The exchange coupling of a Wigner dimer

TL;DR

This paper analytically investigates the exchange coupling in a two-electron one-dimensional Wigner crystal, revealing how the energy splitting depends on electron separation and the effects of a finite potential cutoff.

Contribution

It introduces two methods for calculating the energy splitting in a Wigner dimer, including an exact solution with Whittaker functions and a WKB approximation, enhancing understanding of magnetic properties.

Findings

Energy splitting decays exponentially with electron distance.

Subleading exponential correction significantly affects the splitting.

Methods agree in the overlapping parameter region.

Abstract

We study the exchange coupling in small Wigner crystals confined to one-dimensional space. In particular we concentrate on the simplest nontrivial case of two electrons in a box potential and calculate analytically the energy splitting between the lowest spatially symmetric and antisymmetric states, which is a relevant energy scale for the magnetic properties of the system. In the approximation of a fixed center of mass coordinate, the splitting decays exponentially with the square root of the distance between the electrons at the leading order. We show that the subleading exponential correction significantly increases the splitting and thus becomes crucial in order to describe correctly the exact numerical data for system sizes that are not astronomically large. Two methods of calculation of the energy splitting are developed. The first is based on the analysis of the exact solution that can be expressed in terms of the Whittaker functions. It applies at all values of the short-distance cutoff played by the width of one-dimensional wire that regularizes the Coulomb potential. The second method is based on the quasiclassical (or Wentzel-Kramers-Brillouin) approximation, which applies only for sufficiently large values of the cutoff. The two methods give identical result in the overlapping region. As a side result, our study gives the energy splitting in a triangular double well potential of inverse ``M'' shape.