MATERIALS TRANSACTIONS
Online ISSN : 1347-5320
Print ISSN : 1345-9678
ISSN-L : 1345-9678
Kinetics of Solid-State Reactive Diffusion between Au and Al
Minho OMasanori Kajihara
Author information
JOURNAL FREE ACCESS

2011 Volume 52 Issue 4 Pages 677-684

Details
Abstract

In the wire bonding technique, a thin Au wire is interconnected with an Al layer on a Si chip. During energization heating at solid-state temperatures, however, brittle Au-Al compounds with high electrical resistivities are formed at the interconnection by the reactive diffusion between Au and Al. In order to examine the growth behavior of the Au-Al compounds, the kinetics of the reactive diffusion was experimentally observed using sandwich Al/Au/Al diffusion couples. The diffusion couple was prepared by a diffusion bonding technique and then isothermally annealed at temperatures of 623–723 K for various times up to 103 h. Under such annealing conditions, the diffusion couple is practically considered semi-infinite. Owing to annealing, compound layers consisting of AuAl2, AuAl and Au8Al3 are produced at the initial Au/Al interface in the diffusion couple. The volume fraction in the compound layers is larger for Au8Al3 than for AuAl and AuAl2 in the early stages but becomes smaller for Au8Al3 than for AuAl and AuAl2 in the late stages. However, there are no systematic dependencies of the volume fraction on the annealing time and temperature. The total thickness of the compound layers is proportional to a power function of the annealing time. The exponent of the power function is smaller than 0.5 at 673–723 K. The exponent smaller than 0.5 means that the interdiffusion across the compound layers governs the layer growth and boundary diffusion predominantly contributes to the interdiffusion. On the other hand, at 623 K, the exponent is equal to unity for annealing times shorter than 8 h but smaller than 0.5 for those longer than 8 h. The exponent of unity indicates that the layer growth is controlled by the interface reaction at the migrating interface. Thus, at T=623 K, the transition of the rate-controlling process occurs at a critical annealing time of 8 h.

Content from these authors
© 2011 The Japan Institute of Metals and Materials
Previous article Next article
feedback
Top