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Metal-insulator transition in a boundary three chain model
Phys. Rev. B 113, 035156 – Published 29 January, 2026
DOI: https://doi.org/10.1103/rq6s-z87r
Abstract
We study the boundary physics of topologially trivial Mott insulators, representing the boundary by three coupled Hubbard chains in a linear confining potential. In the Hartree-Fock approximation, the ground state at and slightly off the particle-hole symmetric point remains insulating even at large slopes of the confining potential. By contrast, accounting for quantum fluctuations and correlations through a combination of bosonization and renormalization group (RG) methods, we find that there is always a gapless dipole mode, but it does not contribute to a finite compressibility. Moreover, when increasing the slope of the confining potential at half filling, we find a quantum phase transition between an insulating and a metallic state, indicating the formation of a soft edge state of non-topological origin. Away from half filling, a similar transition takes place.
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