Search arXiv⌕ Search

arXiv · 2610.33606

Second-Harmonic Bulk Response of Fractional Quantum Hall Fluids

Abstract

We develop a bulk description for the second-harmonic Hall response of fractional quantum Hall fluids with broken inversion and rotational symmetries, distinct from edge theories based on nonlinear edge-mode dispersion. By projecting a tilted massive Dirac model onto a single low-energy band, we construct a composite-boson Chern--Simons theory for the lowest Landau level that retains projection-induced nonlinear electromagnetic couplings. The nonlinear Hall resistivity vanishes in the dc limit, while its finite-frequency response retains the characteristic filling-factor dependence $ρ^{(2)}_{TLL}\proptoν^{-2}$, where $ν$ is the Landau-level filling factor. At low frequency, its real and imaginary parts scale as $(ω/ω_c)^2$ and $ω/ω_c$, respectively, where $ω_c$ is the cyclotron frequency, and the response is strongly anisotropic with respect to the crystalline tilt axis. Notably, the Kohn-mode resonances present in the second-order conductivity cancel in the nonlinear Hall resistivity. These results establish finite-frequency nonlinear transport as a bulk probe of fractional quantum Hall fluids without requiring nonlinear edge-mode dispersion.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

J. Luke Pimlott, Pablo Reiser, T. Hans Hansson, Habib Rostami. 2026-10-24. Second-Harmonic Bulk Response of Fractional Quantum Hall Fluids. https://arxiv.org/abs/2610.33606

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Electrically tunable Crossed Andreev Reflection in Bipolar Magnetic Semiconductors

Crossed Andreev reflection (CAR) is a nonlocal quantum transport phenomenon that arises at the interfaces between a superconductor and two spatially separated metals. In this process, an electron incident from one metal combines with another electron originating from the other metal to form a Cooper pair in the SC. In this work, we theoretically investigate the quantum transport properties of a device comprising a central $s$-wave superconductor sandwiched between two bipolar magnetic semiconductor (BMS) leads. BMS materials possess a unique bandstructure where the conduction and valence bands are fully spin-polarized in opposite directions. By applying independent gate voltages to the two BMS leads, we selectively tune their chemical potentials to configure an antiparallel spin alignment at the Fermi energy. In the absence of spin-orbit coupling (SOC), this specific configuration perfectly suppresses both local Andreev reflection and direct electron tunneling (ET), thereby isolating and profoundly enhancing CAR. The introduction of Rashba SOC, however, induces spin-flip scattering that relaxes these strict selection constraints, yielding finite probabilities for competing scattering channels and subsequently reducing the overall CAR efficiency. Nevertheless, for SOC strengths below a critical threshold, CAR remains the dominant transport mechanism over ET. This proposed architecture provides a scalable, stray-field-free method to achieve purely electrostatic control over nonlocal transport, advancing the development of highly efficient superconducting spintronic devices.

cond-mat.mes-hall↗

Gaussian-Bond Hall Viscosity and Nonlocal Hall Response of a Sampled Landau Level

Hall viscosity on a lattice depends on how strain changes microscopic hopping amplitudes. For a specified Gaussian envelope, bond-length derivatives close on the undeformed hopping, expressing the stress as an embedded momentum Hessian and relating the viscosity to higher-order band geometry. In the Kapit--Mueller parent family at rational flux, we show that the stress response equals the strain curvature of the sampled-LLL Gram matrix. The density-normalized viscosity approaches the continuum value 1/4, with an exponentially small sampling correction at finite flux. By contrast, for a straight-bond Peierls source, a low-frequency mass, and a fixed-envelope susceptibility, the viscosity--conductivity comparison exhibits an algebraic deviation, whose leading coefficient follows from a weak-field expansion.

cond-mat.mes-hall↗

Laser-Induced 90-Degree Magnetization Switching for Single-Element 2D Sensing

Magnetoresistive sensors with multiaxial sensitivity are interesting for field mapping applications where local measurement of multiple magnetic field components is needed. Existing device designs are often discretized with separate sensing elements for each vector component, or they require complex detection schemes to distinguish the different components. In this work, we showcase a single-element two-dimensional vector sensor with on-demand reprogrammable sensing axis using light and optically switchable materials. Our device is an anisotropic magnetoresistive sensor with $90^\circ$ togglable sensitivity upon excitation with ultrashort laser pulses. The sensor consists of an optically switchable Co/Gd thin-film bilayer, patterned into a cross shape that stabilizes two orthogonal in-plane magnetization directions. By selectively addressing one diagonal of the cross, a single laser pulses toggle switches the magnetization direction in the center of the cross by $90^\circ$. Moreover, the field sensitivity of the device is toggled between the $x$- and $y$-axes, which we detected electrically with the planar Hall effect. Our results form a milestone towards optically reprogrammable integrated magnetic vector sensors.

cond-mat.mes-hall↗