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. 2023 Jul 24;12:180. doi: 10.1038/s41377-023-01223-1

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© The Author(s) 2023

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/.

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Fig. 4 — a Top: an enlarged adaptation curve upon 532 nm laser irradiation that can be divided into four stages (I, II, III, and IV). Bottom: schematic illustrations of dynamic current decay, corresponding to the four stages denoted in top panel. b Temperature-dependent real-time I_DS upon 532 nm laser irradiation (power intensity: 60 mW/cm²) from 288 to 300 K at zero bias and without cooling. c Normalized real-time I_DS excited by 480 nm, 530 nm, 640 nm light at the same power density of 60 mW/cm² with different areas of light illumination under zero bias voltage, including a small illumination area of about 60 μm² (labeled as 1) and a large one of about 360 μm² (labeled as 2)