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Abstract
Mechanoluminescence (ML) sensing technologies open up new opportunities for intelligent sensors, self-powered displays and wearable devices. However, the emission efficiency of ML materials reported so far still fails to meet the growing application requirements due to the insufficiently understood mechano-to-photon conversion mechanism. Herein, we propose to quantify the ability of different phases to gain or lose electrons under friction (defined as triboelectric series), and reveal that the inorganic-organic interfacial triboelectricity is a key factor in determining the ML in inorganic-organic composites. A positive correlation between the difference in triboelectric series and the ML intensity is established in a series of composites, and a 20-fold increase in ML intensity is finally obtained by selecting an appropriate inorganic-organic combination. The interfacial triboelectricity-regulated ML is further demonstrated in multi-interface systems that include an inorganic phosphor-organic matrix and organic matrix-force applicator interfaces, and again confirmed by self-oxidization and reduction of emission centers under continuous mechanical stimulus. This work not only gives direct experimental evidences for the underlying mechanism of ML, but also provides guidelines for rationally designing high-efficiency ML materials.
Mechanoluminescence enables sensing applications of mechanical stimuli. Here, the authors reveal the importance of interfacial triboelectricity to this phenomenon in inorganic-organic composite materials.
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1 China University of Geosciences Beijing, School of Materials Sciences and Technology, Beijing, China (GRID:grid.162107.3) (ISNI:0000 0001 2156 409X); Xiamen University, College of Materials, Xiamen, China (GRID:grid.12955.3a) (ISNI:0000 0001 2264 7233)
2 Xiamen University, College of Materials, Xiamen, China (GRID:grid.12955.3a) (ISNI:0000 0001 2264 7233); Xiamen University, Fujian Key Laboratory of Surface and Interface Engineering for High Performance Materials, Xiamen, China (GRID:grid.12955.3a) (ISNI:0000 0001 2264 7233)
3 Xiamen University, College of Materials, Xiamen, China (GRID:grid.12955.3a) (ISNI:0000 0001 2264 7233)
4 Japan Advanced Institute of Science and Technology, Graduate School of Advanced Science and Technology, Nomi, Japan (GRID:grid.444515.5) (ISNI:0000 0004 1762 2236)
5 China University of Geosciences Beijing, School of Materials Sciences and Technology, Beijing, China (GRID:grid.162107.3) (ISNI:0000 0001 2156 409X)
6 Ningbo University, School of Materials Science and Chemical Engineering, Ningbo, China (GRID:grid.203507.3) (ISNI:0000 0000 8950 5267)
7 Shenzhen University, College of Materials Science and Engineering, Shenzhen, China (GRID:grid.263488.3) (ISNI:0000 0001 0472 9649)
8 Shenzhen University, College of Physics and Optoelectronic Engineering, Shenzhen, China (GRID:grid.263488.3) (ISNI:0000 0001 0472 9649)
9 Chinese Academy of Sciences, Beijing Institute of Nanoenergy and Nanosystems, Beijing, China (GRID:grid.9227.e) (ISNI:0000000119573309)
10 Fudan University, Department of Vascular Surgery, Zhongshan Hospital, Shanghai, China (GRID:grid.8547.e) (ISNI:0000 0001 0125 2443)
11 Xiamen University, College of Materials, Xiamen, China (GRID:grid.12955.3a) (ISNI:0000 0001 2264 7233); Xiamen University, Fujian Key Laboratory of Surface and Interface Engineering for High Performance Materials, Xiamen, China (GRID:grid.12955.3a) (ISNI:0000 0001 2264 7233); State Key Laboratory of Physical Chemistry of Solid Surfaces, Xiamen, China (GRID:grid.12955.3a) (ISNI:0000 0001 2264 7233)