Zhu, Guodong., Hong, Ikjun., Li, Kewei., Anyika, Theodore., Ugwu, Maxwell T., Nolen, Joshua Ryan., He, Mingze., Caldwell, Joshua David., & Ndukaife C, Justus C. (2025).Ìý.ÌýAdvanced Optical Materials. Advance online publication.Ìý
²Ñ±ð³Ù²¹±ô-²ú²¹²õ±ð»åÌýthermal metasurfaces are special materials designed to control how heat is emitted as light. Unlike traditional materials—such as gray-bodies, near–black bodies, or some dielectric metasurfaces—these metal-based structures keep their emission patterns stable even when temperatures change. However, they often have a major drawback: they lose a lot of energy internally through ohmic losses, which limits their quality (Q) factor, a measure of how sharp and selective their emission is.
This study focuses on solving that problem by finding a way to achieve both high emissivity (how effectively a material emits thermal radiation) and high Q factors in metal-based thermal emitters. The researchers use a design strategy that combines three surface lattice resonances. These resonances support special physical effects called bound states in the continuumÌý²¹²Ô»åÌýelectromagnetically induced absorption (EIA), which together allow the structure to emit light very efficiently and at very specific wavelengths.
Using simulations, the team designed a metal-based metasurface that achieves near-unity emissivity (0.96) and a Q factor of 320. Experiments confirmed strong performance, showing an emissivity of 0.82 and a Q factor of 202—a²ú´Ç³Ü³ÙÌýfive times better than the best previously reported metal-based thermal metasurfaces.
Overall, this work demonstrates a promising way to create efficient, narrow-band, and directional thermal emitters that maintain stable performance even across large temperature changes.

Figure 1
Schematic of the metal-insulator-metal (MIM) configuration used in the study. a) shows the schematic of the thermal metasurface for narrowband directional thermal emission. b) shows the top view of a unit cell of the metasurface comprising a complete circular gold ring and a segmented gold ring. c) shows the side view of a unit cell. A 150 nm gold reflector is thick enough to prevent optical transmission, and a 150 nm aluminum oxide spacer is used to maximize the emission.