TY - JOUR
T1 - Intermetallic growth and void formation in Au wire ball bonds to Al pads
AU - Uno, Tomohiro
AU - Tatsumi, Kohei
N1 - Copyright:
Copyright 2017 Elsevier B.V., All rights reserved.
PY - 1999
Y1 - 1999
N2 - In order to clarify the reliability of Au wire bonds to Al pads, void formation and diffusion behavior were investigated using bonds annealed at various temperatures (423-573 K). We investigated the effects of the annealing environments, Al pad thickness, and bonding conditions on void formation. Voids became larger only when Au-Al intermetallics grew non-uniformly, whereas deleterious voids were not observed in the bonds annealed in vacuum. Oxide film on the surface of Al pads acts as a diffusion barrier at the interface. Optimized bonding conditions (applied pressure, ultrasonic energy) broke up the oxide film, resulting in reduction of void formation. Au5Al2 phase grew dominantly in the early stage of diffusion, then it transformed into Au4Al phase because the Al layer was completely consumed. The activation energy Q of transmission velocity at the Au/Au4Al boundary was 0.85 eV (82 kJ/mol). This is similar to the activation energy of the bond failure by annealing. These results indicate that void formation has a great correlation with the Au4Al growth. It is predicted that the non-uniform diffusion behavior causes vacancies to pile-up and these vacancies coalesce to form several types of voids in the interface.
AB - In order to clarify the reliability of Au wire bonds to Al pads, void formation and diffusion behavior were investigated using bonds annealed at various temperatures (423-573 K). We investigated the effects of the annealing environments, Al pad thickness, and bonding conditions on void formation. Voids became larger only when Au-Al intermetallics grew non-uniformly, whereas deleterious voids were not observed in the bonds annealed in vacuum. Oxide film on the surface of Al pads acts as a diffusion barrier at the interface. Optimized bonding conditions (applied pressure, ultrasonic energy) broke up the oxide film, resulting in reduction of void formation. Au5Al2 phase grew dominantly in the early stage of diffusion, then it transformed into Au4Al phase because the Al layer was completely consumed. The activation energy Q of transmission velocity at the Au/Au4Al boundary was 0.85 eV (82 kJ/mol). This is similar to the activation energy of the bond failure by annealing. These results indicate that void formation has a great correlation with the Au4Al growth. It is predicted that the non-uniform diffusion behavior causes vacancies to pile-up and these vacancies coalesce to form several types of voids in the interface.
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U2 - 10.2320/jinstmet1952.63.7_828
DO - 10.2320/jinstmet1952.63.7_828
M3 - Article
AN - SCOPUS:0032627145
SN - 0021-4876
VL - 63
SP - 828
EP - 837
JO - Nippon Kinzoku Gakkaishi/Journal of the Japan Institute of Metals
JF - Nippon Kinzoku Gakkaishi/Journal of the Japan Institute of Metals
IS - 7
ER -