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铒铥共掺氧化锌薄膜近红外宽带发射及变温行为的研究
引用本文:陈丹丹,徐飞,曹汝楠,蒋最敏,马忠权,杨洁,杜汇伟,洪峰. 铒铥共掺氧化锌薄膜近红外宽带发射及变温行为的研究[J]. 物理学报, 2015, 64(4): 47104-047104. DOI: 10.7498/aps.64.047104
作者姓名:陈丹丹  徐飞  曹汝楠  蒋最敏  马忠权  杨洁  杜汇伟  洪峰
作者单位:1. 上海大学理学院物理系, 索朗光伏材料与器件R&D联合实验室, 分析测试中心, 上海 200444;2. 复旦大学, 应用表面物理国家重点实验室, 微纳光子结构教育部重点实验室, 先进材料实验室, 上海 200433
基金项目:国家自然科学基金(批准号:50602029,61274067,60876045);上海市基础研究重点项目(批准号:09JC1405900);上海大学课程建设项目(批准号:B.08-0101-14-111)资助的课题~~
摘    要:采用磁控共溅射技术制备了铒铥共掺杂氧化锌发光薄膜. 通过优化退火温度, 实现了薄膜的近红外 平坦宽带发射, 总带宽可达到~ 500 nm, 覆盖了光通信S+C+L+U 区波段. 此发射带由Er3+ 的1535 nm (4I13/24I15/2) 发射峰及Tm3+ 的1460 nm (3H43F4), 1640 nm (1G43F2), 1740 nm (3F43H6) 发射峰组成. 研究表明: 退火温度低于800 ℃ 时, 没有观察到薄膜样品明显的光致发光现象; 随着退火温度 从800 ℃ 升高到1000 ℃, I1640/I1535 发射峰强度比从0.2 升高到0.3, I1740/I1535 发射峰强度比从0.5 降低 到0.4, 发射峰强度比均基本保持稳定; 当退火温度高于1000 ℃ 时, I1640/I1535 发射峰强度比从0.3 升高到 0.6, I1740/I1535 发射峰强度比从0.4 升高到0.8, 发射峰强度比均急剧增加. 变温行为表明: 随着温度从10 K 逐渐升高到300 K, 谱线的总带宽基本不变, 在340—360 nm 之间; Tm3+ 在1640 和1740 nm 处的发射峰强度 分别降低了2/3 和1/2, Er3+ 在1535 nm 的发射峰强度增大了1.2 倍. 这是因为随着温度的升高, 声子数目增 多, Er3+ 与Tm3+ 离子之间发生能量传递的概率不断变大, 并且在Tm3+ 离子之间没有发生交叉弛豫现象.

关 键 词:稀土掺杂  氧化锌薄膜  近红外宽带发光  退火处理
收稿时间:2014-08-25

Near infrared broadband from Er-Tm codoped zinc oxide and temperature-dependent properties
Chen Dan-Dan;Xu Fei;Cao Ru-Nan;Jiang Zui-Min;Ma Zhong-Quan;Yang Jie;Du Hui-Wei;Hong Feng. Near infrared broadband from Er-Tm codoped zinc oxide and temperature-dependent properties[J]. Acta Physica Sinica, 2015, 64(4): 47104-047104. DOI: 10.7498/aps.64.047104
Authors:Chen Dan-Dan  Xu Fei  Cao Ru-Nan  Jiang Zui-Min  Ma Zhong-Quan  Yang Jie  Du Hui-Wei  Hong Feng
Affiliation:1. SHU-SolarE R&D Lab, Department of Physics, College of Sciences, Instrumental Analysis and Research Center, Shanghai University, Shanghai 200444, China;2. State Key Laboratory of Surface Physics, Key Laboratory of Micro and Nano Photonic Structure (Ministry of Education), Advanced Materials Laboratory, Fudan University, Shanghai 200433, China
Abstract:Er-Tm codoped ZnO thin film is synthesized by co-sputtering from separated Er, Tm, and ZnO targets. A flat and broad emission band is achieved in a range of 1400-2100 nm by optimizing annealing temperature, and the observed 1460, 1540, 1640 and 1740 nm emission bands are attributed to the transitions of Tm3+: 3H43F4, Er3+ 4I13/24I15/2, Tm3+ 1G43F2 and Tm3+ 3F43H6 transitions, respectively, which cover S, C, L, U bands. The intensity ratios of 1640 to 1535 nm and 1740 to 1535 nm below 1000 ℃ are nearly constant, while the ratios increase sharply above 1000 ℃. The temperature dependence of photoluminescence (PL) spectrum is studied under 10-300 K. With increasing the operation temperature, the bandwidth of broadband is nearly invariable (340-360 nm), and the Tm3+ PL emission intensities of 1640 nm and 1740 nm from Er-Tm co-doped ZnO thin film decrease by a factor of 1.5 and 2, respectively. Moreover, the 1535 nm emission intensity is increased by a factor of 1.2. This phenomenon is attributed to the complicated energy transfer (ET) processes involving both Er3+ and Tm3+ and the increase of phonon-assisted ET rate with temperature as well. And the cross relaxation between Tm3+ ions does not occur.
Keywords:rare earth doping  ZnO thin film  near-infrared broadband luminescence  heat treatment
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