Giant transparent chirality and Kerr optical bistability via polarization-conversion quasi-BICs
High-performance chiral optical devices capable of active all-optical modulation are indispensable for the emerging quantum information processing and spin-encoded photonic logic. However, realizing such devices is constrained by back-scattering noise and the fundamental trade-off between optical chirality and quality (Q) factors inherent in traditional metasurfaces. Here, we overcome these limitations by demonstrating a rationally engineered silicon metasurface that supports high-Q quasi-bound states in the continuum (q-BIC) featuring near-unity transparent chirality. We simultaneously achieve giant transparent chirality (CD co ≈ 1.00 and CD cross ≈ −1.00) and a high Q-factor (Q ≈ 6.7 × 10 5 ) by leveraging an efficient polarization-conversion mechanism. Furthermore, we demonstrate low-threshold (I on ≈ 1.5 kW/cm 2 ) and high-modulation-depth (ΔT ≈ 80%) Kerr optical bistability in the telecommunication C-band (~1551 nm) based on the high-Q chiral q-BIC resonance. These bistable chiroptical responses enable reconfigurable spin-encoded logic gates and an all-optical spin latch exhibiting near-unity modulation contrast (𝛥CD co ≈ 0.97). This work establishes a novel platform for generating high-Q resonances with giant, lossless transparent chirality, offering a new paradigm for low-threshold, high-contrast all-optical quantum photonic devices.
Authors
- Zenghui Chen (ORCID: https://orcid.org/0000-0002-1881-8180)
- Pingan Chen (ORCID: https://orcid.org/0000-0001-8138-0639)
- Hengjun Chen (ORCID: https://orcid.org/0000-0002-2487-4277)
- Zelin Li (ORCID: https://orcid.org/0000-0002-3186-1343)
- Xin-lin Wang
- Xiaojun Li
Institutions
- Twitter (United States) (US)
Publication Details
- Journal
- Journal of Nonlinear Optical Physics & Materials
- Published
- 2026-06-26
- DOI
- https://doi.org/10.1142/s0218863526400114
- Primary Topic
- Metamaterials and Metasurfaces Applications
- Type
- article
- Field-Weighted Citation Impact
- 0.00