van der Waals Transition-Metal Oxide for Vis-MIR Broadband Photodetection via Intercalation Strategy

被引:44
作者
He, Ruihui [1 ]
Chen, Zefeng [3 ,4 ]
Lai, Haojie [1 ]
Zhang, Tiankai [3 ,4 ]
Wen, Jinxiu [5 ]
Chen, Huanjun [5 ]
Xie, Fangyan [6 ]
Yue, Song [1 ]
Liu, Pengyi [1 ]
Chen, Jian [6 ]
Xie, Weiguang [1 ,5 ]
Wang, Xiaomu [2 ]
Xu, Jianbin [3 ,4 ,5 ]
机构
[1] Jinan Univ, Guangzhou Key Lab Vacuum Coating Technol & New En, Guangdong Prov Engn Technol Res Ctr Vacuum Coatin, Siyuan Lab,Dept Phys, Guangzhou 510632, Guangdong, Peoples R China
[2] Nanjing Univ, Sch Elect Sci & Technol, Nanjing 210093, Jiangsu, Peoples R China
[3] Chinese Univ Hong Kong, Dept Elect Engn & Mat Sci, Hong Kong 999077, Peoples R China
[4] Chinese Univ Hong Kong, Technol Res Ctr, Hong Kong 999077, Peoples R China
[5] Sun Yat Sen Univ, State Key Lab Optoelect Mat & Technol, Guangdong Prov Key Lab Display Mat & Technol, Sch Elect & Informat Technol, Guangzhou 510275, Guangdong, Peoples R China
[6] Sun Yat Sen Univ, Instrumental Anal & Res Ctr, Guangzhou 510275, Guangdong, Peoples R China
基金
中国国家自然科学基金;
关键词
2D material; intercalation; metal oxide; broadband absorption; photodetection; 2-DIMENSIONAL MATERIALS; MOO3; MOBILITY; HYDROGENATION; TEMPERATURE;
D O I
10.1021/acsami.9b00181
中图分类号
TB3 [工程材料学];
学科分类号
0805 ; 080502 ;
摘要
Defects engineering can broaden the absorption band of wide band gap van der Waals (vdW) materials to the visible or near-IR regime at the expense of material stability and photoresponse speed. Herein, we introduce an atomic intercalation method that brings the wide band gap vdW alpha-MoO3 for vis-MIR broadband optoelectronic conversion. We confirm experimentally that intercalation significantly enhances photoabsorption and electrical conductivity buts effects negligible change to the lattice structure as compared with ion intercalation. Charge transfer from the Sn atom to the lattices induces an optoelectrical change. As a result, the Sn-intercalated alpha-MoO3 shows room temperature, air stable, broadband photodetection ability from 405 nm to 10 mu m, with photoresponsivity better than 9.0 A W-1 in 405-1500 nm, similar to 0.4 A W-1 at 3700 nm, and 0.16 A W-1 at 10 mu m, response time of similar to 0.1 s, and peak D* of 7.3 X 10(7) cm Hz(0.5) W-1 at 520 nm. We further reveal that photothermal effect dominates in our detection range by real-time photothermal-electrical measurement, and the materials show a high temperature coefficient of resistance value of -1.658% K-1 at 300 K. These results provide feasible route for designing broadband absorption materials for photoelectrical, photothermal, or thermal-electrical application.
引用
收藏
页码:15741 / 15747
页数:7
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