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Enabling wafer thinning using a glass carrier
By Julia Brueckner, Andreas Gaab, Steven Lin, Erica Chang, Toshihiko Ono, Varun Singh, Jay Zhang [Corning Incorporated]
and Sebastian Tussing, Walter Spiess [SÜSS MicroTec]
W afe r t h i n n i ng is a n
industry trend driven by
functional requirements
or form factor considerations. For example,
3D stacked memory uses silicon (Si) that
is thinned to <50µm to enable through-
silicon via (TSV) interconnection.
Insulated-gate bipolar transistor (IGBT)
chips rely on very thin wafers for vertical
structural realization. Many components
used for mobile devices are thinned before
packaging to accommodate the height
constraints imposed by design or aesthetics.
When the final wafer thickness is greater
than 100µm, backgrinding tapes are
typically used to support the wafer during
the thinning process. Thinning beyond this
thickness often necessitates the use of a
more rigid support, such as a carrier wafer.
Wafer thinning is often accompanied
by post-thinning processing that happens
at elevated temperatures, e.g., metal or
dielectric deposition. Differences in the
coefficient of thermal expansion (CTE) of
the carrier and that of the wafer can cause
shape distortion, resulting in undesirable
consequences such as lithography errors, or
even wafer breakage. For convenience, we
use the term warp in this article to describe
shape distortion.
An ideal carrier wafer for wafer thinning
should have a CTE matched to that of the
wafer to be thinned. In this article, we will
also discuss other levers that may be used to
minimize shape distortion during thinning
and post-thinning processing.
This article will explain why glass is
an ideal carrier material. We will also
demonstrate why glass carrier wafers are
not only ideal for laser debonding, but that
they can also be used with automated,
mechanical debonding tools.
What impacts wafer warp?
We begin by first developing the
fundamental understanding of what
impacts wafer warp. In a previous article
in this journal [1], we showed a simplified
formula that can be used to estimate bi-
layer warp as a function of material and Figure 1: Warp as a function of ΔCTE, carrier Young’s modulus, and carrier thickness.
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