Integrated multi-scale model for ionized plasma physical vapor deposition

被引:20
作者
Arunachalam, V [1 ]
Rauf, S [1 ]
Coronell, DG [1 ]
Ventzek, PLG [1 ]
机构
[1] Motorola Inc, Semicond Prod Sector, DigitalDNA Labs, Austin, TX 78721 USA
关键词
D O I
10.1063/1.1371279
中图分类号
O59 [应用物理学];
学科分类号
摘要
In order to aid process development and address extendibility of ionized physical vapor deposition (IPVD) technology to future integrated circuit generations, an integrated model capable of simulating phenomena across the various length scales characteristic of these systems has been developed. The model is comprised of a two-dimensional equipment simulation, which relates process variables to characteristics of material fluxes to the wafer, and a three-dimensional Monte Carlo based feature scale model. The ion-surface interaction data required to model the surface processes is generated by a molecular dynamics based simulation. The integrated model is used to study the effect of various IPVD process parameters such as wafer bias, coil power, target power, and buffer gas composition on copper film profile inside a trench. Variations in film profile across the wafer are also examined. It is found that increasing the wafer bias results in an increase in the mean ion energy and the amount of sputtering inside the feature. This results in material transfer from the bottom of the feature to the sidewalls and faceting of the upper corners of the trench. Two variables, namely the total ion to Cu flux ratio (R(I/N)) and the mean ion energy, are found to play a crucial role in determining the effects of coil power and target power. Increasing the coil power enhances R(I/N) and slightly decreases the mean ion energy. This leads to more sputtering, and therefore a thicker film on the sidewalls relative to that on the bottom. Increase in target power causes R(I/N) to decrease, which decreases sputtering within the feature. Film profiles generally show evidence of enhanced sputtering as buffer gas ionization threshold decreases (He --> Ne --> Ar --> Xe) for the gases considered. These variations can be explained in terms of two factors: Cu flux ionization fraction, which decreases with buffer gas ionization threshold, and mean ion energy, which increases with ionization threshold. (C) 2001 American Institute of Physics.
引用
收藏
页码:64 / 73
页数:10
相关论文
共 23 条
[1]   Three-dimensional spatiokinetic distributions of sputtered and scattered products of Ar+ and Cu+ impacts onto the Cu surface:: Molecular dynamics simulations [J].
Abrams, CF ;
Graves, DB .
IEEE TRANSACTIONS ON PLASMA SCIENCE, 1999, 27 (05) :1426-1432
[2]  
ARUNACHALAM V, 1999, S DRY PROC TOK JAP 1, P63
[3]  
Bang D. S., 1995, Simulation of Semiconductor Devices and Processes. Vol.6, P166
[4]   A UNIFIED LINE-OF-SIGHT MODEL OF DEPOSITION IN RECTANGULAR TRENCHES [J].
CALE, TS ;
RAUPP, GB .
JOURNAL OF VACUUM SCIENCE & TECHNOLOGY B, 1990, 8 (06) :1242-1248
[5]   Monte Carlo simulations of sputter deposition and step coverage of thin films [J].
Coronell, DG ;
Egan, EW ;
Hamilton, G ;
Jain, A ;
Venkatraman, R ;
Weitzman, B .
THIN SOLID FILMS, 1998, 333 (1-2) :77-81
[6]   MODELING BIAS SPUTTER PLANARIZATION OF METAL-FILMS USING A BALLISTIC DEPOSITION SIMULATION [J].
DEW, SK ;
SMY, T ;
TAIT, RN ;
BRETT, MJ .
JOURNAL OF VACUUM SCIENCE & TECHNOLOGY A-VACUUM SURFACES AND FILMS, 1991, 9 (03) :519-523
[7]  
Font G., 1999, B AM PHYS SOC, V44, P74
[8]   THIN-FILM MICROSTRUCTURE MODELING THROUGH LINE-SEGMENT SIMULATION [J].
FRIEDRICH, LJ ;
DEW, SK ;
BRETT, M ;
SMY, T .
THIN SOLID FILMS, 1995, 266 (01) :83-88
[9]   Design issues in ionized metal physical vapor deposition of copper [J].
Grapperhaus, MJ ;
Krivokapic, Z ;
Kushner, MJ .
JOURNAL OF APPLIED PHYSICS, 1998, 83 (01) :35-43
[10]   Liner conformality in ionized magnetron sputter metal deposition processes [J].
Hamaguchi, S ;
Rossnagel, SM .
JOURNAL OF VACUUM SCIENCE & TECHNOLOGY B, 1996, 14 (04) :2603-2608