Abstract

Exploring the quantum geometric properties of solids beyond their topological aspects has become a key focus in current solid-state physics research. We derive the geometric formula for optical conductivity from the quantum metric tensor, applicable to the low-energy regime. This general formulation also depends on the detailed shape of the band dispersion in addition to the geometric properties of the Bloch wave function. We demonstrate, however, that for quadratic band-touching (QBT) semimetals, the optical conductivity simplifies to σ = (e2/8ℏ)d2max when the light frequency exceeds a critical threshold, where dmax represents the maximum Hilbert-Schmidt quantum distance around the band-crossing point. This result indicates that the optical conductivity of QBT semimetals is universal and determined entirely by quantum geometry, independent of other details of the band structure. Furthermore, under time-reversal and rotational symmetries, dmax is restricted to discrete values of 0 or 1, leading to a quantized universal optical conductivity. Through first-principles calculations, we show that our findings are applicable to real materials, including bilayer graphene, Pd₃P₂S8, and other realistic material candidates. Our work underscores the critical role of quantum geometry in governing optical properties, which can be probed through standard optical methods.

Abstract

Exploring the quantum geometric properties of solids beyond their topological aspects has become a key focus in current solid-state physics research. We derive the geometric formula for optical conductivity from the quantum metric tensor, applicable to the low-energy regime. This general formulation also depends on the detailed shape of the band dispersion in addition to the geometric properties of the Bloch wave function. We demonstrate, however, that for quadratic band-touching (QBT) semimetals, the optical conductivity simplifies to σ = (e2/8ℏ)d2max when the light frequency exceeds a critical threshold, where dmax represents the maximum Hilbert-Schmidt quantum distance around the band-crossing point. This result indicates that the optical conductivity of QBT semimetals is universal and determined entirely by quantum geometry, independent of other details of the band structure. Furthermore, under time-reversal and rotational symmetries, dmax is restricted to discrete values of 0 or 1, leading to a quantized universal optical conductivity. Through first-principles calculations, we show that our findings are applicable to real materials, including bilayer graphene, Pd₃P₂S8, and other realistic material candidates. Our work underscores the critical role of quantum geometry in governing optical properties, which can be probed through standard optical methods.

Abstract

Exploring the quantum geometric properties of solids beyond their topological aspects has become a key focus in current solid-state physics research. We derive the geometric formula for optical conductivity from the quantum metric tensor, applicable to the low-energy regime. This general formulation also depends on the detailed shape of the band dispersion in addition to the geometric properties of the Bloch wave function. We demonstrate, however, that for quadratic band-touching (QBT) semimetals, the optical conductivity simplifies to σ = (e2/8ℏ)d2max when the light frequency exceeds a critical threshold, where dmax represents the maximum Hilbert-Schmidt quantum distance around the band-crossing point. This result indicates that the optical conductivity of QBT semimetals is universal and determined entirely by quantum geometry, independent of other details of the band structure. Furthermore, under time-reversal and rotational symmetries, dmax is restricted to discrete values of 0 or 1, leading to a quantized universal optical conductivity. Through first-principles calculations, we show that our findings are applicable to real materials, including bilayer graphene, Pd₃P₂S8, and other realistic material candidates. Our work underscores the critical role of quantum geometry in governing optical properties, which can be probed through standard optical methods.

Abstract

Exploring the quantum geometric properties of solids beyond their topological aspects has become a key focus in current solid-state physics research. We derive the geometric formula for optical conductivity from the quantum metric tensor, applicable to the low-energy regime. This general formulation also depends on the detailed shape of the band dispersion in addition to the geometric properties of the Bloch wave function. We demonstrate, however, that for quadratic band-touching (QBT) semimetals, the optical conductivity simplifies to σ = (e2/8ℏ)d2max when the light frequency exceeds a critical threshold, where dmax represents the maximum Hilbert-Schmidt quantum distance around the band-crossing point. This result indicates that the optical conductivity of QBT semimetals is universal and determined entirely by quantum geometry, independent of other details of the band structure. Furthermore, under time-reversal and rotational symmetries, dmax is restricted to discrete values of 0 or 1, leading to a quantized universal optical conductivity. Through first-principles calculations, we show that our findings are applicable to real materials, including bilayer graphene, Pd₃P₂S8, and other realistic material candidates. Our work underscores the critical role of quantum geometry in governing optical properties, which can be probed through standard optical methods.