Topological signatures in the curvature-induced energy response
cond-mat.mes-hall
Submitted: 2026-08-28
Updated: 2026-09-23
Comments: 17 pages, 6 figures
License: http://creativecommons.org/licenses/by/4.0/
The gist: Relativistic effective field theory predicts a topological energy response to a gravitational field that appears at third order in spatial gradients.
Terminology
Abstract
Relativistic effective field theory predicts a topological energy response to a gravitational field that appears at third order in spatial gradients. Here, we investigate how this response emerges in the nonrelativistic Haldane model using a microscopic lattice formulation of curvature-induced deformations. We find that the leading first-order energy response is nonuniversal and depends on the bond-resolved structure of the deformation; in particular, it vanishes for a symmetric modulation of the three nearest-neighbor hoppings. At third order, the curvature-induced energy response contains a bond-symmetric component together with nonuniversal bond-dependent contributions. The bond-symmetric component, which is isolated by a uniform modulation of the three hoppings, exhibits a universal discontinuity across the topological transition whose magnitude agrees with the relativistic gravitational Chern--Simons prediction. Thus, although the full curvature-induced energy response generally contains nonuniversal lattice contributions, its third-order response retains a universal topological component beyond the relativistic limit.
Related papers
- Magnon Kerr Effect in a Magnetic Thin Film Strongly Coupled to a Microwave Resonator
- Contrasting - and K-Valley Moir'e Physics in Twisted Monolayer/Bilayer WSe 2
- Spectral density of angular momentum transfer from a swift electron to a large spherical nanoparticle
- Why finite-size non-Hermitian eigenvalues can miss asymptotic eigenstates in topological physics
- Intrinsic Floquet Generation and 1/I Quantum Oscillations in a Sliding Charge-Density Wave
- Cascade of topological phase transitions and revival of topological zero modes in imperfect double helical liquids