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机构地区:[1]盐城师范学院物理系,江苏盐城224002 [2]华东理工大学物理系,上海200237
出 处:《光谱学与光谱分析》2003年第1期154-156,共3页Spectroscopy and Spectral Analysis
基 金:江苏省教育厅自然科学研究基金项目
摘 要:本文用超声分散的方法将α Fe2 O3 超微粒分散于硬脂酸 /正己烷 /氯仿溶液中 ,使α Fe2 O3 超微粒被硬脂酸表面修饰。α Fe2 O3 超微粒被表面修饰后 ,紫外 可见光的吸收边从 392nm移动到 896nm ;红外光谱中的Fe—O键振动峰出现了“红移”现象 ,分别从 52 4 36cm- 1 移动到 52 1 33cm- 1 和从 446 37cm- 1 移动到 443 34cm- 1 ,表面修饰后 ,α Fe2 O3 超微粒X 射线衍射的相对强度明显增大 ,衍射峰位置向衍射角减小的方向移动。The α-Fe 2O 3 ultrafine particles were equally dispersed in the solutions of stearic acid/n-hexane/chloroform by the ultrasonic method, the surfaces of the α-Fe 2O 3 ultrafine particles were decorated by stearic acid, and the α-Fe 2O 3 ultrafine particles decorated had very good flowage characteristic. Before α-Fe 2O 3 ultrafine particles were decorated, the UV absorption was very strong at wavelengths shorter than 290 nm, and there was a shoulder peak at 330 nm. The absorption band edges of α-Fe 2O 3 ultrafine particles was at 392 nm, and shifted toward blue, which was in contrast with that of bulk Fe 2O 3. This was caused by the quanta size effect and surface effect. IR characteristic peaks of the α-Fe 2O 3 ultrafine particles appeared at 524.36 and 446.37 cm -1. After α-Fe 2O 3 ultrafine particles were decorated, the absorption side moved from 392 to 896 nm, which significantly shifted to the red in contrast with that of bulk F 2O 3. The vibration of Fe-O bond moved from 524.36 to 521.33 cm -1 and from 446.37 to 443.34 cm -1, respectively. These were caused by the dielectric confinement effect. The relative intensity of X-ray diffraction obviously increased, and the diffraction peak size moved toward the direction of smaller diffraction angle after the α-Fe 2O 3 ultrafine particles were decorated.
关 键 词:表面修饰 α-Fe2O3超微粒 光谱特性 N型半导体
分 类 号:TN304.21[电子电信—物理电子学]
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