1.Tsinghua Shenzhen International Graduate School, Tsinghua University, Shenzhen 518055, China
2.Department of Electrical and Computer Engineering, National University of Singapore, Singapore 117583, Singapore
3.Institute of Precision Optical Engineering, School of Physics Science and Engineering, Tongji University, Shanghai 200092, China
4.Key Laboratory of Multifunctional Nanomaterials and Smart Systems, Suzhou institute of Nano-Tech and Nano-Bionics (SINANO), Chinese Academy of Sciences (CAS), Suzhou 215123, China
Cheng-Wei Qiu (chengwei.qiu@nus.edu.sg)
Qinghua Song (song.qinghua@sz.tsinghua.edu.cn)
纸质出版日期:2023-4-30,
网络出版日期:2023-3-7,
收稿日期:2022-8-14,
修回日期:2022-12-30,
录用日期:2023-2-1
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Arbitrarily polarized bound states in the continuum with twisted photonic crystal slabs[J]. 光:科学与应用, 2023,12(4):542-550.
Qin, H. Y.et al. Arbitrarily polarized bound states in the continuum with twisted photonic crystal slabs.Light: Science & Applications,12, 542-550 (2023).
Arbitrarily polarized bound states in the continuum with twisted photonic crystal slabs[J]. 光:科学与应用, 2023,12(4):542-550. DOI: 10.1038/s41377-023-01090-w.
Qin, H. Y.et al. Arbitrarily polarized bound states in the continuum with twisted photonic crystal slabs.Light: Science & Applications,12, 542-550 (2023). DOI: 10.1038/s41377-023-01090-w.
Arbitrary polarized vortex beam induced by polarization singularity offers a new platform for both classical optics and quantum entanglement applications. Bound states in the continuum (BICs) have been demonstrated to be associated with topological charge and vortex polarization singularities in momentum space. For conventional symmetric photonic crystal slabs (PhCSs)
BIC is enclosed by linearly polarized far fields with winding angle of 2
π
which is unfavorable for high-capacity and multi-functionality integration-optics applications. Here
we show that by breaking
σ
z
-symmetry of the PhCS
asymmetry in upward and downward directions and arbitrarily polarized BIC can be realized with a bilayer-twisted PhCS. It exhibits elliptical polarization states with constant ellipticity angle at every point in momentum space within the vicinity of BIC. The topological nature of BIC reflects on the orientation angle of polarization state
with a topological charge of 1 for any value of ellipticity angle. Full coverage of Poincaré sphere (i.e.
$$- {{\pi \over 4}} \le \chi \le {{\pi \over 4}}$$
and
$$- {{\pi \over 2}} \le \psi \le {{\pi \over 2}}$$
) and higher-order Poincaré sphere can be realized by tailoring the twist angles. Our findings may open up new avenues for applications in structured light
quantum optics
and twistronics for photons.
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