Year
Month
(Peer-Reviewed) Perovskite nanocrystals in glass for high efficiency and ultra-high resolution dynamic holographic multicolor display
Chao Ruan ¹, Xinkuo Li ¹, Ke Sun ², Jianrong Qiu ¹, Dezhi Tan ¹
¹ State Key Laboratory of Extreme Photonics and Instrumentation, College of Optical Science and Engineering, and School of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, China
中国 杭州 浙江大学光学科学与工程学院、材料科学与工程学院 极端光学技术与仪器全国重点实验室
² China International Science & Technology Cooperation Base for Laser Processing Robotics, Wenzhou University, Wenzhou 325035, China
中国 温州 温州大学激光加工机器人国家国际科技合作基地
Opto-Electronic Advances, 2026-03-25
Abstract

Incorporating perovskite nanocrystals (PNCs) in the glass matrix has been demonstrated to be an effective route to improve their stability for long-term operation. However, simultaneously achieving high luminance and high photoluminescence (PL) quantum yield (QY) is challenging. Herein, we report a strategy that employs fluoride ion doping to modify the three-dimensional glass network, thereby optimizing the crystallization behavior of PNCs and achieving both high luminance and high PLQY in full-spectrum.

Leveraging these high-performance transparent composites, we constructed a dynamic holographic multicolor display system by integrating with a spatial light modulator (SLM), achieving a pixel density as high as 20,247 pixels per inch (PPI). We further propose a vertically stacked, multilayer full-color display architecture that overcomes the limitations of color filters in light-utilization efficiency and the bottlenecks of conventional planar sub-pixel layouts in terms of spatial utilization and resolution.
Perovskite nanocrystals in glass for high efficiency and ultra-high resolution dynamic holographic multicolor display_1
Perovskite nanocrystals in glass for high efficiency and ultra-high resolution dynamic holographic multicolor display_2
Perovskite nanocrystals in glass for high efficiency and ultra-high resolution dynamic holographic multicolor display_3
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