Abstract
Exceptional point (EP) is a special degeneracy of nonHermitian systems. Onedimensional transmission systems operating at EPs are widely studied and applied to chiral conversion and sensing. Lately, twodimensional systems at EPs have been exploited for their exotic scattering features, yet so far been limited to only the nonvisible waveband. Here, we report a universal paradigm for achieving a highefficiency EP in the visible by leveraging interlayer loss to accurately control the interplay between the lossy structure and scattering lightwaves. A bilayer framework is demonstrated to reflect back the incident light from the left side (  r_{−1}  >0.999) and absorb the incident light from the right side (  r_{+1}  < 10^{–4}). As a proof of concept, a bilayer metasurface is demonstrated to reflect and absorb the incident light with experimental efficiencies of 88% and 85%, respectively, at 532 nm. Our results open the way for a new class of nanoscale devices and power up new opportunities for EP physics.
Similar content being viewed by others
Introduction
Exceptional point (EP)—characteristic of nonHermitian systems—refers to the spectral singularity of open systems whose eigenvalues and their corresponding eigenvectors degenerate simultaneously^{1,2,3}. NonHermitian systems have numerous alluring optical properties at EPs^{4,5,6,7} and have attracted extensive attention because of their great prospects in applications such as optical sensing^{8,9,10}, integrated optics^{11}, and other fields^{12,13,14,15,16,17}. In the early stage of implementing EPs, the optical gain and loss were integrated as nonconservative components in a simple onedimensional transmission system to achieve Eps^{18,19}, while the optical gain often leads to complex and unstable systems. EPs can also be observed by designing complex permittivity in allpassive systems, which inspires the study of EPrelated phenomena^{20}, for instance, the oneway cloaking^{21,22,23}. However, onedimensional transmission systems have limited capabilities in controlling lightwaves^{24,25,26,27,28}.
Metasurface, a class of artificial materials that transcends natural materials through the orderly design of subwavelength structures^{29,30,31,32,33,34,35,36}, has become a new platform to realize complex optical Eps^{27,37,38,39,40,41,42,43,44,45,46}. The reflection/transmission or diffraction of the metasurface can be described by scattering matrix^{47,48,49,50}. For a twoport scattering metasurface system (Fig. 1a), the scattering matrix describing the diffraction properties of the system is \(\left[\begin{array}{cc}{r}_{0} & {r}_{1}\\ {r}_{+1} & {r}_{0}\end{array}\right]\) (r_{0} is the specular reflection, r_{−1} and r_{+1} are retroreflections). When \(\sqrt{{r}_{1}{r}_{+1}}=0\), the eigenvalues of the scattering matrix are degenerate and an EP occurs. A common way to implement scattering EP is regulating the loss of the gradient metasurfaces by introducing a specific loss in a unit cell^{37,38,39}. Recent works have demonstrated nonHermitian metasurfaces composed of a lossassisted supercell (Fig. 1a) in the microwave range operating at an EP^{40,41,42}. However, direct extensions of inplane loss in a gradient metasurface from nonvisible waveband to visible light remain a formidable challenge, since the adjustable inplane loss and corresponding manufacturing process in the visible are lacking^{44}. Further, the complex and rebellious interplay between inplane lossy structure and lightwave restricts optical efficiency. Therefore, achieving highefficiency EP at optical nonHermitian metasurface is still a challenging task in photonics. Notably, twodimensional scattering systems operating at EPs in the visible are unexplored.
Here, we propose a strategy to use the interlayer loss to accurately control the interplay between the lossy structure and lightwaves via regulating the multiple scattering process using a bilayer architecture (Fig. 1a). A highefficiency scattering nonHermitian metasurface operating at an EP in the visible was demonstrated for the first time (Fig. 1b) to reflect back the incident light with leftside incidence (  r_{−1}  >0.999) and absorb the incident light with rightside incidence (  r_{+1}  <10^{−4}). As a proof of concept, we design a bilayer metasurface composed of TiO_{2} metagrating and Si subwavelength grating: the metagrating in the upper layer achieves the directional regulation of lightwave, and the lossy subwavelength grating in the lower layer achieves an adjustable absorption. The fabricated sample is experimentally demonstrated to reflect and absorb incident light with efficiencies of 88% and 85%, respectively, at 532 nm. Our work exhibits a universal paradigm for achieving a highefficiency EP in a twoport scattering system, which would inspire more novel photonic devices for wave manipulation.
