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采用电子陶瓷工艺制备了一系列玻璃/尖晶石陶瓷复合材料,结果表明:复合材料的介电常数、热膨胀系数和显微硬度随着尖晶石含量的增加而增加,而且材料中硼酸铝的生成对复合材料的介电和热膨胀性能有一定影响.所制备的复合材料具有低的介电常数(5.5~6.5)、低的热膨胀系数(5.3×10-6~5.5×10-6℃-1)和低的烧结温度(≤1000℃),有望用于先进的微电子封装基板材料.

参考文献

[1] Tummala R R .Ceramic and glass-ceramic packaging in the 1990s[J].Journal of the American Ceramic Society,1991,74(05):895-908.
[2] Shimada Y;Kobayashi Y;Kata K et al.Large scale multiplayer glass ceramic substrate for supercomputer[J].IEEE Transactions on Components Packaging and Manufacturing Technology,1990,13(04):751-758.
[3] Bridged D R;McMillan P W .Development of the Alpha-cordierite phase in glass-ceramics for use in electronic devices[J].Glass Technology,1985,26:286-292.
[4] Sarah H K;Ananda H K;Herron L W .Cordierite glass-ceramics for multilayer ceramic packaging[J].American Ceramic Society Bulletin,1993,72:90-95.
[5] Jean J.-H.;Gupta T.K. .Design of low dielectric glass+ceramics for multilayer ceramic substrate[J].IEEE transactions on components, packaging, and manufacturing technology.Part B.Advanced packaging,1994(2):228-233.
[6] Jean Jau-ho;Gupta Tapan K .Alumina as a devitrification inhibitor during sintering of borosilicate glass powders[J].Journal of the American Ceramic Society,1993,76(08):2010-2016.
[7] Jean Jau-ho;Gupta Tapan K .Isothermal and nonisothermal sintering kinetics of glass-filled ceramics[J].Journal of Materials Research,1992,7(12):3342-3347.
[8] EI-Kheshen A A .Effect of alumina addition on properties of glass/ceramic composite[J].British Ceramic Transactions,2003,102(05):205-209.
[9] Jean J H;Chang C R .Effect of crystallizable cordierite glass on devitrification of Pyrex borosilicate glass[J].Materials Science and Engineering A,1995,199:L11-L13.
[10] Imanaka Y;Kamehara N;Niwa K .The sintering process of glass/ceramic composites[J].Journal of the Ceramic Society of Japan,1990,98(08):817-822.
[11] 陈若愚,汪海东,夏树屏,高世扬.硼酸铝晶须合成物料的热分析[J].盐湖研究,1997(03):79.
[12] 李武.硼酸铝晶须的性质、制备和开发前景[J].盐湖研究,2000(03):40-43.
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