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对Sn(Sb)O2干凝胶的结构进行了试验及模拟研究,通过BET-N2吸附及XRD分析,详细研究了SnO2凝胶在200~600 ℃干燥过程中凝胶骨架纳米结构及其变化规律,并研究了掺杂元素Sb对纳米结构演变的影响.研究发现:SnO2干凝胶为1~10 nm的纳米多孔结构,其结构特征符合圆柱体通孔模型;随着固化温度的升高,凝胶骨架粗化,但结构特征相似性不变,孔体积率也基本不变;Sb的增加有细化骨架的作用.

参考文献

[1] Ma HL.;Hao XT.;Ma J.;Yang YG.;Huang J.;Zhang DH.;Xu XG. .Thickness dependence of properties of SnO2 : Sb films deposited on flexible substrates[J].Applied Surface Science: A Journal Devoted to the Properties of Interfaces in Relation to the Synthesis and Behaviour of Materials,2002(1/4):313-318.
[2] SANTOR-PENA J;BROUSSE T;SANCHZ L et al.Antimony doping effect on the electrochemical behavior of SnO2 thin electrodes[J].Journal of Power Sources,2001,97-98:232-234.
[3] Aegerter MA;Reich A;Ganz D;Gasparro G;Putz J;Krajewski T .Comparative study of SnO2:Sb transparent conducting films produced by various coating and heat treatment techniques[J].Journal of Non-Crystalline Solids: A Journal Devoted to Oxide, Halide, Chalcogenide and Metallic Glasses, Amorphous Semiconductors, Non-Crystalline Films, Glass-Ceramics and Glassy Composites,1997(0):123-128.
[4] RAZZATO A P;BROUSSOUS L;SANTILLI C V et al.Structure of SnO2 aclcosol and films prepared by sol-gel dip coating[J].Journal of Non-Crystalline Solids,2001,284:61-67.
[5] Terrier C.;Roger JA.;Chatelon JP. .ELECTRICAL AND OPTICAL PROPERTIES OF SB-SNO2 THIN FILMS OBTAINED BY THE SOL-GEL METHOD[J].Thin Solid Films: An International Journal on the Science and Technology of Thin and Thick Films,1997(1/2):95-100.
[6] 王剑华;郭玉忠;刘荣佩.SnO2的溶胶-凝胶制备研究[J].稀有金属,1998(22):136-139.
[7] 黄瑞安 .溶胶-凝胶法SnO<,2>材料制备中的溶胶结构表征、演化动力学研究[D].昆明理工大学,1999.
[8] 郭玉忠,黄瑞安,孙加林.SnO2溶胶系水解缩合实验研究[J].硅酸盐学报,2001(02):157-162.
[9] Brinker C J;SHERER G W .Sol-Gel glass II:viscous sintering[J].Journal of Non-Crystalline Solids,1985,72:345-356.
[10] SHERER G W;BRINKER C J .Sol-gel glass III:viscous sintering[J].Journal of Non-Crystalline Solids,1985,72:369-378.
[11] 朱步瑶.界面化学基础[M].北京:化学工业出版社,1996
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