Results
Models and theory
Traditional nonHermitian metasurface utilizes N subunits in one period to realize a gradient phase, as shown in Fig. 1a. When the lightwave impinges the metasurface with opposite directions, the metasurface would impose a pair of identical phase gradients (dφ/dx) to the lightwave, leading to the asymmetric reflection or transmission, also known as the generalized Snell’s law^{51}. In the case of extremely asymmetric responses, if the lossy structure is introduced, the lossy structure will absorb the lightwave selectively^{40}. Particularly, the perfect absorption will be achieved by elaborately designing the extinction coefficient and geometric parameters of the lossy structure, such that the twoport scattering metasurface system reaches an EP^{39,42}. However, the combination of lossless and lossy structures makes it difficult to regulate the interplay between lossy structure and lightwaves completely when lightwave impinges the metasurface from opposite directions. Therefore, traditional inplane lossy nonHermitian metasurfaces cannot exhibit highefficiency EPs. It is of the utmost importance in developing new design methodology to accurately control the interplay between lossy structure and lightwave for creating highefficiency optical EPs.
The highefficiency metasystem at an EP is essentially a wave vectordependent perfect retroreflector and absorber, as shown in the right of Fig. 1a. The key issue for achieving a highefficiency is controlling the interplay between lossy structure and lightwaves precisely: when the lightwave impacts from one side, the perfect retroreflector requires no interplay between the lossy structure and lightwave; when the lightwave impacts from the opposite side, the perfect absorber requires full interplay between the lossy structure and lightwave. Inplane lossless and lossy hybrid structures can never completely isolate the scattering of lightwaves from opposite directions. Hence, we propose the strategy to use an asymmetric metagrating and an interlayer lossy structure to accurately control the interplay between the lossy structure and the lightwave. On the one hand, the metagrating in the upper layer achieves a perfect retroreflection for the incident lightwave from one side by regulating the interference of Blochmode supported by the metagrating. On the other hand, the lossy structure in the lower layer achieves total absorption for the incident lightwave from the other side by adjusting the absorption coefficient of the lossy structure via a complex multiple scattering process.
Design of highefficiency scattering EP
The highefficiency metasystem at an EP is composed of an asymmetric metagrating for perfect retroreflection and a lossy structure for perfect absorption. The perfect retroreflection is based on Littrow grating by controlling the interference of Blochmodes^{52,53} with twogroove grating configuration. Firstly, a highefficiency Littrow grating is designed by leveraging the efficiency spectrum verse geometric parameters as shown in Section 1 of Supporting Information. When the geometric parameters of the twogroove grating are selected, the retroreflection amplitudes are approaching unity as shown in Section 1 of Supporting Information. The Littrow grating has exactly the same response when lightwaves impinge grating from two symmetrical directions given as \(\left[\begin{array}{cc}{r}_{0} & {r}_{1}\\ {r}_{+1} & {r}_{0}\end{array}\right]=\left[\begin{array}{cc}0 & 1\\ 1 & 0\end{array}\right]\). To break the symmetrical response of the grating, we moved the positions of the two grooves a certain distance, as shown in the inset of Fig. 2a. We can thus break the symmetric response while maintaining the retroreflection amplitude r_{−1} of 1 by changing the grating parameters locally. As exhibited in the spectra of Fig. 2a, the metagrating completely reflects the incident light from the left and partially reflects the incident light from the opposite direction. In this case, the scattering matrix of the metagrating develops to \(\left[\begin{array}{cc}{r}_{0} & {r}_{1}\\ {r}_{+1} & {r}_{0}\end{array}\right]=\left[\begin{array}{cc}0 & 1\\ x & 0\end{array}\right]\), where x ≫ 0 at the designed wavelength of 532 nm.
