process development of a novel wafer level packaging with tsv applied in high-frequency range...
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REVIEW PAPER
Process development of a novel wafer level packagingwith TSV applied in high-frequency range transmission
Xiao Chen • Jiajie Tang • Gaowei Xu •
Le Luo
Received: 4 September 2012 / Accepted: 6 December 2012 / Published online: 18 December 2012
� Springer-Verlag Berlin Heidelberg 2012
Abstract The process development of a novel wafer level
packaging with TSV applied in high-frequency range
transmission is presented. A specially designed TSV
structure (a core TSV and six shielding TSVs) is adopted to
connect the components on different sides of the high-
resistivity silicon wafer. And the microstrip line in the
microwave monolithic integrated circuit is used to transmit
high-frequency signal in packaging structure together with
the low permittivity intermediate dielectric polymer, ben-
zocyclobutene. The TSV fabrication process and the multi-
layer interconnection is illustrated in details. The electrical
measurement result of the microstrip lines connected by
TSVs reveals the resistances within 0.719 X, a return loss
better than 23.8 dB and an insertion loss better than
2.60 dB from 14 to 40 GHz.
1 Introduction
Continuous increase in demand for product miniaturization,
high package density, high performance and integration of
different functional chips has lead to the development of
three dimensional (3D) packaging technology, in which
multi-chips are assembled by vertical interconnects by
through silicon vias (TSV) at wafer level packaging. 3D
packaging has higher packaging density, shorter intercon-
nection, lower noise and lower profile (Jang et al. 2007;
Beica et al. 2008; Kumagai et al. 2008). In order to achieve
extremely high-density integration, system-in-package (SiP)
encounters the challenges in package size, process, thermal
and electrical performances (Tummala and Swaminathan
2008). The 3D packaging technology with TSV may offer an
optional solution to this problem.
Using the TSV interconnection on SiP, the multi-layer
interconnection and the active components such as MMIC
chips can be separately integrated on each side of the sil-
icon substrate. Because the MMIC chips may take the risk
of the failures in the fabrication processes (Corrosion,
release and high-temperature annealing) when they are
integrated into the substrate. Owing to TSV, the MMIC
chips can be integrated on one side of the wafer after these
fabrication processes and the assembling of other devices
on the other side. Not only the shortest vertical connec-
tions, less loss and parasitic effect can be ensured, but also
the failure and reliability problems can be greatly
decreased. Accordingly, the mass production of the sub-
strate with integrated active/passive devices, MEMS
devices and optoelectronic devices, etc. can be achieved in
advance. Accordance with the recent references (Ho et al.
2008; Lim et al. 2011; Kannan et al. 2011), some pre-
liminary work on the performance of the single TSV in
high-frequency range have been reported. However, the
aspect ratios (AR) of the TSVs fabricated in these papers
are relatively low (AR = 1–3). Moreover, the microwave
performances of the interconnection structure with TSVs
together with the application of different active compo-
nents such as the MMIC chips assembled in the silicon
substrate based SiP are not involved in the previous work.
X. Chen (&) � J. Tang � G. Xu � L. Luo
State Key Laboratory of Transducer Technology,
Shanghai Institute of Microsystem and Information Technology,
Chinese Academy of Sciences, Shanghai, China
e-mail: [email protected]
L. Luo
e-mail: [email protected]
X. Chen � J. Tang
Graduate School of Chinese Academy of Sciences,
Beijing, China
123
Microsyst Technol (2013) 19:483–491
DOI 10.1007/s00542-012-1712-9
In this paper, a wafer-level SiP structure fabricated
between both sides of the silicon wafer using high AR
TSVs (AR = 7) is presented. A specially-designed TSV
structure (a core TSV and six shielding TSVs) through the
silicon can achieve the inter-side connection of the two
sides of the substrate to transmit the high frequency signal
from the MMIC embedded in the silicon substrate to the
other side of the wafer. To reduce the transmission loss of
TSV in high-frequency, the high-resistivity silicon is
adopted as the substrate with BCB as the intermediate
dielectric layer. Besides, the fabrication steps including the
TSV formation and the BCB process on two sides of wafer
are discussed in details. This new technology of two sides
fabrication is a powerful platform for the high-density
integration of microwave application in the complicated
3D package modules.
