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发展了一种制备高烧结性Y2O3粉的新途径,并以此为原料,在相对低温下采用普通烧结的办法制备出透明Y2O3陶瓷.以硝酸钇为母盐,氨水为沉淀剂,通过控制反应体系中硫酸根离子的含量,生成树枝状的前驱物晶粒,其轴径比为6,经过1100℃煅烧分解,获得一次颗粒为60um,颗粒呈球形,低团聚高纯度的Y2O3粉体.该粉体经过模压成型,不加添加剂,于1700℃真空烧结,得到显微组织均匀的透明Y2O3多晶体,其在近红外区的透光率达70%.

A new method for obtaining highly sinterable Y2O3 powders was developed. Those powders were used to prepare transparent bodies with
conventional sintering at relatively low temperature. Yttrium nitrate was used as a mother salt, and ammonia as a precipitant reagent, the fine
and dendritic precursor crystal was prepared by controlling the content of sulfate ions in the reaction system. The highly pure and low-agglomerated
Y2O3 powders were obtained by calcinating the precursor at 1100℃, the primary particles were spherical and about 60nm
in diameter. The powder compact pressed in steel die could be sintered to transparency without additives under vacuum at 1700℃. The sintered
transparent Y2O3 polycrystalline exhibited a homogeneous microstructure and its transmittance was up to 70% in the near infrared wavelength region.

参考文献

[1] 关振铎. 无机材料物理性能. 北京: 清华大学出版社, 1992. 188--190.
[2] 徐政. 现代功能陶瓷. 北京: 国防工业出版社, 1998. 123--124.
[3] Greskovich C, Chernoch J P. J. Appl. Phys., 1973, 44 (10): 4599--4604.
[4] Chang N C. J. Appl. Phys., 1963, 34 (12): 3500--3506.
[5] Lefever R A. Mater. Res. Bull., 1967, 2 (9): 865--868.
[6] Dutta S K. Mater. Res. Bull., 1969, 4 (11): 791--793.
[7] Greskovich C. Am. Ceram. Soc. Bull., 1973, 52 (5): 473--476.
[8] Ikesue A. J. Am. Ceram. Soc., 1996, 79 (2): 359--364.
[9] Ikesue A. J. Jap. Ceram. Soc., 1995, 103 (11): 1155--1160.
[10] Wolfgang M. J. Am. Ceram. Soc., 2000, 83 (7): 1557--1574.
[11] Vollater D. Aerosol Methods and Advanced Technikquies for Nawoparticle Science and Napowder Technology. Drusburg, Germany, 1993. 15--30.
[12] Ikegami T. J. Jap. Ceram. Soc., 1999, 107 (3): 297--300.
[13] Noriko S. J. Am. Ceram. Soc., 1998, 81 (8): 2023--2027.
[14] Ikesue A. J. Am. Ceram. Soc., 1997, 80 (6): 1517--1521.
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