To further realize high efficiency (x = 0), a composite structure with a lossy interface under the spacer (the inset of Fig. 2c) is deployed to support the lightwave to undergo a multiple scattering process. The final response of the system can be described as
Here, R and R’ are the reflection coefficients of the metagrating as a plane wave is being incident from air and spacer, while the T and T’ are the transmission coefficients as a plane wave is being incident from air and spacer. A is a complex coefficient describing the effect of absorption/reflection amplitude and phase accumulation during the propagation, which is completely determined by the underlying lossy structure and spacer (detailed equations are given in Section 2 of Supporting Information). Although the metagrating itself cannot directly construct the scattering matrix required by highefficiency optical nonHermitian metasystem at EP, the multiple scattering process would enhance the ability of the metagrating in controlling lightwaves, thus expanding the range of the scattering matrix. Because the metagrating will reflect all the incident light back when it comes from the left (as shown in Fig. S3 of Supporting Information), we only need to consider the effect of the lossy structure on r_{+1}. As a result, the behaviors of lightwaves from opposite directions are completely isolated. Figure 2b shows the amplitude of r_{+1} versus the amplitude and phase of complex coefficient A. With a specific combination of amplitude and phase, the amplitude of r_{+1} can be controlled dynamically from near 0 to 1. When proper parameters such as (0.4538, 0.3412) for the amplitude and phase as marked by a yellow square are selected, the r_{+1} = x is less than 10^{−4} (near zero), which means 100% absorption. In this case, the scattering matrix of the metasystem develops to \(\left[\begin{array}{cc}{r}_{0} & {r}_{1}\\ {r}_{+1} & {r}_{0}\end{array}\right]=\left[\begin{array}{cc}0 & 1\\ 0 & 0\end{array}\right]\). Figure 2c demonstrates a wave vectordependent perfect retroreflector and absorber.
The eigenvalues of the scattering matrix of a nonHermitian system are \({\lambda }_{\pm }={r}_{0}\pm \sqrt{{r}_{+1}{r}_{1}}\). Figure 2d shows the evolution trajectories of eigenvalues with the amplitude variation of A while the phase of A equals 0.3412. Distinctly, when the amplitude of A is at 0.4538, an EP appears as the eigenvalues coalesce into a real number value, which is similar to what was observed in acoustic and optical systems^{39,42}. With the amplitude of A increasing, the amplitude of r_{+1} initially decreases and then increases, while the amplitude of r_{−1} is stably greater than 0.998, as shown in Fig. 2e. The amplitude of r_{+1} equals 0 when the amplitude of A is at 0.4538, indicating that the extraordinary retroreflection from the right port is completely suppressed. At the same time, the phase of r_{+1} experiences an abrupt change of π at the EP and the phase of r_{−1} is virtually constant when the amplitude of A changes, as shown in Fig. 2f. From the above analysis, it is not difficult to find that we have theoretically achieved a highefficiency optical nonHermitian system at an EP.
Experiments
As a proof of concept, we propose to use a Si subwavelength grating to realize the desired absorption/reflection, and an elaborately designed spacer to realize the phase accumulation, as shown in Fig. 3a. Although the resonant grating can also implement the desired absorption/reflection, the Si subwavelength grating not only simplifies the design, but also relaxes the alignment requirements in the fabrication. The phase accumulation during the propagation can be realized directly by choosing a spacer with a proper thickness (with a thickness larger than a quarterwavelength of light inside the spacer). Figure 3a shows the amplitude and phase of A verse the incident angle when the duty cycle of Si grating is 0.468 and the thickness of the spacer is 397.5 nm. It is worth noting that the transmittance is very small and can be neglected. The amplitude and phase of A are 0.458 and 0.354, respectively, at an incident angle of 20.6° as marked by a green square, corresponding to the requirement of the highefficiency optical nonHermitian metasurface at an EP. In the design process, what we care about is the amplitude and phase of the structure in the lower layer, that is coefficient A. Therefore, there is no limitation for the period or other matching problems. As long as it satisfies the requirements of Fig. 2b, it is a good candidate for highefficiency nonHermitian metasurface. Then, a highefficiency optical nonHermitian metasurface operating at EP, which is composed of the TiO_{2} metagrating and Si grating, is obtained. Detailed parameters of the bilayer metasurface are listed in Fig. S4 of Supporting Information.