2 Design and process flow
The special constructure of microwave transmission con-
tains a microstrip line (MSL) on the MMIC embedded in a
high-resistivity silicon substrate, Cu-TSV, BCB/metal
multilayer interconnection, L1 and L2 (the MSL on the
packaging substrate). Figure 1a, b shows the top and cross-
sectional views of the interconnection configuration.
MMIC is used to achieve planar interconnection with BCB
as the intermediate dielectric layer. Similar to the coaxial
line, the structure is composed of a core TSV and six
shielding TSVs. The core TSV transmits signal, and the
shielding TSVs are around the core and connected to the
ground. According to the simulation results, the perfor-
mance of the proposed structure is very close to the coaxial
line case. The TSV (40 lm in diameter with 280 lm in
depth) with vertical profile is fabricated. To further
improve the high-frequency performance, high-resistivity
silicon (3,000–4,000 X cm) is selected as the substrate
material. BCB is an excellent dielectric material with low
permittivity (2.65) and low dissipation factor (0.0008)
(Ding et al. 2009; Seok et al. 2006). It is utilized for its
good chemical resistance, high planarization, low moisture
absorption and photo-sensitive characteristic as well.
The fabrication steps including the TSV formation [the
blind-via etching, seed layer deposition, blind via filling
and chemical mechanical polish (CMP) of Cu] and the
BCB process on two sides of wafer are discussed in details.
Figure 2 shows the whole designed flow of the intercon-
nection method of SiP. First, a cavity is formed for MMIC
embedding by KOH etching (Fig. 2a). After a SiO2 layer
(2 lm thick) is deposited as hard mask, the blind vertical
vias are etched to the desired depth by Bosch etching
(Fig. 2b). The SiO2 mask is removed and a new SiO2 layer
(2 lm thick) is deposited by thermal oxidation to cover the
sidewalls of vias for electrical isolation and the whole
Fig. 1 The top and cross-
sectional views of the
interconnection configuration:
a top view; b cross-section view
484 Microsyst Technol (2013) 19:483–491
123
surface besides the KOH cavities. And the vias are then
coated by Ti as adhesion layer and Cu as seed layer by
electron beam evaporation (Fig. 2c). In addition, a photo-
resist thin layer, which is a mask, is deposited only in the
KOH cavities by the spray photoresist technology, thus the
Ti/Cu layer cannot be deposited in the cavities. In the Cu
electroplating process, the blind vias are filled without
defect (Fig. 2d). After the electroplating, the Cu over
burden on the top of wafer is removed by CMP and the
wafer backside is thinned down to expose the backside of
the TSVs (Fig. 2e). Afterwards, a new seed layer of
TiW/Au (50 nm/300 nm) is sputtered for the multilayer
interconnection. Then the ground layer is fabricated by
electroplating (Fig. 4f). And a BCB layer with a thickness
of approximately 25 lm is deposited followed by BCB
exposure and development. The tapered via-holes take
shape through BCB (Tang et al. 2011). Then a Cr/Au
(50 nm/300 nm) seed layer is deposited on the wafer sur-
face by the magnetron sputtering. Following the lithogra-
phy process, inter-layer connection and L2 are patterned
and electroplated to 3 lm. Thus, the tapered hollow vias
are formed. After removing the photo-resist, the seed layer
is etched by the ion-beam (Fig. 4g) (Tang et al. 2011).
After that, the wafer is turned over. An MMIC chip is
embedded and stuck on the bottom of the trench with silver
paste. After leveling, the embedded wafer is baked in a
150 �C oven for 1 h to solidify the Ag paste (Fig. 4h)
(Tang et al. 2011). A layer of photo-BCB with a thickness
of approximately 25 lm is spin-coated, placed horizontally
for planarization and then baked. (Fig. 2i). Then the
BCB/metal interconnection is fabricated (Fig. 2j) (Tang
et al. 2011).
3 Key technologies of fabrication
In this section, the key technologies, such as the seed layer
deposition into deep vias, Cu electroplating with no voids
and the BCB process will be discussed in details.
3.1 Seed layer deposition into deep blind-vias
The silicon wafer is etched using Bosch deep reactive ion
etch process for a blind vertical via with 40 lm diameter
and 280 lm depth in surface technology system (Fig. 3).
