Search arXiv⌕ Search

arXiv · 2611.00743

Energy-Centroid Trembling near Exceptional Points in Photonic Time Crystals

Abstract

In a photonic time crystal with a modulated Lorentz restoring coefficient, modulation reweights the potential energy of the polarization and loss drains its kinetic energy; when these sectors are offset within a pulse, the energy centroid trembles in every cycle while the Poynting-flux velocity stays bounded. Near the gap-edge exceptional point the mode geometry amplifies these offsets, and for a narrow-band pulse on one passband Floquet branch the trembling-velocity amplitude generically grows as the inverse square root of the momentum detuning, rounded by finite bandwidth. Loss modulated in phase or in antiphase with the restoring coefficient can change the trembling coefficient while the band-slope and Petermann coefficients barely move. In the lossy example studied, a forward field pulse launched with the polarization at rest exhibits delayed bursts near the beat recurrence after substantial energy loss, with monochromatic amplitudes following the inverse three-halves power of the detuning over the computed range. Intracycle energy exchange and preparation thus shape the centroid motion beyond what the band slope and the Floquet Petermann factor determine.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Kyungmin Lee, Younsung Kim, Minwook Kyung, Seungmin Yeon, Bumki Min. 2026-10-31. Energy-Centroid Trembling near Exceptional Points in Photonic Time Crystals. https://arxiv.org/abs/2611.00743

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

KEEP EXPLORING

Related papers

Valley polarization driven by two-color circular fields from a strong-field tunneling perspective

Valley polarization in hexagonal materials driven by the form of the lightwave and its orientation relative to the lattice, rather than solely by the helicity of the driver, has recently been demonstrated both theoretically and experimentally. This has extended valley control to the non-resonant, sub-cycle regime and to inversion-symmetric materials. One interpretation of this field-orientation-dependent valley polarization is that the laser-dressed, cycle-averaged band structure obtained from a Floquet-type approach is modified so as to lift the degeneracy between the valleys. Here, we derive a complementary explanation based on strong-field tunneling dynamics. We show that the effective valley gap at the dominant injection times depends on the orientation of the field relative to the lattice through the trigonal-warping term of the low-energy dispersion. We derive general expressions for co- and counter-rotating $ω+Nω$ fields and show that the leading orientation-dependent contribution survives the cycle average only for field configurations compatible with the threefold lattice symmetry, most notably counter-rotating $ω+2ω$ and co-rotating $ω+4ω$ fields.

physics.optics↗

Advances in the Vacuum Magnetic Birefringence measurement using a pulsed Foil Coil

In this paper, in the framework of the {\it Biréfringence Magnétique du Vide} (BMV) experiment, we present our current apparatus in detail and we discuss its critical points. We also report the results obtained using specially designed pulsed coils called Foil Coils. Our novel measurement of the vacuum linear magnetic birefringence constant is $K_{VMB} < 1.7 \cdot 10^{-21}~\text{T}^{-2}$ at a confidence level of 68$\%$, which is an improvement with respect to our previous 2014 measurement.

physics.optics↗

Asymptotic electromagnetic transition conditions for thin layers: the arithmetic-mean field and susceptibility hybridization

Effective transition conditions that replace a thin polarizable layer by a zero-thickness sheet are commonly applied in electromagnetic models of two-dimensional (2D) materials and metasurfaces. These conditions usually take the arithmetic mean of the fields on either side as the polarizing field at the boundary, and characterize the layer by the $0^\mathrm{th}$ moment of its susceptibility, but both choices are typically imposed rather than derived. We derive transition conditions for a finite-thickness, in-plane homogeneous, in-plane isotropic layer with a general nonlocal susceptibility, using a single-scale asymptotic expansion in $η= l\max(k_0,q)$, where $l$ is the layer thickness, $k_0$ the free-space wavenumber and $q$ the in-plane wavenumber. The sheet limit must be taken after resumming the out-of-plane depolarizing field, as this ensures that the resulting sheet susceptibility is independent of the material thickness. The arithmetic mean then emerges as the leading-order polarizing field for general susceptibility profiles. Asymmetries in the layer profile modify the effective susceptibility appearing in the transition conditions, rather than altering the arithmetic-mean field prescription. If the spatial profile is not even in both out-of-plane coordinates, in-plane and out-of-plane response hybridize, turning the diagonal volumetric susceptibility into a $q$-dependent effective tensor surface susceptibility with off-diagonal components. Mirror symmetry alone does not remove this hybridization. Comparison with exact solutions for local and separable layers shows that the derived conditions remain accurate to $O(η)$ across propagating and evanescent excitations, whereas the standard sheet conditions fail once hybridization becomes appreciable.

physics.optics↗