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Sokhoyan R, Thureja P, Sisler J, Grajower M, Shayegan K, Feigenbaum E, Elhadj S, Atwater HA. Electrically tunable conducting oxide metasurfaces for high power applications. NANOPHOTONICS (BERLIN, GERMANY) 2023; 12:239-253. [PMID: 39634855 PMCID: PMC11501733 DOI: 10.1515/nanoph-2022-0594] [Citation(s) in RCA: 3] [Impact Index Per Article: 1.5] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 09/28/2022] [Revised: 12/20/2022] [Accepted: 12/21/2022] [Indexed: 12/07/2024]
Abstract
Active metasurfaces designed to operate at optical frequencies are flat optical elements that can dynamic, subwavelength-scale wavefront control of reflected or transmitted light. The practical and fundamental power-handling limits of active metasurfaces at high pulse energies and high average powers determine the potential applications for these emerging photonic components. Here, we investigate thermal performance limits of reflective gate-tunable conducting oxide metasurfaces illuminated with high power density laser beams, for both continuous wave (CW) and pulsed laser illumination. Our gate-tunable metasurfaces use indium tin oxide (ITO) as an active material, which undergoes an epsilon-near-zero (ENZ) transition under applied electrical bias. We experimentally show that under CW illumination, there is no significant change in the electrically tunable metasurface optical response for high irradiances ranging from 1.6 kW/cm2 to 9.1 kW/cm2 when the illuminating laser beam diameter is 7 μm. Even under an applied bias, when over 60% of the incoming light is absorbed in a 1 nm-thick charge accumulation layer within ITO, the local temperature rise in the metasurface is modest, supporting its robustness for high-power applications. Additionally, we theoretically show that in the ENZ regime, the metasurface reflectance can be increased by a factor of 10 by replacing the active ITO layer with cadmium oxide (CdO). Thus conducting oxide metasurfaces can tolerate the power densities needed in higher power applications, including free space optical communications, to light detection and ranging (LiDAR), as well as laser-based additive manufacturing.
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Affiliation(s)
- Ruzan Sokhoyan
- Thomas J. Watson Laboratories of Applied Physics, California Institute of Technology, Pasadena, CA91125, USA
| | - Prachi Thureja
- Thomas J. Watson Laboratories of Applied Physics, California Institute of Technology, Pasadena, CA91125, USA
| | - Jared Sisler
- Thomas J. Watson Laboratories of Applied Physics, California Institute of Technology, Pasadena, CA91125, USA
| | - Meir Grajower
- Thomas J. Watson Laboratories of Applied Physics, California Institute of Technology, Pasadena, CA91125, USA
| | - Komron Shayegan
- Thomas J. Watson Laboratories of Applied Physics, California Institute of Technology, Pasadena, CA91125, USA
| | - Eyal Feigenbaum
- National Ignition Facility and Photon Science, Lawrence Livermore National Laboratory, Livermore, CA94550, USA
| | - Selim Elhadj
- National Ignition Facility and Photon Science, Lawrence Livermore National Laboratory, Livermore, CA94550, USA
- Materials Engineering Division, Lawrence Livermore National Laboratory, Livermore, CA94550, USA
| | - Harry A. Atwater
- Thomas J. Watson Laboratories of Applied Physics, California Institute of Technology, Pasadena, CA91125, USA
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Atikian HA, Sinclair N, Latawiec P, Xiong X, Meesala S, Gauthier S, Wintz D, Randi J, Bernot D, DeFrances S, Thomas J, Roman M, Durrant S, Capasso F, Lončar M. Diamond mirrors for high-power continuous-wave lasers. Nat Commun 2022; 13:2610. [PMID: 35545622 PMCID: PMC9095672 DOI: 10.1038/s41467-022-30335-2] [Citation(s) in RCA: 6] [Impact Index Per Article: 2.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 09/19/2021] [Accepted: 04/26/2022] [Indexed: 12/02/2022] Open
Abstract
High-power continuous-wave (CW) lasers are used in a variety of areas including industry, medicine, communications, and defense. Yet, conventional optics, which are based on multi-layer coatings, are damaged when illuminated by high-power CW laser light, primarily due to thermal loading. This hampers the effectiveness, restricts the scope and utility, and raises the cost and complexity of high-power CW laser applications. Here we demonstrate monolithic and highly reflective mirrors that operate under high-power CW laser irradiation without damage. In contrast to conventional mirrors, ours are realized by etching nanostructures into the surface of single-crystal diamond, a material with exceptional optical and thermal properties. We measure reflectivities of greater than 98% and demonstrate damage-free operation using 10 kW of CW laser light at 1070 nm, focused to a spot of 750 μm diameter. In contrast, we observe damage to a conventional dielectric mirror when illuminated by the same beam. Our results initiate a new category of optics that operate under extreme conditions, which has potential to improve or create new applications of high-power lasers. Mirrors that demonstrate 98% reflectivity and withstand 10 kilowatts of focused continuous-wave laser light are created by nanoscale fabrication of single-crystal diamond. The work finds applications in medicine, defence, industry, and communications.
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Affiliation(s)
- Haig A Atikian
- John A. Paulson School of Engineering and Applied Sciences, Harvard University, Cambridge, MA, 01238, USA
| | - Neil Sinclair
- John A. Paulson School of Engineering and Applied Sciences, Harvard University, Cambridge, MA, 01238, USA.,Division of Physics, Mathematics and Astronomy, and Alliance for Quantum Technologies (AQT), California Institute of Technology, Pasadena, CA, 91125, USA
| | - Pawel Latawiec
- John A. Paulson School of Engineering and Applied Sciences, Harvard University, Cambridge, MA, 01238, USA
| | - Xiao Xiong
- John A. Paulson School of Engineering and Applied Sciences, Harvard University, Cambridge, MA, 01238, USA.,Key Laboratory of Quantum Information and Synergetic Innovation Center of Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, Anhui, 230026, China
| | - Srujan Meesala
- John A. Paulson School of Engineering and Applied Sciences, Harvard University, Cambridge, MA, 01238, USA
| | - Scarlett Gauthier
- John A. Paulson School of Engineering and Applied Sciences, Harvard University, Cambridge, MA, 01238, USA
| | - Daniel Wintz
- John A. Paulson School of Engineering and Applied Sciences, Harvard University, Cambridge, MA, 01238, USA
| | - Joseph Randi
- Pennsylvania State University Applied Research Laboratory, Electro-Optics Center, Freeport, PA, 16229, USA
| | - David Bernot
- Pennsylvania State University Applied Research Laboratory, Electro-Optics Center, Freeport, PA, 16229, USA
| | - Sage DeFrances
- Pennsylvania State University Applied Research Laboratory, Electro-Optics Center, Freeport, PA, 16229, USA
| | - Jeffrey Thomas
- Pennsylvania State University Applied Research Laboratory, Electro-Optics Center, Freeport, PA, 16229, USA
| | - Michael Roman
- Laser Technology and Analysis Branch, Naval Surface Warfare Center, Dahlgren Division, Dahlgren, VA, 22448, USA
| | - Sean Durrant
- Laser Technology and Analysis Branch, Naval Surface Warfare Center, Dahlgren Division, Dahlgren, VA, 22448, USA
| | - Federico Capasso
- John A. Paulson School of Engineering and Applied Sciences, Harvard University, Cambridge, MA, 01238, USA
| | - Marko Lončar
- John A. Paulson School of Engineering and Applied Sciences, Harvard University, Cambridge, MA, 01238, USA.
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