The electric field distributions of the nonHermitian metasurface are exhibited in Fig. 3b, c to visually manifest the realization of highefficiency EP: when impinging the metasurface from the left direction, the lightwave is bounded within the metagrating, leading to no interplay between Si grating and lightwave; when impinging the metasurface from the righthand side, the lightwave penetrates the metagrating and is absorbed by the Si grating. In short, the highefficiency optical nonHermitian metasurface at EP is achieved via regulating the interplay between lossy structure and lightwave precisely by means of elaborately designing the TiO_{2} metagrating and Si grating.
A preparation process for bilayer microstructures was used to fabricate the sample as shown in Methods. Figures 4a, b show the top view and back view of the sample. The upper layer is TiO_{2} metagrating while the lower layer is Si grating. The angleresolved spectrum system in the microregion (as shown in Fig. S5 of Supporting Information) from Ideaoptics Inc. was employed in a darkroom to verify the spectral property of the nonHermitian metasurface. In the test, the angle resolution was realized by focusing the reflective beam in the Fourier plane of the lens. Then, the farfield scattered lightwaves from all angles of the sample were detected. We conducted two separate tests with incident angles of 30° and −30° as shown in the purple and red boxes of Fig. 4c. When the incident light impacted from the left, most of the light was reflected by the sample to the incident path. When the incident light came from the right, there was very little retroreflection light. The farfield scattered light from all angles at 532 nm was shown in Fig. 4d. The scattered field intensity of r_{−1} is 7.2 times stronger than r_{0}, while r_{0} is 3.7 times stronger than r_{+1}. In general, the scattered field intensity ratio between r_{−1} and r_{+1} is about 26.7:1. In this case, the fabricated sample demonstrated reflection efficiencies of 88%, 12%, and 3% for r_{−1}, r_{0}, and r_{+1}, respectively. The retroreflection and absorption efficiencies were 88% and 85%, respectively, for the left and rightside incidence at 532 nm. The degeneration of experimental results compared with designed results comes from the fabrication tolerance because the optical response of nonHermitian metasurface operating at EP is very sensitive to structural parameters. The efficiency could be further increased to the designed efficiency by optimizing the preparation process.
Discussion
The most important issue to realize the highefficiency optical nonHermitian metasurface at EP is regulating the interplay between the lossy structure and lightwaves. By utilizing the control ability of metagrating in the electromagnetic wave, an asymmetric response can be obtained. Nonetheless, it does not meet the demand of a nonHermitian metasurface operating at an EP. We propose an exquisite strategy to use an interlayer loss to accurately control the system loss. A multiple scattering process is stimulated by a bilayer configuration to enhance the ability in controlling lightwaves. We have theoretically achieved a highefficiency optical nonHermitian system at an EP by delicately regulating the interlayer loss. As a proof of concept, a subwavelength lossy grating is employed to realize the specific absorption and a bilayer highefficiency optical nonHermitian metasurface at EP is demonstrated. In fact, other structures like resonant structures, absorbing films and so forth, are also potential candidates for interlayer loss. Hence, the design of the highefficiency optical nonHermitian metasurface at EP using the proposed methodology is not cumbersome. However, due to the high sensitivity of nonHermitian systems, their performance is extremely sensitive to structural parameters, putting forward extremely stringent requirements for the preparation and testing, which is the major difficulty for the highefficiency optical nonHermitian metasurface operating at EP. Besides, if using the nonlinear material to realize the specific absorption or increasing the power of the input laser, the nonlinear EP or other nonlinear effects may be able studied^{54,55}.
In conclusion, to the best of our knowledge, we realized the first highefficiency scattering nonHermitian metasurface operating at EP in the visible by completely isolating the behavior of lightwaves from opposite directions. An interlayer loss is introduced to accurately control the system loss while a metagrating is used to realize a perfect retroreflector. The interlayer loss is precisely engineered by changing the duty cycle of a subwavelength lossy grating. We demonstrate a highefficiency scattering nonHermitian metasurface at 532 nm using our nontrivial methodologies in both design and experiment. Our work paves a new avenue toward the design of versatile optical metasurface platforms involving the EP or higherorder EP, which may inspire more functional photonic devices for wave manipulation.
