Static structure factor and the dispersion of the Girvin-MacDonald-Platzman density mode for fractional quantum Hall fluids on the Haldane sphere

TL;DR

This paper calculates the dispersion of neutral excitations in fractional quantum Hall fluids on the Haldane sphere, extending previous plane-based results and deriving the algebra for sphere geometry.

Contribution

It derives the Girvin-MacDonald-Platzman algebra for the Haldane sphere and computes the density-mode dispersion for various FQH states in this geometry.

Findings

GMP mode accurately describes primary Jain states at long wavelengths on the sphere.

Derived the algebra for LLL-projected density operators on the Haldane sphere.

Extended previous plane-based calculations to spherical geometry.

Abstract

We study the neutral excitations in the bulk of the fractional quantum Hall (FQH) fluids generated by acting with the Girvin-MacDonald-Platzman (GMP) density operator on the uniform ground state. Creating these density modulations atop the ground state costs energy, since any density fluctuation in the FQH system has a gap stemming from underlying interparticle interactions. We calculate the GMP density-mode dispersion for many bosonic and fermionic FQH states on the Haldane sphere using the ground state static structure factor computed on the same geometry. Previously, this computation was carried out on the plane. Analogous to the GMP algebra of the lowest Landau level (LLL) projected density operators in the plane, we derive the algebra for the LLL-projected density operators on the sphere, which facilitates the computation of the density-mode dispersion. Contrary to previous results on the plane, we find that, in the long-wavelength limit, the GMP mode accurately describes the dynamics of the primary Jain states.