Abstract

The so-called minimal models of unconventional superconductivity are lattice models of interacting electrons derived from materials in which electron pairing arises from purely repulsive interactions. Showing unambiguously that a minimal model actually can have a superconducting ground state remains a challenge at nonperturbative interactions. We make a significant step in this direction by computing ground states of the 2D \mbox{U-V} Hubbard model - the minimal model of the quasi-1D superconductors - by parallelized DMRG, which allows for systematic control of any bias and that is sign-problem-free. Using distributed-memory supercomputers and leveraging the advantages of the \mbox{U-V} model, we can treat unprecedented sizes of 2D strips and extrapolate their spin gap both to zero approximation error and the thermodynamic limit. Our results for the spin gap are shown to be compatible with a spin excitation spectrum that is either fully gapped or has zeros only in discrete points, and conversely that a Fermi liquid or magnetically ordered ground state is incompatible with them. Coupled with the enhancement to short-range correlations that we find exclusively in the $d_{xy}$ pairing-channel, this allows us to build an indirect case for the ground state of this model having superconducting order in the full 2D limit, and ruling out the other main possible phases, magnetic orders and Fermi liquids.

Highlights

  • Understanding the impact of interparticle repulsions in fermionic quantum systems remains one of the most challenging problems in physics

  • We make a significant step in this direction by computing ground states of the 2D U-V Hubbard model—the minimal model of the quasi-1D superconductors—by parallelized density matrix renormalization group (DMRG), which allows for systematic control of any bias and that is sign-problem-free

  • Together with the strong enhancement exclusive to the dxy channel of correlations that we find with increasing strip width, our results make the case for SC singlet pairing with dxy order being the dominant component in the ground state of the U-V model at half filling when repulsion is competitive with kinetic energy

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Summary

Introduction

Understanding the impact of interparticle repulsions in fermionic quantum systems remains one of the most challenging problems in physics. The resulting physics is essentially of free particles (the so-called Landau quasiparticles), with interactions mostly leading to a renormalization of some physical parameters such as the mass. This Fermi liquid (FL) approach has seen very broad success and allowed to understand the effects caused by perturbations on top of the Fermi liquid, such as instabilities towards, e.g., a Bardeen-Cooper-Schrieffer (BCS) superconducting (SC) state, a magnetically ordered (MO) state or a charge density wave (CDW) state [1].

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