Study paves the way for new class of nanoscale devices, new opportunities in photonics

Recently, , a class of artificial materials that transcends through the orderly design of subwavelength structures, has become a new platform to realize complex optical EPs.

A common way to implement scattering EP in the acoustic/microwave range is regulating the loss of the gradient metasurfaces by introducing a specific loss in a unit cell. However, direct extensions of in-plane loss in a gradient metasurface from non-visible waveband to remain a formidable challenge, since the adjustable in-plane loss and corresponding manufacturing process in the visible are lacking.

Furthermore, the complex and rebellious interplay between in-plane lossy structure and lightwave restricts optical efficiency. Therefore, achieving high-efficiency EP at optical non-Hermitian metasurface is still a challenging task in photonics. Notably, two-dimensional scattering systems operating at EPs in the visible are unexplored.

In a paper published in Light: Science & Applications, a team of scientists, led by Professor Cheng-Wei Qiu from Department of Electrical and Computer Engineering, National University of Singapore, Singapore and Xinbin Cheng from Institute of Precision Optical Engineering, School of Physics Science and Engineering, Tongji University, Shanghai, and co-workers have reported a universal paradigm for achieving a high-efficiency EP in the visible by leveraging interlayer loss to accurately control the interplay between the lossy structure and scattering lightwaves.

Fig 1. a, The physical model and principle of the optical non-Hermitian metasurfaces operating at an EP based on the in-plane loss. b, The physical model and principle of the optical non-Hermitian metasurfaces operating at an EP based on the interlayer loss. Credit: Tao He, Zhanyi Zhang, Jingyuan Zhu, Yuzhi Shi, Zhipeng Li, Heng Wei, Zeyong Wei, Yong Li, Zhanshan Wang, Cheng-Wei Qiu, Xinbin Cheng

Fig 2. a, The spectra and schematics of the high-efficiency optical non-Hermitian meta-system at EP. The |r₋₁| is larger than 0.999 and |r₊₁| is less than 10⁻⁴. b, Trajectories of eigenvalues with the evolution of absorption parameter. c, The amplitude of non-specular reflection coefficients r₋₁ and r₊₁ by varying absorption parameter. Credit: Tao He, Zhanyi Zhang, Jingyuan Zhu, Yuzhi Shi, Zhipeng Li, Heng Wei, Zeyong Wei, Yong Li, Zhanshan Wang, Cheng-Wei Qiu, Xinbin Cheng

Fig 3. a, Top view and back view of the sample. The upper layer is TiO2 metagrating and the lower layer is Si grating. b, The far-field scattered light from all angles of the sample with incident angles of 30° and -30°. c, The experimental measured far-field scattered light from all angles with incident angles of 30° and -30° at 532 nm. Credit: Tao He, Zhanyi Zhang, Jingyuan Zhu, Yuzhi Shi, Zhipeng Li, Heng Wei, Zeyong Wei, Yong Li, Zhanshan Wang, Cheng-Wei Qiu, Xinbin Cheng