Exact ground state of interacting electrons in magic angle graphene

Fuente: arXiv
Saved in:
Bibliographic Details
Main Authors: Becker, Simon, Lin, Lin, Stubbs, Kevin D.
Format: Preprint
Published: 2023
Subjects:
Online Access:
Tags: Add Tag
No Tags, Be the first to tag this record!
_version_ 1866909627567833088
author Becker, Simon
Lin, Lin
Stubbs, Kevin D.
author_facet Becker, Simon
Lin, Lin
Stubbs, Kevin D.
contents One of the most remarkable theoretical findings in magic angle twisted bilayer graphene (TBG) is the emergence of ferromagnetic Slater determinants as exact ground states for the interacting Hamiltonian at the chiral limit. This discovery provides an explanation for the correlated insulating phase which has been experimentally observed at half filling. This work is the first mathematical study of interacting models in magic angle graphene systems. These include not only TBG but also TBG-like systems featuring four flat bands per valley, and twisted trilayer graphene (TTG) systems with equal twist angles. We identify symmetries of the Bistritzer-MacDonald Hamiltonian that are responsible for characterizing the Hartree-Fock ground states as zero energy many-body ground states. Furthermore, for a general class of Hamiltonian, we establish criteria that the ferromagnetic Slater determinants are the unique ground states within the class of uniformly half-filled, translation invariant Slater determinants. We then demonstrate that these criteria can be explicitly verified for TBG and TBG-like systems at the chiral limit, using properties of Jacobi-$θ$ and Weierstrass-$\wp$ functions.
format Preprint
id arxiv_https___arxiv_org_abs_2312_15314
institution arXiv
publishDate 2023
record_format arxiv
spellingShingle Exact ground state of interacting electrons in magic angle graphene
Becker, Simon
Lin, Lin
Stubbs, Kevin D.
Mathematical Physics
Mesoscale and Nanoscale Physics
Strongly Correlated Electrons
One of the most remarkable theoretical findings in magic angle twisted bilayer graphene (TBG) is the emergence of ferromagnetic Slater determinants as exact ground states for the interacting Hamiltonian at the chiral limit. This discovery provides an explanation for the correlated insulating phase which has been experimentally observed at half filling. This work is the first mathematical study of interacting models in magic angle graphene systems. These include not only TBG but also TBG-like systems featuring four flat bands per valley, and twisted trilayer graphene (TTG) systems with equal twist angles. We identify symmetries of the Bistritzer-MacDonald Hamiltonian that are responsible for characterizing the Hartree-Fock ground states as zero energy many-body ground states. Furthermore, for a general class of Hamiltonian, we establish criteria that the ferromagnetic Slater determinants are the unique ground states within the class of uniformly half-filled, translation invariant Slater determinants. We then demonstrate that these criteria can be explicitly verified for TBG and TBG-like systems at the chiral limit, using properties of Jacobi-$θ$ and Weierstrass-$\wp$ functions.
title Exact ground state of interacting electrons in magic angle graphene
topic Mathematical Physics
Mesoscale and Nanoscale Physics
Strongly Correlated Electrons
url https://arxiv.org/abs/2312.15314