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FIG. 3. Enlarged SEM images of interface shown in Fig. 2͑b͒ ͑a͒ top inter-
face, ͑b͒ bottom interface.
FIG. 2. ͑a͒ Schematic of sandwich structure, ͑b͒ cross-section of the sample
reflowed at 200 °C for 600 s using eutectic SnPb solder on Cr/Cu/Au film.
posed Ti or Cr surface, it exerts a lifting force to the
Cu6Sn5 grains due to gravity or density difference. When the
grains transform to spheroids which have a nonwetting con-
tact angle ͑180°͒ to the Ti or Cr surfaces, they may be lift up
from the bottom interface by the gravity force. Although the
detailed mechanism of spalling such as shape change of the
Cu6Sn5 grains and their wetting behavior on Ti or Cr sur-
faces remains to be studied, the gravity effect seems in
agreement with the observed asymmetric behavior.
On the wetting behavior of Cu6Sn5 on Ti or Cr surfaces,
we expect some adhesion between them since they are all
metals. Nevertheless, the dewetting of the intermetallic from
the metal surface is due to the total surface energy changes in
the shape change from a scallop to a spheroid. It includes
their interfaces with the molten solder.
The avoidance of ripening assisted spalling in product
may be achieved by locking the intermetallic compounds
with a ‘‘phased’’ region between Cr and Cu.11 In phasing Cr
and Cu, the crystallites of Cr and Cu become intermixed and
the intermetallics of Cu become locked into the Cr so that
they will not separate easily. Follow-on studies are planned
to examine intermetallic ripening on phased structures.
In summary, the spalling of the Cu-Sn compounds at the
solder interface on thin film metallization is an important
reliability issue of flip-chip technology. We have found that
the ripening among the Cu6Sn5 grains assisted the spalling.
Under the influence of gravity, the spalling tends to occur
predominantly at the bottom interface of a solder joint.
This research was supported by SRC contract No. 93-
NJ-356 and NSF contract No. DMR-9320769.
lops begins to change into spheroids. The change is accom-
panied by decreasing the contact area between the grains and
bottom metallization. This is because there is no more Cu;
the ripening becomes conservative. The smaller grains will
be dissolved into the bigger grains. The contact area de-
creases and it exposes the Ti or Cr surface to the liquid
solder, in turn, spalling will lead to more exposed surface as
shown in Fig. 1͑b͒. If the Ti and Cr surfaces are oxidized,
they can not be wetted by the solder. It can present a serious
dewetting problem and the interface will be vulnerable to
mechanical failure. In the earlier report on solution-assisted
spalling by Berry et al.7 no ripening reaction among the
Cu6Sn5 grains was mentioned. We show that it is the conser-
vative ripening which dissolves the smaller grains and results
in spalling. We have observed the same type of spalling in
the reflow of solder on the Cr/Cu/Au films.
In the face-to-face samples of two wafers with a solder
joint in between them, the schematic in Fig. 2͑a͒ shows the
sandwiched structure while the micrograph in Fig. 2͑b͒
shows the cross-section of a reacted sample. The small ͑ϳ0.5
mg͒ solder disk with a thickness of about 120 m was sand-
wiched by two wafers and the wafers were supported by
spacers with the same thickness to maintain the spacing. The
cross-section of the sandwich was polished using SiC paper
and alumina powder, and a light etching was performed us-
ing a mixture of 5% HCl in methanol to delineate the inter-
facial structure of the solder joint.10 Figures 3͑a͒ and 3͑b͒ are
the enlarged micrographs of the top and bottom interfaces of
the joints. They clearly show an asymmetric spalling behav-
ior of the two solder interfaces. After 10 min reflow at
200 °C, although a severe spalling has already occurred at
the bottom interface, the Cu-Sn compounds at the top inter-
face do not show any spalling. Because of the selective re-
action of Cu with Sn, the composition of solder next to the
Cu-Sn compounds will be enriched in Pb. Therefore, there is
a concentration gradient of Pb in the molten solder to mix the
solder. However, when the molten solder flows to the ex-
1 Semiconductor Industry Association, Semiconductor Technology Work-
shop Working Group Reports ͑Semiconductor Research Cooperation, Re-
search Triangle Park, NC, 1992͒.
2 R. R. Tummala, E. J. Rymaszewski, Microelectronics Packaging Hand-
book ͑Van Nostrand Reinhold, New York, 1989͒.
3 D. Seraphim, R. Lasky, and C. Y. Li, Principles of Electronic Packaging
͑McGraw-Hill, New York, 1989͒.
4 L. J. Fried, H. Havas, J. S. Lechaton, J. S. Logan, G. Paal, and P. A. Totta,
IBM J. Res. Dev. 26, 362 ͑1982͒.
Appl. Phys. Lett., Vol. 68, No. 16, 15 April 1996 Kim, Tu, and Totta 2205
130.133.66.132 On: Thu, 27 Nov 2014 14:11:34