Diffusion soldering fundamentals and application
Transcript of Diffusion soldering fundamentals and application
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Diffusion solderingfundamentals and application
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Solder IP
Conventional soldering
Solders act by:
- wetting the metal surfaces forming the joints,
- flowing between these surfaces filling the space between them,
- metallurgically bonding to the surfaces when solidified.
Soldering: joining process below 425 oC using filler metals
(solders) having melting temperatures below those of base metals
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Conventional soldering
Substitutes for Sn-Pb solders
Sn-based multicomponent alloys with alloying elementssuch as Bi, In, Ag and Zn
Directive 2002/95/EC - New electrical and electronic
equipment should be free of lead and other hazardous
substances by July 1st, 2006.
WEEE 2002/96/EC - Waste Electrical and Electronic
Equipment (WEEE) – deadline 2008
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Operating temperature of many electronic devices built on silicon
carbide and III-V compound semiconductors exceeds 350 oC (jet
engines, nuclear reactors, geothermal walls, automotive electronics,
industrial robots, and space electronics).
Miniaturization of components and contact areas in electronic
packaging increase the specific load of contacts due to heat dissipation
(chip resistors and resistant heating elements).
Challenges for new joints
IBM: First a solution of the interconnection problem;
Then everything else
Limitation
Service temperature: 60-100 C below soldering temperature
(220-260 C for Sn-Pb solders)
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High temperature stability:~2 to 3 fold higher than thefabrication temperature
High mechanical strength
Small energy consumptiondue to low fabrication tem-perature
Environmentally friendly
Reduction in size and cost
No high temperature expo-sure of other circuit ele-ments
High temperature stable con-tacts of resistive heaters forthick-film hot plates, resistiveelements for gas sensors
Selective-area sealing and co-mplete package sealing of mi-crocircuits
Development of packages foroptoelectronics and othermicrocircuit application
Wafer-to-wafer joining, flip-chip joining, 3D integrationetc.
Producing metal-polyethyleneinterconnection
Need for a new lead-free joining technology
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100% HM
100% LM
Co
nce
ntra
tion
trian
gle
LM
HMa
HM
LM
HMHM LMb
time
Tj=const., p=const.
IP1
c
IP2 IP1
d
eIP2
(HM)f
Tj
IP2
IP1
(HM)
LMHM
CLCSC2 C1C3
Tm
HM- high-melting component (substrate)
LM- low-melting component (solder)
IP- intermetallic phase
(HM)- solid solution of LM in HM
Tj- joining temperature
Tm- melting temperature of LM
Diffusion Soldering
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The diffusion soldering should be distinguished fromthe diffusion brazing. Although both processesinvolve the same bonding mechanism, the solidsolution of LM in HM is ultimately formed duringbrazing in the interconnection area instead of theintermetallic phase. It also means that proces isperformed at such temperatures or for such systemswhere there is no intermetallic phases.
The term transient liquid phase diffusion bonding(TLP) is also frequently used to describe the joiningprocess involving isothermal solidification. However, itis also claimed, that no interface remains after the TLPbonding operation, which resembles the diffusionbrazing rather than diffusion soldering.
