Ionized physical vapor deposition of integrated circuit interconnects

被引:107
作者
Hopwood, J [1 ]
机构
[1] Northeastern Univ, Boston, MA 02115 USA
关键词
D O I
10.1063/1.872829
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
Interconnects, once the technological backwater of integrated circuit technology, now dominate integrated circuit cost and performance. As much as 90 percent of the signal delay time in future integrated circuit designs will be due to the interconnection of semiconductor devices while the remaining 10 percent is due to transistor-related delay. This shifts the thrust of critical research toward an improved understanding of interconnect science and technology. Shrinking circuit geometries will require high aspect ratio (AR) vias to interconnect adjacent metal layers. By the year 2007 it is predicted that logic circuits will use 6 to 7 interconnected metal layers with via ARs of 5.2:1. Memory will need fewer layers, but ARs as high as 9:1. In this paper, the demands of interconnect technology will be reviewed and the opportunities for plasma-based deposition of vias will be discussed. One promising new method of fabricating high-aspect ratio vias is ionized physical vapor deposition (I-PVD). The technique economically creates a unidirectional flux of metal which is uniform over 200-300 mm diameter wafers. Since metal ejected by conventional sputtering is primarily neutral and exhibits a cosine angular velocity distribution, sputtered metal atoms do not reach the bottom of high AR vias. By sputtering these atoms into a moderate pressure (4 Pa), high-density Ar plasma, however, the metal atoms are first thermalized and then ionized. The ions are then readily collimated by the plasma sheath and directionally deposited into narrow, deep via structures. Experiments have consistently shown that over 80% of the metal species are ionized using I-PVD. The physical mechanisms responsible for ionization will be discussed from both an experimental and modeling perspective and the spatial variation of metal ionization is experimentally determined. (C) 1998 American Institute of Physics.
引用
收藏
页码:1624 / 1631
页数:8
相关论文
共 45 条
[21]   MECHANISMS FOR HIGHLY IONIZED MAGNETRON SPUTTERING [J].
HOPWOOD, J ;
QIAN, F .
JOURNAL OF APPLIED PHYSICS, 1995, 78 (02) :758-765
[22]   RECOMMENDED DATA ON THE ELECTRON-IMPACT IONIZATION OF ATOMS AND IONS - FLUORINE TO NICKEL [J].
LENNON, MA ;
BELL, KL ;
GILBODY, HB ;
HUGHES, JG ;
KINGSTON, AE ;
MURRAY, MJ ;
SMITH, FJ .
JOURNAL OF PHYSICAL AND CHEMICAL REFERENCE DATA, 1988, 17 (03) :1285-1363
[23]   Simulations of metal thin film thermal flow processes [J].
Liao, H ;
Cale, TS .
JOURNAL OF VACUUM SCIENCE & TECHNOLOGY B, 1996, 14 (04) :2615-2622
[24]  
LIEBERMAN MA, 1994, PRINCIPLES PLASMA DI, P140
[25]   ELECTRON-IMPACT IONIZATION CROSS-SECTIONS FOR ATOMS UP TO Z=108 [J].
LOTZ, W .
ZEITSCHRIFT FUR PHYSIK, 1970, 232 (02) :101-&
[26]   MOBILITIES AND REACTIONS OF IONS IN ARGON [J].
MCAFEE, KB ;
SIPLER, D ;
EDELSON, D .
PHYSICAL REVIEW, 1967, 160 (01) :130-&
[27]  
MUARKA SP, 1993, METALLIZATION THEORY
[28]   Ionized physical vapor deposition of Cu for high aspect ratio damascene trench fill applications [J].
Nichols, CA ;
Rossnagel, SM ;
Hamaguchi, S .
JOURNAL OF VACUUM SCIENCE & TECHNOLOGY B, 1996, 14 (05) :3270-3275
[29]  
ONO T, 1988, JPN J APPL PHYS, V23, pL534
[30]  
POWELL R, 1996, COMMUNICATION