Abstract

Quantum geometry has emerged as a central and ubiquitous concept in quantum sciences, with direct consequences on quantum metrology and many-body quantum physics. In this context, two fundamental geometric quantities are known to play complementary roles:~the Fubini-Study metric, which introduces a notion of distance between quantum states defined over a parameter space, and the Berry curvature associated with Berry-phase effects and topological band structures. In fact, recent studies have revealed direct relations between these two important quantities, suggesting that topological properties can, in special cases, be deduced from the quantum metric. In this work, we establish general and exact relations between the quantum metric and the topological invariants of generic Dirac Hamiltonians. In particular, we demonstrate that topological indices (Chern numbers or winding numbers) are bounded by the quantum volume determined by the quantum metric. Our theoretical framework, which builds on the Clifford algebra of Dirac matrices, is applicable to topological insulators and semimetals of arbitrary spatial dimensions, with or without chiral symmetry. This work clarifies the role of the Fubini-Study metric in topological states of matter, suggesting unexplored topological responses and metrological applications in a broad class of quantum-engineered systems.

Highlights

  • Using the formula in Eq (15), we find that this monopole charge can be obtained from the quantum metric as where the Brillouin zone 4 was replaced by a sphere S4

  • The general relations derived in this work indicate that the topological indices characterizing topological insulators and semimetals are directly connected to the underlying quantum metric, within the framework of Dirac Hamiltonians

  • While this class of systems was originally introduced as toy models in condensed matter physics, they are today realized in a broad class of synthetic systems, including ultracold gases in optical lattices, solid state qubits and photonics devices

Read more

Summary

Gapped systems without chiral symmetry

These results are consistent with the findings of Ref. Where the five matrices Γ 0,1,2,3,4 are 4 × 4 Dirac matrices and where the momenta span a fourdimensional Brillouin zone In this case, the quantum metric identifies a 4-sphere of radius 1 [Eq (7)], and the relevant topological invariant is the second Chern number associated with the doubly-degenerate low-energy band [38]. The quantum metric identifies a 4-sphere of radius 1 [Eq (7)], and the relevant topological invariant is the second Chern number associated with the doubly-degenerate low-energy band [38] We recall that this invariant, which was measured in cold atoms [70, 71], plays a central role in the 4D quantum Hall effect [72, 73].

Gapped systems with chiral symmetry
Gapless Weyl-type systems
Relation to the Cramér-Rao bound and measurement uncertainty
Concluding remarks
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call