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Absence of small magic angles for disordered tunneling potentials in twisted bilayer graphene

Simon Becker, Izak Oltman, Martin Vogel

Abstract

We consider small random perturbations of the standard high-symmetry tunneling potentials in the Bistritzer-MacDonald Hamiltonian describing twisted bilayer graphene. Using methods developed by Sjöstrand for studying the spectral asymptotics of non-selfadjoint pseudo-differential operators, we prove that for sufficiently small twisting angles the Hamiltonian will not exhibit a flat band with overwhelming probability, and hence the absence of the so-called \textit{magic angels}. Moreover, we prove a probabilistic Weyl law for the eigenvalues of the non-selfadjoint tunneling operator, subject to small random perturbations, of the Bistritzer-MacDonald Hamiltonian in the chiral limit.

Absence of small magic angles for disordered tunneling potentials in twisted bilayer graphene

Abstract

We consider small random perturbations of the standard high-symmetry tunneling potentials in the Bistritzer-MacDonald Hamiltonian describing twisted bilayer graphene. Using methods developed by Sjöstrand for studying the spectral asymptotics of non-selfadjoint pseudo-differential operators, we prove that for sufficiently small twisting angles the Hamiltonian will not exhibit a flat band with overwhelming probability, and hence the absence of the so-called \textit{magic angels}. Moreover, we prove a probabilistic Weyl law for the eigenvalues of the non-selfadjoint tunneling operator, subject to small random perturbations, of the Bistritzer-MacDonald Hamiltonian in the chiral limit.
Paper Structure (23 sections, 21 theorems, 262 equations, 1 figure)

This paper contains 23 sections, 21 theorems, 262 equations, 1 figure.

Key Result

Theorem 2.2

Let $0 < \varepsilon < \exp( -C_1 h^{-2} \varepsilon_0(h))$, $C_1>1$ sufficiently large, let $N=N(\tau_0^2)$, and let with $C>0$ large enough. Then, for $h>0$ small enough

Figures (1)

  • Figure 1: Top left: Away from magic angles $h$, $\operatorname{Spec}(D_h)=h\Gamma^*$ with two-fold multiplicity. Top right: Spectrum of randomly perturbed operator $D_h$ away from magic angles $h$. Bottom left: Spectrum of $D_h$ numerically computed at largest magic angle $h$. In reality the spectrum is the entire complex plane. Bottom right: Spectrum of random perturbation of $D_h$ for $h$ the largest magic angle.

Theorems & Definitions (31)

  • Remark 2.1
  • Theorem 2.2
  • Corollary 2.3
  • Theorem 2.4
  • Theorem 2.5
  • Remark 3.1
  • Proposition 4.1
  • Proposition 4.2
  • Proposition 4.3
  • proof
  • ...and 21 more