And a SiO2 layer is deposited by thermal oxidation for
electrical isolation, and the vias are then coated by the
adhesion layer and seed layer.
Fig. 2 Process flow of the
interconnection in SiP
Fig. 3 The silicon substrate
with the blind vias and the
trench
Microsyst Technol (2013) 19:483–491 485
123
In this study, the electron beam evaporation technology
is developed to deposit barrier and seed layers into deep
vias. To improve the adhesion and step coverage of the
layers into deep microvias, a deposition program composed
of heating silicon and multi-step evaporation method is
used in evaporation process. And a 0.2 lm titanium layer
as barrier and adhesion layer and a 0.5 lm copper seed
layer are deposited into the vertical deep vias by electron
beam evaporation carried on Sccot-380 equipment. The
electron beam evaporation parameter is summarized in
Table 1. The layer deposition performed on vertical vias
shows a depth of 280 lm and a diameter of 40 lm. The
profile of the thin-film distribution is analyzed from cross-
section of the sample by SEM (Hitachi-S4800). As shown
in Fig. 4, the Ti/Cu layer is very thin on the sidewall of the
deeper vertical vias, and the sidewall is rough due to
BOSCH etching process. The thin seed layer also forms a
continuous conductive layer with thickness ranging from
96 to 320 nm on the vertical sidewall, which remains
acceptable for the copper electroplating of the blind vias.
3.2 Cu electroplating for deep blind-vias
To realize the copper fast-filling without voids into deep
microvias, in this study we use a commercial electroplating
solution (Model: UTP SYS-3320) including three electro-
lyte additives (accelerator, suppressor or leveler) from
Sinyang. In general, the accelerators enhance copper
deposition while the suppressors and levelers suppress the
deposition. The accelerators have much higher diffusion
rates than suppressors and levelers and they are distributed
uniformly in the high AR fast-filling case. The suppressors
and levelers are distributed mostly at the top region of deep
via, only a little at the bottom. Therefore, faster deposition
at the bottom of deep via while suppressing the deposition
at the top is needed for achieving void free filling (Fang
et al. 2011; Tsui et al. 2009), as indicated in Fig. 5.
In the electroplating process, the ultra-sonic treatment is
firstly used to fill the deep via with copper electroplating
solution. Subsequently, the electroplating process for verti-
cal deep via is developed with Cu plating solution. The
current density of the power source is the most important
parameter for improving the via filling quality. After Cu
electroplating into the blind vias, the void appears at the
bottom or the middle of vertical deep via as shown in Fig. 6a, b.
In order to avoid voids in the via, a multi-step electroplating
process is used. First, a low current density (0.8 ASD) is
adopted to realize a most fully filling at the bottom of vias
Table 1 Parameters of the electron beam evaporation
Variable Value
Evaporation rate of Ti 0.2 nm/s
Evaporation rate of Cu 1/3/5 nm/s
Evaporation time of Cu 50/50/60 s
Si temperature 200 �C
Chamber pressure 7.5 9 10-7–8.9 9 10-7 torr
Silicon rotational speed 15 rpm
Fig. 4 SEM images of barrier
layer (Ti) and seed layers (Cu)
deposited in the blind via
486 Microsyst Technol (2013) 19:483–491
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and the plating time is 2 h. Secondly, the electroplating
current density and plating time are 1.0 ASD and 2 h,
respectively, resulting in a fully filling in the middle. In the
end, the electroplating current density and plating time are
also 1.2 ASD and 1.5 h. In Fig. 6c, the deep via is filled with
copper without any defect (voids or seams).
A thick layer of Cu overburden (15–20 lm) is plated on
the wafer surface. The CMP with a commercial slurry
(Model: STSV2000) from Anji is developed for removal of
the copper. The top image of the vias after CMP is shown
in Fig. 7. Subsequently, the wafer backside is thinned
down to expose the backside of the TSV and the fine
grinding is then used for planarization. After the CMP
process, the Cu of both sides of the TSVs columns is easily
oxidized to form Cu oxidation. Followed by BCB/metal
multilayer interconnection preparation, the Cu oxidation is
etched by 0.5 lm thick to expose Cu by the ion-beam
process. And two new seed layers of TiW–Au are depos-
ited on both surfaces of the wafer and then the Au layers
are electroplated to 3 lm thick in case of the Cu oxidation
in the lateral process.
