arXiv subjects

Shengxuan Xia

Publications and source records attributed to Shengxuan Xia.

3 recordsLinked to original sources

arXiv2026

Tunable high-$Q$ Janus-to-chiral bound states in the continuum in bilayer PhCs

We propose a bilayer all-dielectric PhC for controlling Janus bound states in the continuum (BIC) and optical chirality through symmetry-selective perturbations. Starting from a symmetry-protected $Γ$-point BIC, we use interlayer displacement as one geometric control knob to generate different topological charges in the upward radiation and downward radiation channels. A subsequent diagonal in-plane displacement reconstructs the polarization topology around the BIC and generates a Janus-chiral BIC with strong handedness selectivity. In contrast, other in-plane perturbations generate chiral quasi-BICs with finite radiative coupling, for which the circular dichroism (CD) and resonance wavelength can be continuously tuned. We further show that material conductivity provides an additional dissipative degree of freedom for actively modulating the chiral response, with a switchable CD exceeding 0.89. Near-field optical-chirality distributions and multipole decompositions reveal that the chiral response originates from a symmetry-induced imbalance of local optical handedness and a spin-selective magnetic-dipole resonance. These results reveal the topological relationship between Janus radiation, polarization singularities and intrinsic chirality, thus paving a scalable route toward reconfigurable high-$Q$ chiral photonics.

physics.optics↗

arXiv2025

Janus bound states in the continuum in structurally symmetric photonic crystals

We propose a sigma_z-symmetry-preserving approach to achieve Janus bound states in the continuum (Janus BICs) exhibiting asymmetric topological charges in the upward and downward radiation channels. While prior approaches typically involve explicit structural perturbations to break vertical symmetry, our design leverages a bilayer photonic crystal slab (PCS) system with independently tunable refractive indices, introducing an optical asymmetry without altering the geometric symmetry. In the optical symmetry case, the system supports symmetry-protected BICs at Gamma point with topological charge q = -1, and Friedrich-Wintgen BICs (FW-BICs) at off-Gamma point with q = +1. Upon introducing refractive index detuning, the polarization vortex splits into two circularly polarized states (C points) with half-integer topological charge (q = 1/2), shifting oppositely in momentum space for upward and downward radiation, while the symmetry-protected BICs remain unaffected. Janus BICs are established through the shift of upward-radiating C points shift towards the Gamma point, accumulating a total topological charge of q = -1, while the downward-radiating counterpart contributes q = +1, leading to a net topological charge reversal between the two radiation channels. This purely optical mechanism allows for the realization of Janus BICs without any structural deformation. Their asymmetric topological nature makes them ideally suited for applications in unidirectional light sources, chiral photonic interfaces, and topological photonic circuits, offering a promising platform for on-chip optical communication, sensing, and quantum information processing.

physics.optics↗

arXiv2020

Graphene plasmon-phonon coupled modes at the exceptional point

Properties of graphene plasmons are greatly affected by their coupling to phonons. While such coupling has been routinely observed in both near-field and far-field graphene spectroscopy, the interplay between coupling strength and mode losses, and its exceptional point physics has not been discussed. By applying a non-Hermitian framework, we identify the transition point between strong and weak coupling as the exceptional point. Enhanced sensitivity to perturbations near the exceptional point is observed by varying the coupling strength and through gate modulation of the graphene Fermi level. Finally, we also show that the transition from strong to weak coupling is observable by changing the incident angle of radiation.

cond-mat.mes-hall↗