2008/04/30 by Erhai Zhao, W. Vincent Liu · 84 citations
Physics and Astronomy · #Ansatz #Cold Atom Physics and Bose-Einstein Condensates #Condensed matter physics #Fermi Gamma-ray Space Telescope #Fermi gas #Fermi liquid theory #Instability #Luttinger liquid #Pairing #Phase (matter) #Phase diagram #Physics #Physics of Superconductivity and Magnetism #Quantum #Quantum mechanics #Quantum tunnelling #Quantum, superfluid, helium dynamics #Renormalization group #Scaling #Spin (aerodynamics) #Superconductivity #Superfluidity #cond-mat.other #cond-mat.supr-con
paper · pdf · doi:10.1103/physreva.78.063605
published in Physical Review A 78(6) (American Physical Society) · new expanded version, 8 pages, updated references
arxiv created 2008/11/18 · openalex publication_date 2008/12/05 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
We present a theory for a lattice array of weakly coupled one-dimensional ultracold attractive Fermi gases (1D tubes) with spin imbalance, where strong intratube quantum fluctuations invalidate mean-field theory. We first construct an effective field theory, which treats spin-charge mixing exactly, based on the Bethe ansatz solution of the 1D single tube problem. We show that the 1D Fulde-Ferrel-Larkin-Ovchinnikov (FFLO) state is a two-component Luttinger liquid, and its elementary excitations are fractional states carrying both charge and spin. We analyze the instability of the 1D FFLO state against intertube tunneling by renormalization group analysis, and find that it flows into either a polarized Fermi liquid or a FFLO superfluid, depending on the magnitude of interaction strength and spin imbalance. We obtain the phase diagram of the quasi-1D system and further determine the scaling of the superfluid transition temperature with intertube coupling.