3.3 The BCB of process on the two sides of wafer
In this work, the photosensitive BCB process on the two
sides of wafer is used. The process flow of BCB includes
BCB spin-coating, pre-baking, lithography, pre-develop-
ment baking, development, post-development baking,
curing (Tang et al. 2011). On the first side of wafer, the
BCB layer is spun at 1100 rpm for 30 s and a thickness of
about 25 lm BCB was achieved. And then the pre-baking
process is performed on an enclosed hotplate for 90 s at
110 �C with flowing nitrogen. And the wafer is exposed to
deep UV light with the exposure dose ranges from 1,800 to
2,000 mJ/cm2. After UV exposure, the wafer is immersed
in 40 �C BCB developer (DS3000) following the pre-
develop baking. The last step was a hard cure for 60 min in
a nitrogen atmosphere.
To adapt to the two sides interconnection of wafer, some
adjustments of process should be made on the other side of
the wafer. Both the baking and the cure which use a heating
plate in conventional BCB process are replaced by oven
baking in the atmosphere of nitrogen to prevent the structure
on the backside from being destroyed. The temperature and
the time of the pre-baking step are 120 �C and 12 min,
respectively. And those of pre-development baking and post-
Fig. 5 Model of the absorption of electrolyte additives
Fig. 6 Cross-section image of vias with different current density and
plating time
Fig. 7 The top image of the core TSV and six shielding TSVs after
CMP
Microsyst Technol (2013) 19:483–491 487
123
development baking are set to be 120 �C and 5 min, sepa-
rately. Since the BCB layers fabricated on the first side of the
wafer will be cured again, the cure temperature on BCB of
the first side could be reduced to 180 �C. And in the last BCB
cure step on the other side, the cure temperature will be rise
back to 210 �C in the standard BCB soft cure process. In
addition, the silicon is very fragile on the BCB process and
can thus not be handled with standard semiconductor
equipment for subsequent process. In order to overcome this
issue, the TSV wafer is mounted temporary on support wafer
for dry etching, lithography and electroplating. In the tem-
porary bonding process, the photoresist (Model: Shipley
6112), as the bonding material, is spun on a support wafer.
Then the TSV wafer is bonded to the support wafer on a
heating plate at 120 �C for 2 min. The method for debonding
is that the bonded wafers are immersed in the organic solu-
tion of stripping photoresist (acetone). The debonding tem-
perature is the room temperature.
In the process of BCB spin-coating, BCB accumulate or
hole occurs on the edge of TSV as shown in Fig. 8. The
nonuniform coating of BCB may arise from the difference
in height between the top of the TSVs and the substrate
silicon in the process of spin-coating. To avoid the non-
uniform, the BCB is spined on the wafer until BCB dripped
down covers the TSVs, and the standing time of wafer
coated by BCB is extended to 1 h. In addition, the BCB
accumulation also occurs in interval space between MMIC
chip and trench etched (Fig. 9a). The height of MMIC
embedded in trench and the depth of the trench need to be
accurately measured. If the height difference of MMIC in
the trench above the substrate silicon is less than 5 lm, the
BCB accumulation could be avoided (Fig. 9b).
4 Simulation and measurement results
The coaxial line structure through silicon substrate cannot
be achieved in the fabrication process. In this work, a
specially-designed TSV structure through the silicon,
which is composed of a core TSV and six shielding TSVs,
is used (Fig. 7). The core TSV transmits signal, and the
shielding TSVs are around the core and connected to the
ground. In the simulation of the microwave transmission
performance, the same MSL using one single TSV with no
shielding TSV and using coaxial line to achieve the inter-
side connection are also simulated and compared to the
results of the proposed structure. As shown as Fig. 10, the
performance of the proposed structure is very close to
the coaxial line case. Both the return loss is better than
30 dB from 18 to 30 GHz. The insertion loss of propose
structure is 0.55 dB at 24 GHz which is 0.04 dB larger than
the coaxial line case. However, the S21 of the case with no
shielding TSV is nearly 1 dB at 24 GHz. The microwave
transmission performance of the proposed structure is as
good as the case of the coaxial line and easier to be
fabricated.
