欢迎登录材料期刊网

材料期刊网

高级检索

介绍了化学气相沉积(CVD)中的传质现象研究的最新进展,从传质方程的建立到边界条件确定都进行了详细的介绍,并举例说明了数值分析的结果对反应器设计与工艺参数的优化的指导作用.

参考文献

[1] Jitendra S G;Raymond L T .[J].Journal of Materials Science,1988,23:4331.
[2] Holstein W L;Fitzjohn J L .[J].Journal of Crystal Growth,1989,94:131.
[3] Hirschfelder J O;Curtiss C F;Bird R B.Kmetic Theoryof Gases and Liquids[M].Wiley,New York,1967
[4] Kleijn C R;Hoogendoom C J .[J].Journal of the Electrochemical Society,1989,136:3423.
[5] Reid R C;Prausnitz J M;Poling B E.The Propernes of Goses and Liqulds[M].MeGraw-Hill New York,1987
[6] 费祥麟.高等流体力学[M].西安:西安交通大学出版社,1989
[7] 高本辉;崔素言.真空物理[M].北京:科学出版社,1983
[8] Moffat H K;Jensen K F .[J].Journal of the Electrochemical Society,1989,135
[9] Kleijn C R;Hoogendoom C S .[J].Chemical Engineering Science,1991,46:321.
[10] Wahl G .[J].Thin Solid Films,1977,4O:13.
[11] Houtman C;Graves D B;Jensen K F .[J].Journal of the Electrochemical Society,1986,133:96.
[12] Michaelidis M;Pollard R .[J].Journal of the Electrochemical Society,1984,131:806.
[13] Coltrin M E;Kee R J;Zvanc G H .[J].Journal of the Electrochemical Society,1989,136:819.
[14] Ouazzan J;Rosenbcrger F .[J].Journal of Crystal Growth,1990,100:545.
[15] Vlacia J I;Howell S;Korner H et al.[J].Applied Surface Science,1989,38:370.
[16] Gokoglu S A;Kuczmarski M;Tsui P et al.[J].Journal of Phys(paris)Colloq c5 Syppl,1989,50(05):5.
[17] Evans G;Greif R .[J].International Journal of Heat and Mass Transfer,1989,32:895.
[18] Weber G;Van Opdorp C;Keijser D .[J].Journal of Applied Physics,1990,67:2109.
[19] Fotiadis P I;Kieda S;Jensen K F .[J].Journal of Crystal Growth,1990,102:441.
[20] Fottadis P I;Baekhok M;Jersen K F et al.[J].Journal of Crystal Growth,1990,100:577.
[21] Fotidis D I;Kremer A M;Mckenna D R et al.[J].Journal of Crystal Growth,1987,85:154.
[22] Rhee S;Seekeley J;Ilegbysi O J .[J].Journal of the Electrochemical Society,1987,134:2552.
[23] Kleijn C R;Hoogendoom C J;Hasper A J .[J].Electrochemical Society,1991,138:509.
上一张 下一张
上一张 下一张
计量
  • 下载量()
  • 访问量()
文章评分
  • 您的评分:
  • 1
    0%
  • 2
    0%
  • 3
    0%
  • 4
    0%
  • 5
    0%