Exact solution for infinitely strongly interacting Fermi gases in tight waveguides

Physics – Condensed Matter – Strongly Correlated Electrons

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4 pages, 3 figures, version accepted for publication in Phys. Rev. Lett

Scientific paper

10.1103/PhysRevLett.102.160402

We present an exact analytical solution of the fundamental systems of quasi-one-dimensional spin-1/2 fermions with infinite repulsion for arbitrary confining potential. The eigenfunctions are constructed by the combination of Gireardeau's hard-core contacting boundary condition and group theoretical method which guarantees the obtained states to be simultaneously the eigenstates of $S$ and $S_z$ and fulfill the antisymmetry under odd permutation. We show that the total ground-state density profile behaves like the polarized noninteracting fermions, whereas the spin-dependent densities display different properties for different spin configurations. We also discuss the splitting of the ground states for large but finite repulsion.

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