The specimen of the proposed BCB/metal interconnec-
tion accompanied by TSVs for two sides connection is
fabricated and the Fig. 11 shows the photograph of the
front and back sides of the test vehicle whose cross-sec-
tional structure is shown in Fig. 1b. The test structure
includes the MSL in MMIC, TSV, L1 (the MSL on the
packaging substrate) and L2 (the MSL on backside of the
packaging substrate). The parameters of the structure are
listed in the Table 2. The electrical resistances and the
microwave transmission performance of the test vehicle
will be measured.
The resistances of the test vehicle structure are tested by
a Cascade-M150 probe-station. The theoretical resistance
is 0.52 X. The measured electrical resistance value is
within 0.719 X by Kelvin measurement. The measured
resistance is close to the theoretical resistance.
Fig. 8 BCB holes image on the edge of TSV
Fig. 9 BCB accumulate images on interval space between MMIC
chip and trench. a BCB accumulate, b BCB uniform after process
improved
488 Microsyst Technol (2013) 19:483–491
123
After the RF data are de-embedded, the microwave
transmission performance of the structure is measured by
Agilent 8722D network analyzer from 14 to 40 GHz. And
the measurement results are shown in Fig. 12. The mea-
surement results reveal a return loss better than 23.8 dB
and an insertion loss better than 2.60 dB. And the mini-
mum value of S21 is 1.42 dB. Especially in the range from
14 to 26.8 GHz, the return loss is better than 15 dB. And
the simulation curve of the S11 and S21 are shown as
Fig. 13. A difference of 1.5–2.5 dB of S21 between the
measurement and the simulation of the test vehicle is
observed in the measurement frequency range.
The relatively large loss may result from several rea-
sons. The BCB coating on the substrate is nonuniform and
its thickness is hard to be precisely controlled to be con-
sistent with the designed value (25 lm thick). And the
BCB thickness around the interior via is a bit thinner than
Fig. 10 The performance of the proposed specimen, the coaxial line
case and the no shielding via case. a The insertion loss; b The return
loss
Fig. 11 Photographs of the front and back sides of the test vehicle
Table 2 Parameters of the interconnection structure
Variable Value (lm)
Length of MSL 900
TSV diameter 40
Substrate thickness 280
Length of L1 350
Length of L2 50
Fig. 12 The measurement result of the microwave transmission
performance
Microsyst Technol (2013) 19:483–491 489
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25 lm thick in the other part of the surface, as shown in
Fig. 14. Moreover, the deviation in width of the transmis-
sion line is induced by the lithography inaccuracy. All
these will lead to the impedance mismatch of the trans-
mission line. Moreover, the relatively large loss may result
from the contact resistances, interlayer connections and the
negative effect caused by the BCB-covered auxiliary sili-
con wafer which is attached below the test wafer for
backside insulation in the measurement. This 3D inter-
connection method in the microwave subsystem integration
with MMIC chips will be improved in our future work.
5 Conclusions
A wafer-level system-in-packaging structure using through
silicon via (TSV) for integration on both sides of the Si
wafer is proposed and realized. BCB/metal multilayer
interconnection is used to achieve 3D integration on the
substrate, and a specially designed TSV structure is adop-
ted to connect the components on different sides of the
wafer through the substrate. The TSV fabrication process
and the multi-interconnection is illustrated in details. The
measurement of the interconnection structure are presented
to investigate the electrical resistances and high-frequency
performance. The measurement result reveals the resis-
tances is within 0.719 X and a return loss better than
23.8 dB and an insertion loss better than 2.60 dB from 14
to 40 GHz. This 3D interconnection method will be applied
in the microwave multichip module in our future work.
Acknowledgments This work is supported by National Major Fun-
damental Research Program of China (Grant No. 2009CB320207) and
National Science and Technology Major Project—Research, Devel-
opment and Industry of RDL/Embedding Wafer-Level Packaging and
High-Density Bumping Technology (No. 2011ZX02602). The authors
would also like to thank the support of Jiangsu Changjiang Electronics
Technology Co., Ltd, Shanghai Anji Microelectronics Co., Ltd. and
Shanghai Sinyang Semiconductor Materials Co., Ltd.
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