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Conventional soldering
good joint filling
tolerance to surface preparation
Diffusion bonding
higher service temperature
smaller thermal expansion
mismatch stresses
Diffusion Soldering
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Potential candidates for diffusion soldering
interlayer substrate
solder’s materials
Al Ni
In Cu, Ag
Ni,Cu,AgSn
In-48 at.%Sn Cu
In-22 at.%Bi Cu
No. Element (at.%) TM
[oC]A B C
1 In(60.3) Bi(21.4) Sn(18.3) 61
2 In(78) Bi(22) --- 72
3 In(52) Sn(48) --- 118
4 In --- --- 156
5 Sn(84.8) Zn(15.2) --- 199
6 Sn --- --- 232
7 Al --- --- 660
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Cu/Sn/Cu interconnection
(Cu6Sn5)-hexagonal – 415 oC
e(Cu3Sn)-orthorombic - 676 oC
(Cu10Sn3)-hexagonal – 642 oC
d(Cu41Sn11)-cubic – 586 oC
600
400
200
800
1000
1200
0 10 20 30 40 50 60 70 80 90 100
Atomic Percent TinCu Sn
(Sn)
(Cu)
L
e
676°C
415°C
227°C
d
Te
mp
era
ture
º C
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Cu/Sn/Cu interconnection
S. Bader, W. Gust, H. Hieber, Acta Metall. Mater. 43, 329
(1995)
6Cu+5Sn(l) Cu6Sn5
Cu6Sn5 5Sn(l) Cu3Sn
Cu6Sn5 + 9Cu 5 Cu3Sn
a
Cu
Si
e
1 min
c10 m
LM
Cu
Cue
e
20 min
10 m
LM
10 m
LM
b
Cu
Si
e
5 min
240 C eutectic Pb-Sn- 183 C
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S. Bader, W. Gust, H. Hieber, Acta Metall. Mater. 43, 329 (1995)
Cu/Sn/Cu interconnection
Tensile test
When both IPs presentstrength twice larger than for pure Sn (18 MPa)
DEMAND FOR ELECTRONIC INDUSTRY: Rm = 3-5 MPa
Thermal cycling
-45 oC/0.5 h +125 oC/0.5 h
5 s
5 s
Cu/1.5 m Sn/Cu – 5 min at 330 oC
For more than 300 cycles and p=0.8 MPa
Rm = 27 MPa
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X.J. Liu, H.S.Liu, I. Ohnuma et. al.
Experimental determination and thermodynamic calculation of the phase equilibria in the Cu-In-Sn system
J. Electronic Mater. 30 (2001) 1093-1103
x(I
n)
x(Sn)
0.0
0.2
0.3
0.5
0.7
0.9
0.0 0.2 0.4 0.6 0.8 1.00 0.2 0.4 0.6 0.8 10
0.2
0.4
0.6
0.8
1
x(Sn)
x(In
)
Cu
In
Sn
Liquid+
Liquid
Fcc_A1
+eFcc+d'
+
+L
iqu id
d+
d+
+ e
e+Cu3Sn
-CuIn
Fcc
+ d
d-CuIn
d+Fcc+Cu77InSn23
Fcc+Cu77InSn23+d'
ed
'
dd '
dd'+e
Fcc+ed'
'+d
300 0C
d Cu7In3
Cu11In9
Liquid
dCu6Sn5
++liquid
Cu6Sn5
300 C
X(I
n)
X(Sn)
0.0
0.2
0.3
0.5
0.7
0.9
0.0 0.2 0.4 0.6 0.8 1.00 0.2 0.4 0.6 0.8 10
0.2
0.4
0.6
0.8
1
X(Sn)
X(In)
Cu
In
Sn
Liquid
-CuIn+Liquid
Liquid++d+
+ e
Fcc
+ d+ d
'
e-Cu3Sn
