts. Due to different spin statistics, condensed noninteracting bosons do not support a finite QSSC under the same setup. We also find that an approximate form of the QSSC survives when perturbative effects from interactions, weak harmonic background traps, and finite temperature are present, which suggests that our findings should be observable with available experimental capabilities.