Abstract

We study tunneling of weakly interacting spinless electrons at zero temperature through a single δ barrier in one-dimensional wires and rings of finite lengths. Our numerical calculations are based on the self-consistent Hartree–Fock approximation, nevertheless, our results exhibit features known from correlated many-body models. In particular, the transmission in a wire of length L at the Fermi level is proportional to L - 2 α with the universal power α (depending on the electron–electron interaction only, not on the strength of the δ barrier). Similarly, the persistent current in a ring of the circumference L obeys the rule I ∝ L - 1 - α known from the Luttinger liquid and Hubbard models. We show that the transmission at the Fermi level in the wire is related to the persistent current in the ring at the magnetic flux h / 4 e .

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