Berry curvature and quantum metric in copper-substituted lead phosphate apatite

TL;DR

This study investigates the quantum geometrical properties of copper-substituted lead phosphate apatite, revealing highly anisotropic Berry curvature and quantum metric that could influence magnetism and flat band superconductivity mechanisms.

Contribution

It introduces a tight-binding model analysis of the material's quantum geometry, highlighting anisotropic Berry curvature and quantum metric in the normal state.

Findings

Berry curvature pattern remains unchanged along out-of-plane momentum

Net orbital magnetization from Berry curvature is zero

Quantum metric components suggest anisotropic superfluid stiffness

Abstract

The recent discovery of copper-substituted lead phosphate apatite, also known as LK-99, has caught much attention owing to certain experimental evidence of room-temperature superconductivity, although this claim is currently under intensive debate. Be it superconducting or not, we show that the normal state of this material has peculiar quantum geometrical properties that may be related to the magnetism and the mechanism for flat band superconductivity. Based on a recently proposed spinless two-band tight-binding model for the Pb-Cu hexagonal lattice subset of the crystalline structure, which qualitatively captures the two flat bands in the band structure, we elaborate the highly anisotropic Berry curvature and quantum metric in the regions of Brillouin zone where one flat band is above and the other below the Fermi surface. In these regions, the Berry curvature has a pattern in the planar momentum that remains unchanged along the out-of-plane momentum. Moreover, the net orbital magnetization contributed from the Berry curvature is zero, signifying that the magnetism in this material should come from other sources. The quantum metric has a similar momentum dependence, and its two planar components are found to be roughly the same but the out-of-plane component vanishes, hinting that the superfluid stiffness of the flat band superconductivity, shall it occur, may be quite anisotropic.