Materials and methods
Sample fabrication
A preparation process for bilayer microstructures was used to fabricate the sample. Firstly, the Si was deposited on fused silica substrates using ion beam sputtering deposition in Vecco Spector System. The ionbeam voltage and ionbeam current were set as 900 V and 400 mA, respectively, with a base pressure of 4 × 10^{−4} Torr. The deposition rate of Si was 1.13 Å·s^{–1}. Then, a layer of positive electron beam resist (EBR) (ZEP520A) with a thickness of 120 nm was spincoated on the coating, followed by baking for 5 min at 180 °C on a hot plate. A 10nm chromium was then evaporation coated to avoid charging effects during the writing process. Next, target patterns were defined on the resist layer by EBL on a Raith 5200 system (100 kV, 3 nA). After EBL, the chromium was removed by chromium remover and the EBR was developed in amyl acetate for 1 min under gentle agitation. After that, we got the Si gratings on Oxford PlasmaPro100 Cobra with ICPRIE (inductively coupled reactive ion etching) using a mixture of SF_{6} and CHF_{3} gas (15 and 50 sccm, respectively) at a pressure of 15 mTorr, substrate bias of 380 V, ICP power of 800 W. Etch rate was approximately 1 nm·s^{–1}. A layer of negative optical photoresist HSQ (hydrogen silsequioxane) of thickness 500 nm was spincoated and exposed by the EBL process to cover the Si gratings. The thickness was corrected to the target value using ICPRIE. A layer of positive EBR (PMMA) with a thickness of 450 nm was spincoated on the HSQ, and exposed by the EBL process to get the negative metagrating patterns. The PMMA was developed with MIBK:IPA = 3:1 for 1 min under gentle agitation. The TiO_{2} is deposited directly onto the exposed EBR through atom layer deposition (ALD) at a low temperature (90 °C) to avoid the glass transition of EBR. During the ALD process, a standard twopulse system of water and TiCl_{4} precursor was used with a 0.05s water pulse followed by a 3s delay and a 0.4s TiCl_{4} pulse followed by a 4s delay, to ensure the complete reaction and full removal of the excessive precursors and reaction byproducts. The deposition rate was about 0.07 nm/cycle. This process ultimately left a nearly blanket film of TiO_{2} covering the entire EBR patterns which must be removed to expose individual patterns. This film was removed with ICPRIE using a mixture of CHF_{3} and Ar gas (20 and 80 sccm, respectively) at a pressure of 15 mT, substrate bias of 380 V, ICP power of 800 W. Etch rate was approximately 1.67 nm·s^{−1}. After the covering film was removed, we used oxygen plasma to remove the remaining photoresist and placed the samples in PG Remover for 24 h to make sure the EBR is removed completely.
Data availability
Data underlying the results presented in this paper are available from the corresponding author upon reasonable request.
References
Sun, Y. et al. Experimental demonstration of a coherent perfect absorber with PT phase transition. Phys. Rev. Lett. 112, 143903 (2014).
Zhu, X. F. et al. PTsymmetric acoustics. Phys. Rev. X 4, 031042 (2014).
Ashida, Y., Gong, Z. P. & Ueda, M. Nonhermitian physics. Adv. Phys. 69, 249–435 (2020).
Lawrence, M. et al. Manifestation of PT symmetry breaking in polarization space with terahertz metasurfaces. Phys. Rev. Lett. 113, 093901 (2014).
Chen, P. Y. et al. Generalized parity–time symmetry condition for enhanced sensor telemetry. Nat. Electron. 1, 297–304 (2018).
Sweeney, W. R. et al. Perfectly absorbing exceptional points and chiral absorbers. Phys. Rev. Lett. 122, 093901 (2019).
Zhang, X. L., Jiang, T. S. & Chan, C. T. Dynamically encircling an exceptional point in antiparitytime symmetric systems: asymmetric mode switching for symmetrybroken modes. Light Sci. Appl. 8, 88 (2019).
Zhong, Q. et al. Sensing with exceptional surfaces in order to combine sensitivity with robustness. Phys. Rev. Lett. 122, 153902 (2019).
Park, J. H. et al. Symmetrybreakinginduced plasmonic exceptional points and nanoscale sensing. Nat. Phys. 16, 462–468 (2020).
Hodaei, H. et al. Enhanced sensitivity at higherorder exceptional points. Nature 548, 187–191 (2017).
Li, A. D. et al. Hamiltonian hopping for efficient chiral mode switching in encircling exceptional points. Phys. Rev. Lett. 125, 187403 (2020).
