AVS 60th International Symposium and Exhibition | |
Electronic Materials and Processing | Thursday Sessions |
Session EM-ThA |
Session: | Materials and Process for Advanced Interconnects II |
Presenter: | K. Shah, Applied Materials, Inc. |
Authors: | S. Kesapragada, Applied Materials, Inc. K. Shah, Applied Materials, Inc. |
Correspondent: | Click to Email |
While much attention is focused on transistor innovation, it is interconnect performance that is
also now challenging Moore’s law because of its performance and scaling limitations. The last
time interconnects were overhauled for performance reasons was more than 15 years ago when
aluminum was replaced with copper interconnects fabricated in the revolutionary dualdamascene
architecture.
Copper dual-damascene interconnects provided superior lower resistance, and the incorporation
of porous low-k dielectrics into this architecture drove down the capacitance – together these two
materials have reduced RC delay and reduced energy consumption. However, the reduction of
the low-k dielectric constant has slowed in recent years. As they become more porous, these
dielectric materials become fragile, unable to cope with the mechanical stress that chips undergo
during packaging. They are not robust enough to maintain their low-k properties through the
dual-damascene process integration steps. In addition, the resistance of the interconnect is rising
dramatically because of three main factors: (i) the conventional tantalum nitride/tantalum highresistance
metallic barriers that block copper diffusion and prevent oxidation are taking up a
larger fraction of the metal interconnect cross-section, (ii) surface scattering increases as the
critical dimensions of the wires become smaller than the bulk mean free path of the electrons,
and (iii) grain boundary scattering increases as the copper grain size scales approximately with
the critical dimensions of the wires in dual-damascene fabricated interconnects. Hence, the RC
delay for interconnects has started to rise dramatically as the node shrinks beyond 22nm, driven
by the rise in resistivity for conventional damascene copper interconnects. This presentation
looks at process and integration-level inflections that promise to limit RC delay increase while
also achieving void-free gap fill in nano-scale interconnects.