Beyond Symmetry: Harnessing Quantum Magnetoelectricity for Novel Light Control
New research delves into the exotic light-matter interactions arising from broken symmetries in quantum materials, opening doors to advanced metamaterials and quantum devices.
![The distributions of [latex]\pi^+ \pi^-[/latex] and [latex]K_S^0 K_S^0[/latex] pairs are modeled with relativistic Breit-Wigner functions to identify resonance peaks, while a smoothly varying function accounts for residual background, effectively distinguishing signal from noise in the data.](https://arxiv.org/html/2601.09777v1/x6.png)


![The system demonstrates how variations in a deformation parameter influence energy distribution-specifically, the real part of the Hawking-Eberhardt function [latex]\text{HEE}[/latex] and quantities [latex]\mathcal{Q}\_{\pm}[/latex]-for both purely timelike intervals and scenarios with non-vanishing chemical potential, suggesting a nuanced relationship between spacetime geometry and energy fluctuations at [latex]t=2[/latex], [latex]\beta=\sqrt{8}\pi[/latex], [latex]\Omega=0[/latex], and [latex]c=12\pi[/latex].](https://arxiv.org/html/2601.10213v1/x4.png)
![Light can induce magnetization through the intrinsic quantum geometry of a material, specifically via the quadrupole density of the quantum metric and a weighted quantum metric term [latex]\partial\left(Gv\right)[/latex], demonstrating a pathway where polarized light directly influences magnetic properties.](https://arxiv.org/html/2601.09637v1/x1.png)
![The study demonstrates how the Zeeman effect, parameterized by [latex] R_s [/latex], modulates Landau levels and their corresponding oscillations, revealing that a strong Zeeman effect ([latex] R_s = -1 [/latex]) can induce a π phase shift in the oscillating conductivity, precisely mirroring the signature of a non-trivial Berry phase ([latex] \beta = 0.5 [/latex]) observed with [latex] R_s = 1 [/latex], under conditions of oscillation frequency [latex] F = 129.5 T [/latex], Fermi energy [latex] E_F = 60 meV [/latex], and effective mass [latex] m^* = 0.25 m_0 [/latex].](https://arxiv.org/html/2601.09560v1/x4.png)
![Simulated annealing reveals that complex spin configurations-including single and double-[latex]QQ[/latex]-spiral and staggered states-emerge from local interactions, with the resulting magnetic order dependent on parameters like temperature [latex]K[/latex], static interaction strength [latex]J_{sta}[/latex], and spiral wavevector [latex]Q_{sp}[/latex], as demonstrated by the variety of observed patterns and the unnormalized superposition [latex]\bm{S}_{i}[/latex] serving as a comparative reference.](https://arxiv.org/html/2601.09267v1/x2.png)