Peng, B. et al. Lossinduced suppression and revival of lasing. Science 346, 328–332 (2014).
Song, H. G. et al. Roomtemperature polaritonic nonHermitian system with single microcavity. Nat. Photonics 15, 582–587 (2021).
Parto, M. et al. NonHermitian and topological photonics: optics at an exceptional point. Nanophotonics 10, 403–423 (2020).
Zhang, J. et al. A phonon laser operating at an exceptional point. Nat. Photonics 12, 479–484 (2018).
Wang, C. Q. et al. Electromagnetically induced transparency at a chiral exceptional point. Nat. Phys. 16, 334–340 (2020).
Zyablovsky, A. A. et al. Exceptional points as lasing prethresholds. Laser Photonics Rev. 15, 2000450 (2021).
Rüter, C. E. et al. Observation of parity–time symmetry in optics. Nat. Phys. 6, 192–195 (2010).
Chang, L. et al. Parity–time symmetry and variable optical isolation in active–passivecoupled microresonators. Nat. Photonics 8, 524–529 (2014).
Hou, J. K. et al. Selfinduced transparency in a perfectly absorbing chiral secondharmonic generator. PhotoniX 3, 22 (2022).
Lin, Z. et al. Unidirectional invisibility induced by PTsymmetric periodic structures. Phys. Rev. Lett. 106, 213901 (2011).
Feng, L. et al. Experimental demonstration of a unidirectional reflectionless paritytime metamaterial at optical frequencies. Nat. Mater. 12, 108–113 (2013).
Huang, Y. et al. Unidirectional reflectionless light propagation at exceptional points. Nanophotonics 6, 977–996 (2017).
Chen, W. J. et al. Exceptional points enhance sensing in an optical microcavity. Nature 548, 192–196 (2017).
ElGanainy, R. et al. NonHermitian physics and PT symmetry. Nat. Phys. 14, 11–19 (2018).
Miri, M. A. & Alù, A. Exceptional points in optics and photonics. Science 363, eaar7709 (2019).
Song, Q. H. et al. Plasmonic topological metasurface by encircling an exceptional point. Science 373, 1133–1137 (2021).
Shu, X. Q. et al. Fast encirclement of an exceptional point for highly efficient and compact chiral mode converters. Nat. Commun. 13, 2123 (2022).
Deng, Z. L. et al. Extreme diffraction control in metagratings leveraging bound states in the continuum and exceptional points. Laser Photonics Rev. 16, 2100617 (2022).
He, T. et al. Perfect anomalous reflectors at optical frequencies. Sci. Adv. 8, eabk3381 (2022).
Zhou, Y. et al. Multifunctional metaoptics based on bilayer metasurfaces. Light Sci. Appl. 8, 80 (2019).
McClung, A., Mansouree, M. & Arbabi, A. Atwill chromatic dispersion by prescribing light trajectories with cascaded metasurfaces. Light Sci. Appl. 9, 93 (2020).
Liu, M. Z. et al. Multifunctional metasurfaces enabled by simultaneous and independent control of phase and amplitude for orthogonal polarization states. Light Sci. Appl. 10, 107 (2021).
Shi, Y. Z. et al. Optical manipulation with metamaterial structures. Appl. Phys. Rev. 9, 031303 (2022).
Shi, Y. Z. et al. Chiralityassisted lateral momentum transfer for bidirectional enantioselective separation. Light Sci. Appl. 9, 62 (2020).
Qin, J. et al. Metasurface micro/nanooptical sensors: principles and applications. ACS Nano 16, 11598–11618 (2022).
Song, A. L. et al. Asymmetric absorption in acoustic metamirror based on surface impedance engineering. Phys. Rev. Appl. 12, 054048 (2019).
Ju, F. F. et al. Asymmetric acoustic retroflection with a nonHermitian metasurface mirror. Appl. Phys. Express 14, 124001 (2021).
Wang, X. et al. Extremely asymmetrical acoustic metasurface mirror at the exceptional point. Phys. Rev. Lett. 123, 214302 (2019).
Wang, X. C. et al. Extreme asymmetry in metasurfaces via evanescent fields engineering: angularasymmetric absorption. Phys. Rev. Lett. 121, 256802 (2018).
