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Exceptional points in lossy media lead to deep polynomial wave penetration with spatially uniform power loss

Abstract

Waves entering a spatially uniform lossy medium typically undergo exponential intensity decay, arising from either the energy loss of the Beer–Lambert–Bouguer transmission law or the evanescent penetration during reflection. Recently, exceptional point singularities in non-Hermitian systems have been linked to unconventional wave propagation. Here, we theoretically propose and experimentally demonstrate exponential decay free wave propagation in a purely lossy medium. We observe up to 400-wave deep polynomial wave propagation accompanied by a uniformly distributed energy loss across a nanostructured photonic slab waveguide with exceptional points. We use coupled-mode theory and fully vectorial electromagnetic simulations to predict deep wave penetration manifesting spatially constant radiation losses through the entire structured waveguide region regardless of its length. The uncovered exponential decay free wave phenomenon is universal and holds true across all domains supporting physical waves, finding immediate applications for generating large, uniform and surface-normal free-space plane waves directly from dispersion-engineered photonic chip surfaces.

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Fig. 1: Linear wave penetration and uniform energy losses across a periodically structured medium with EP-containing band diagrams.
Fig. 2: CMT and numerical analysis of the light radiated by a periodically structured SiNx slab waveguide.
Fig. 3: Experimental observation of the deep linear wave penetration with decay-free radiation profiles.
Fig. 4: Radiation loss profiles in non-Hermitian periodically structured media.

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Data availability

The data that support the findings of this study are available from the corresponding authors upon reasonable request.

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Acknowledgements

A.Y. acknowledges support under the Professional Research Experience Program (PREP), funded by the National Institute of Standards and Technology and administered through the Department of Chemistry and Biochemistry, University of Maryland. We also thank T. LeBrun, H. Lezec, J. Liu, J. A. Liddle and E. Secula for reading the manuscript and making insightful comments. The research was performed in part at the NIST Center for Nanoscale Science and Technology. This work is partially supported by the NIST-on-a-chip programme.

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Authors

Contributions

A.Y. and S.K. contributed to the project equally. S.K. conceived the idea. A.Y. and S.K. performed FEM and FDTD simulations. D.A.W. and A.Y. fabricated samples. Q.L., B.J.R. and K.S. contributed to the experimental device design and fabrication process development. A.Y. and S.K. characterized samples. A.Y. and V.A.A. developed theoretical analysis. A.Y., S.K. and V.A.A. contributed to the data interpretation. V.A.A. supervised the project. The manuscript was written through the extensive contributions of all authors. All authors have approved the final version of the manuscript.

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Correspondence to Alexander Yulaev, Sangsik Kim or Vladimir A. Aksyuk.

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Nature Nanotechnology thanks Stefan Rotter and the other, anonymous, reviewer(s) for their contribution to the peer review of this work.

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Extended data

Extended Data Fig. 1 Free-space beam angle and intensity dependences on the optical wavelength.

(a) The orange curve shows the radiation angle as a function of the wavelength for DC = 0.527. The black dashed line indicates 0°. (b) The corresponding band diagram (BD) for infinite grating. The dashed blue arrows depict the wavelength tuning. Once the wavelength crosses the EPs in the BD (panel b), the outcoupling angle experiences high variation about the chip’s normal, that is noticeable as a double kink in the wavelength dependence of the outcoupled angle (panel a).

Extended Data Fig. 2 Spatially uniform and non-uniform energy losses in non-Hermitian periodically structured media excited from one side.

FEM simulated time-averaged power flow along the uniform periodically structured waveguide in the positive z-direction (a) and averaged |E| over one grating period (low-pass spatial filtering) (b) vs. the coordinate z for the optical frequency tuned to the EP wavelength (red curve) and detuned (black curve) from the EP wavelength. The waveguide is excited by a wave incident from the left side at z = 10 µm.

Extended Data Fig. 3 Linear radiative energy losses experimentally observed in 45 µm, 100 µm, 180 µm, and 250 µm long gratings with ≈ 50 % DC.

Insets depict top-view optical images of the projected free-space beams. The saturated ≈ 20 µm wide spike at the grating input is due to the fabrication imperfections related to the electron lithography proximity effect (Supplementary Fig. 10).

Extended Data Fig. 4 Sample fabrication flowchart.

The partially etched gratings and supporting photonic structures are fabricated by sequential electron beam lithography patterning and etching of a silicon nitride layer, followed by silicon dioxide cladding deposition, as described in the Sample Fabrication section of the Methods.

Extended Data Fig. 5 Experimental apparatus.

Light from a tunable laser was fiber coupled through an attenuator (A) and polarization controller (PC) to the inverted taper waveguide couplers on the grating chip (device under test, DUT). Grating emission was imaged by a microscope camera. Free space linear polarizer P was used for polarization selective imaging to tune the input fiber polarization to transverse electric. Images were captured at the grating plane with additional images captured above the grating plane to assess emission angle.

Supplementary information

Supplementary Information

Supplementary discussion and Figs. 1–13.

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Yulaev, A., Kim, S., Li, Q. et al. Exceptional points in lossy media lead to deep polynomial wave penetration with spatially uniform power loss. Nat. Nanotechnol. 17, 583–589 (2022). https://doi.org/10.1038/s41565-022-01114-3

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