Abstract

We numerically solve the Hubbard model on the Bethe lattice with finite coordination number $z=3$, and determine its zero-temperature phase diagram. For this purpose, we introduce and develop the `variational uniform tree state' (VUTS) algorithm, a tensor network algorithm which generalizes the variational uniform matrix product state algorithm to tree tensor networks. Our results reveal an antiferromagnetic insulating phase and a paramagnetic metallic phase, separated by a first-order doping-driven metal-insulator transition. We show that the metallic state is a Fermi liquid with coherent quasiparticle excitations for all values of the interaction strength $U$, and we obtain the finite quasiparticle weight $Z$ from the single-particle occupation function of a generalized "momentum" variable. We find that $Z$ decreases with increasing $U$, ultimately saturating to a non-zero, doping-dependent value. Our work demonstrates that tensor-network calculations on tree lattices, and the VUTS algorithm in particular, are a platform for obtaining controlled results for phenomena absent in one dimension, such as Fermi liquids, while avoiding computational difficulties associated with tensor networks in two dimensions. We envision that future studies could observe non-Fermi liquids, interaction-driven metal-insulator transitions, and doped spin liquids using this platform.

Highlights

  • The Hubbard model is a cornerstone of condensed matter physics

  • In the one-dimensional case, the variational uniform MPS (VUMPS) algorithm [55] has been found to be much more efficient than other methods that work in the thermodynamic limit, such as infinite timeevolving block decimation (iTEBD) or earlier infinite density matrix renormalization group (DMRG) algorithms [63,64,65,66], and we find its extension in the form of the variational uniform tree state algorithm (VUTS) algorithm we develop to be very efficient

  • We have introduced a numerical algorithm, VUTS, to study quantum models on the Bethe lattice. We apply it to the Hubbard model for coordination number z = 3, allowing for a two-site unit cell, obtain the T = 0 phase diagram, and study the doping-induced Mott transition

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Summary

INTRODUCTION

The Hubbard model is a cornerstone of condensed matter physics. As a paradigmatic model of strongly correlated electrons [1], it is simple to formulate yet rich in behavior. We demonstrate that the doped metal hosts coherent quasiparticles at all studied values of the interaction strength U , from weak to strong coupling, and determine the behavior of the quasiparticle weight as a function of U This answers in the affirmative the question of whether Fermi-liquid behavior applies as soon as the peculiar kinematic constraints of one dimension are alleviated, and provides a concrete description of a Fermi-liquid ground state with tensor networks. The smooth behavior in χ of the correlation functions and their properties at all distances give a smooth behavior of the occupation function near the Fermi energy, which allows us to reliably extract information about quasiparticle coherence in the metallic phase This demonstrates that our method can be used to reliably study critical phases of matter on the Bethe lattice already at the level of accuracy we achieve here.

VARIATIONAL UNIFORM TREE STATE ALGORITHM
MODEL AND PHASE DIAGRAM
QUASIPARTICLES
Single-particle basis of symmetric states
Quasiparticles in the interacting system
DISCUSSION
Summing the Hamiltonian terms
Fermions
Convergence strategies
Truncation error and run time
Full Text
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