Magnetic Interactions of Wigner Crystal in Magnetic Field and Berry Curvature: Multi-Particle Tunneling through Complex Trajectories

Abstract

We study how an out-of-plane magnetic field $B({\bf r})$ and a Berry curvature $Ω({\bf k})$ modify the exchange interactions in a two-dimensional Wigner crystal (WC) using a semi-classical large-$r_s$ expansion. When only a magnetic field is present, ring-exchange processes arise from multi-particle tunneling through {\it complex} trajectories which constitute {\it complex instanton} solutions of the coordinate-space path integral. To leading order in $B$, each exchange constant $J_a$ acquires an Aharonov-Bohm phase along the zero-field tunneling trajectory. When a Berry curvature is present, the multi-particle tunneling must be considered in a complexified phase space $({\bf r}, {\bf k})$. To leading order in $Ω$, $J_a$ acquires a Berry phase along a {\it purely imaginary} momentum-space trajectory. When $B$ and $Ω$ are both present, in addition to having both Aharonov-Bohm and Berry phases, the exchange magnitude $|J_a|$ is also modified due to an effective-mass renormalization. These effects could be relevant for the WC and proximate phases recently observed in rhombohedral multilayer graphene.

Figures (1)

• Figure 1: Exchange magnitude $J_a^{(0)}$ [see \ref{['eq:exchange-constant-introduction']} and Table \ref{['table:results']}] normalized by the largest one $J_3^{(0)}$ as a function of $r_s$ ($15 \leq r_s \leq 80$).