Fcc+ d'
Fcc_A1 Bct_A5
-CuIn
'-CuIn
d-CuIn
d+d'
Fcc+d
+Bct+e +
++BctFcc+e+d'
e+d+d
'
d
Liq
ui
d+
+
e+d'
200 0C
-InSn
Liquid+
d Cu7In3
Cu2In
Cu11In9
Liquid + +
Cu6Sn5 + Liquid
X(I
n)
X(Sn)
0.0
0.2
0.3
0.5
0.7
0.9
0.0 0.2 0.4 0.6 0.8 1.00 0.2 0.4 0.6 0.8 10
0.2
0.4
0.6
0.8
1
X(Sn)
X(In)
Cu
In
Sn
Liquid
-CuIn+Liquid
Liquid++d+
+ e
Fcc
+ d+ d
'
e-Cu3Sn
Fcc+ d'
Fcc_A1 Bct_A5
-CuIn
'-CuIn
d-CuIn
d+d'
Fcc+d
+Bct+e +
++BctFcc+e+d'
e+d+d
'
d
Liq
ui
d+
+
e+d'
200 0C
-InSn
Liquid+
200 C
[Cu6(Sn,In)5]
d[Cu41(Sn,In)11]
e[Cu3(Sn,In)]
d[Cu7(In,Sn)3] ~ 613 oC
[Cu2(In,Sn)] ~ 391 oC
Cu/In-Sn/Cu interconnection
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Cu
phase
(scallop)
In-Sn solder
10 m
5 m
coarse-grained
fine-grainedCu
Cu
phase
phase
10 m
Cu/In-48Sn/Cu interconnection - [Cu6(Sn,In)5] phase
200 °C / 10 h
180 °C / 3 h
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Cu/In-48Sn/Cu interconnection- [Cu6(Sn,In)5] and d[Cu41(Sn,In)11] phases
0.5 m
phase
coarse-grained
phase
fine-grained
200 nm
Cu
d
d
d
In L Sn L
Cu K
Cu
phase
500 nm
1
200
131
30110
0001
4
0001
1230
[013] zone axis [2110] zone axis [5410] zone axis
Lp. Cu In Sn phase
1 99.4 0.2 0.4 Cu
2 71.6 16.6 11.8 d
3 53.4 21.4 25.3 (fine)
4 55.8 19.7 24.6 (coarse)
d[Cu41(Sn,In)11]
200 °C / 60 h
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Cu
CuCud phase
20 m
Cu Cu Cu phase
phase
d
phase
In-Sn
solder
d phase
20 m 50 m
200 C / 24 h 300 C / 10 min
300 C / 3 days
x(I
n)
x(Sn)
0.0
0.2
0.3
0.5
0.7
0.9
0.0 0.2 0.4 0.6 0.8 1.00 0.2 0.4 0.6 0.8 10
0.2
0.4
0.6
0.8
1
x(Sn)x(
In)
Cu
In
Sn
Liquid+
Liquid
Fcc_A1
+eFcc+d'
+
+L
iqu id
d+
d+
+e
e+Cu3Sn
-CuIn
Fcc
+ d
d-CuIn
d+Fcc+Cu77InSn23
Fcc+Cu77InSn23+d'
ed
'
dd '
dd'+e
Fcc+ed'
'+d
300 0C
X(I
n)
X(Sn)
0.0
0.2
0.3
0.5
0.7
0.9
0.0 0.2 0.4 0.6 0.8 1.00 0.2 0.4 0.6 0.8 10
0.2
0.4
0.6
0.8
1
X(Sn)
X(In)
Cu
In
Sn
Liquid
-CuIn+Liquid
Liquid++d+
+ e
Fcc
+ d+ d
'
e-Cu3Sn
Fcc+ d'
Fcc_A1 Bct_A5
-CuIn
'-CuIn
d-CuIn
d+d'
Fcc+d
+Bct+e +
++BctFcc+e+d'
e+d+d
'
d
Liq
ui
d+
+
e+d'
200 0C
-InSn
Liquid+
300 C
Cu/In-48Sn/Cu interconnection - d[Cu41(Sn,In)11] phase
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1 µm
Cu Sn In
57.8 32.5 9.7
59.3 28.1 12.6
62.3 18.7 19.0
64.7 12.2 23.1
Cu6(Sn,In)5
Cu2(In,Sn)
d+e
εd
Cu
0.1 m
Cu
Cu/In-48Sn/Cu interconnection - e[Cu3(Sn,In)] and d[Cu7(In,Sn)3] phases
0
20
40
60
80
100
0 50 100 150 200 250 300
odległość [nm]
skła
d c
hem
iczn
y [
at.
