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GexSb20Se80-x玻璃的拉曼光谱和X射线光电子能谱
引用本文:许思维,王丽,沈祥.GexSb20Se80-x玻璃的拉曼光谱和X射线光电子能谱[J].物理学报,2015,64(22):223302-223302.
作者姓名:许思维  王丽  沈祥
作者单位:1. 北京工业大学应用数理学院, 北京 100124; 2. 宁波大学信息科学与工程学院, 宁波 315211
基金项目:国家自然科学基金(批准号: 11474014)和北京市教育委员会科技计划重点项目(批准号: Kz2011100050010)资助的课题.
摘    要:用拉曼散射光谱和X射线光电子能谱研究了GexSb20Se80-x(x=5 mol%, 10 mol%, 15 mol%, 17.5 mol%, 20 mol%和25 mol%)玻璃的结构. 通过对拉曼光谱和X射线光电子能谱(Ge 3d, Sb 4d 和Se 3d谱)进行分解, 发现当硫系玻璃处于富Se状态下时, 玻璃结构中会出现Se–Se–Se结构单元, 其数量随着Ge含量的增加而迅速减少, 并最终在Ge15Sb20Se65玻璃结构中消失; Ge和Sb原子分别以GeSe4/2 四面体和SbSe3/2三角锥结构单元在玻璃结构中出现, GeSe4/2四面体结构单元的数量会随着Ge浓度的增加而增加, 而SbSe3/2三角锥结构单元的数量基本保持稳定. 另一方面, 在缺Se的硫系玻璃中, 玻璃会有Ge–Ge和Sb–Sb同极键产生, 随着Ge含量的增大, 这种同极键的数量会越来越多; 而GeSe4/2四面体和SbSe3/2三角锥结构的数量则相应减少. 在所有玻璃样品的结构中均有同极键Se–Se的存在. 当玻璃组分越接近完全化学计量配比时, 异质键Ge–Se和Sb–Se将占据玻璃结构中的主导地位, 同极键Ge–Ge, Sb–Sb和Se–Se 的比例降为最小.

关 键 词:拉曼光谱  X射线光电子能谱  结构  硫系玻璃
收稿时间:2015-05-04

Raman scattering and X-ray photoelectron spectra of GexSb20Se80-x Glasses
Xu Si-Wei,Wang Li,Shen Xiang.Raman scattering and X-ray photoelectron spectra of GexSb20Se80-x Glasses[J].Acta Physica Sinica,2015,64(22):223302-223302.
Authors:Xu Si-Wei  Wang Li  Shen Xiang
Institution:1. College of Applied Sciences, Beijing University of Technology, Beijing 100124, China; 2. College of Information Science and Engineering, Ningbo University, Ningbo 315211, China
Abstract:In this paper, we prepare several GexSb20Se80-x glasses (x=5 mol%, 10 mol%, 15 mol%, 17.5 mol%, 20 mol%, and 25 mol%), and measure their Raman and X-ray photoelectron spectra (Ge 3d, Sb 4d, and Se 3d) in order to understand the evolution of the glass structure with chemical composition. We further decompose the spectra into different structural units according to the assignments of these structural units in the previous literature. It is found that the structural units of Se–Se–Se trimers exist in the Se-rich glasses, but the number of the structural units of trimers decreases rapidly with the increase of Ge concentration and finally becomes zero in Ge15Sb20Se65 glass. With the increase of Ge concentration, the quantity of GeSe4/2 tetrahedral structures increases, but the number of SbSe3/2 pyramidal structures remains almost unchanged in the Se-rich glasses. On the other hand, the numbers of Ge–Ge and Sb–Sb homopolar bonds increase with the increase of Ge concentration, but those of the GeSe4/2 tetrahedral and SbSe3/2 pyramidal structures decrease in the Se-poor glasses. Moreover, the Se–Se homopolar bonds exist in all the glasses, and they cannot be completely suppressed. When the composition is close to stochiometric value, the glass is dominated by heteropolar Ge–Se and Sb–Se bonds, but has negligible quantities of Ge–Ge, Sb–Sb and Se–Se homopolar bonds. The transition threshold, rather than the transition predicted by the topological constraint model, occurs at the chemically stoichiometric glasses. This suggests that chemical order, rather than topological order, is a main factor in determining structures and physical properties of Ge–Sb–Se glasses.
Keywords:Raman scattering  X-ray photoelectron spectroscopy  structure  chalcogenide glasses
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