Li, M. et al. Controlling asymmetric retroreflection of metasurfaces via localized loss engineering. IEEE Trans. Antennas Propag. 70, 11858–11866 (2022).
Dong, S. H. et al. Lossassisted metasurface at an exceptional point. ACS Photonics 7, 3321–3327 (2020).
Park, S. H. et al. Observation of an exceptional point in a nonHermitian metasurface. Nanophotonics 9, 1031–1039 (2020).
Li, Z. P. et al. Nonhermitian electromagnetic metasurfaces at exceptional points. Prog. Electromagnetics Res. 171, 1–20 (2021).
Kang, M., Chen, J. & Chong, Y. D. Chiral exceptional points in metasurfaces. Phys. Rev. A 94, 033834 (2016).
Özdemir, Ş. K. et al. Paritytime symmetry and exceptional points in photonics. Nat. Mater. 18, 783–798 (2019).
Cannata, F., Dedonder, J. P. & Ventura, A. Scattering in PTsymmetric quantum mechanics. Ann. Phys. 322, 397–433 (2007).
Mostafazadeh, A. Spectral singularities of complex scattering potentials and infinite reflection and transmission coefficients at real energies. Phys. Rev. Lett. 102, 220402 (2009).
Ge, L., Chong, Y. D. & Stone, A. D. Conservation relations and anisotropic transmission resonances in onedimensional PTsymmetric photonic heterostructures. Phys. Rev. A 85, 023802 (2012).
Ambichl, P. et al. Breaking of PT symmetry in bounded and unbounded scattering systems. Phys. Rev. X 3, 041030 (2013).
Yu, N. F. et al. Light propagation with phase discontinuities: generalized laws of reflection and refraction. Science 334, 333–337 (2011).
Lalanne, P., Hugonin, J. P. & Chavel, P. Optical properties of deep lamellar Gratings: A coupled Blochmode insight. J. Lightwave Technol. 24, 2442–2449 (2006).
Ito, K. & Iizuka, H. Highly efficient 1storder reflection in Littrow mounted dielectric doublegroove grating. AIP Adv. 3, 062119 (2013).
Chen, Y. et al. Exceptional points with memory in a microcavity Brillouin laser. Optica 9, 971–979 (2022).
Benzaouia, M., Stone, A. D. & Johnson, S. G. Nonlinear exceptionalpoint lasing with ab initio MaxwellBloch theory. APL Photonics 7, 121303 (2022).
Acknowledgements
This work was supported by the National Natural Science Foundation of China (61925504, 62192770, 62305252, 61621001, 62205246, 62020106009, 6201101335, 62205249, 62192772, 62192771), Shanghai Pilot Program for Basic Research, Science and Technology Commission of Shanghai Municipality (17JC1400800, 20JC1414600, 21JC1406100), the “Shu Guang” project supported by Shanghai Municipal Education Commission and Shanghai Education (17SG22), Shanghai Municipal Science and Technology Major Project (2021SHZDZX0100), Special Development Funds for Major Projects of Shanghai Zhangjiang National Independent Innovation Demonstration Zone (Grant No. ZJ2021ZD008), The Fundamental Research Funds for the Central Universities, Project funded by China Postdoctoral Science Foundation (2022M712401).
Author information
Authors and Affiliations
Contributions
T.H., X.C., C.W.Q. and Y.L. conceived the original idea. T.H. and Z.Z. conducted the numerical simulations. X.C., C.W.Q. and Z.W. supervised the project. Z.Z. and T.H. prepared the devices with assistance from J.Z. on EBL. Z.Z. and T.H. performed the measurements and analysed the data. T.H., C.W.Q., Y.S., Z.L., H.W. wrote the manuscript. All authors discussed the results and commented on the manuscript.
Corresponding authors
Ethics declarations
Conflict of interest
The authors declare no competing interests.
Supplementary information
Rights and permissions
Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/.
About this article
Cite this article
He, T., Zhang, Z., Zhu, J. et al. Scattering exceptional point in the visible. Light Sci Appl 12, 229 (2023). https://doi.org/10.1038/s41377023012824
Received:
Revised:
Accepted:
Published:
DOI: https://doi.org/10.1038/s41377023012824
This article is cited by

Exceptional dynamics at exceptional points
Light: Science & Applications (2024)