%]
Cu-delta
Sn-delta
In-delta
Cu-epsilon
Sn-epsilon
In-epsilon
distance
ch
em
ical
co
mp
os
itio
n
220 °C / 243 h
d
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x(I
n)
x(Sn)
0.0
0.2
0.3
0.5
0.7
0.9
0.0 0.2 0.4 0.6 0.8 1.00 0.2 0.4 0.6 0.8 10
0.2
0.4
0.6
0.8
1
x(Sn)
x(In
)
Cu
In
Sn
Liquid+
Liquid
Fcc_A1
+eFcc+d'
+
+L
iqu id
d+
d+
+e
e+Cu3Sn
-CuIn
Fcc
+ d
d-CuIn
d+Fcc+Cu77InSn23
Fcc+Cu77InSn23+d'
ed
'
dd '
dd'+e
Fcc+ed'
'+d
300 0C
a
b
c
d
ef
gh
i
j
k
d Cu7In3
e Cu3Sn
d Cu41Sn11
Cu6Sn5
Cu2In
48%Sn52%In
L
a
b
e
d
d
Cu
c
d-e
f-g
h
i-j
k
e ed
ed
ed d
0.1 m
d [Cu41(Sn,In)11]
[Cu6(Sn,In)5]
Clark J.B.: Conventions for plotting the
diffusion paths in multiphase ternary
diffusion couples on the isothermal
section of a ternary phase diagram,
Trans. Metal. Soc. AIME 227, (1963)
1250-1251.
Concentration of elements at points 1-13 across the joint [at.%],
SEM (EDX)
1 2 3 4 5 6 7 8 9 10 11 12 13
Cu 2 8 7 15 31 60 56 66 74 74 76 91 100
In 32 39 64 62 51 20 22 17 13 10 6 5 0
Sn 66 53 29 23 18 20 22 17 13 16 18 4 0
Cu/In-48Sn/Cu interconnection - diffusion path
300 °C / 6 h
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[Cu6(Sn,In)5] 180-220 °C
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d[Cu41(Sn,In)11]
d [Cu7(In,Sn)3] e [Cu3(In,Sn)]
300 -350 °C
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Temperature and
time of
production
Phases present in the joined area Shear strength [MPa]
200 C/3 hours [Cu6(Sn,In)5] and In-Sn solder 4.6
200 C/5 hours [Cu6(Sn,In)5] and In-Sn solder 7.1
200 C/3 days [Cu6(Sn,In)5] 11.2
250 C/3 hours [Cu6(Sn,In)5], d[Cu41(Sn,In)11], In-Sn solder 4.2
300 C/3 hours [Cu6(Sn,In)5], d [Cu41(Sn,In)11], In-Sn solder 4.7
300 C/5 hours [Cu6(Sn,In)5], d [Cu41(Sn,In)11], In-Sn solder 6.4
300 C/3 days d [Cu41(Sn,In)11] 28.5
Shear test at room temperature in Cu/In-48Sn/Cu joint
Shear test at elevated temperature in Cu/In-48Sn/Cu joint
Temperature
and time of
production
Phases present in the joined area Shear strength [MPa]
200 C/3 days [Cu6(Sn,In)5] 9.5 (test at 100 °C )
200 C/2 weeks [Cu6(Sn,In)5] and d[Cu41(Sn,In)11] 9.8 (test at 100 °C )
300 C/1 week d [Cu41(Sn,In)11] The fracture occurred in copper substrate.
Joint was not destroyed at 100 and 150 °C
300 °C/2 weeks d [Cu41(Sn,In)11] The fracture occurred in copper substrate.
Joint was not destroyed at 100 and 150 °C
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Te
mp
era
ture
º C
20 40 60 80
Atomic percent Ni
Cu+5at.%Ni/Sn/Cu+5at.%Ni interconnection
Cuiping Wang, Jinjin Zhu, Yong Lu,
Yihui Guo, and Xingjun Liu,
Journal of Phase Equilibria and
Diffusion Vol. 35 No. 1, 2014.
C. Schmetterer, H.
Flandorfer, CH. LueF,
A. Kodentsov, H. Ipser
Cu-Ni-Sn: A Key
System for Lead-Free
Soldering Journal of
Electronic Materials,
Vol. 38, No. 1, 2009.
240 ºC
[(Cu1-xNix)6Sn5] e[Cu3Sn]
KPMI Fall Meeting, 13-14 November 2014, Yeosu, South Korea
Paweł Zięba, Anna Wierzbicka-Miernik Diffusion soldering- fundamentals and application
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Cu+5at.%Ni/Sn/Cu+5at.%Ni interconnection [(Cu1-xNix)6Sn5]
250°C / 2 min 250°C / 5 min
250°C / 10 min 250°C / 15 min
Lp. Cu at.% Sn at.% Ni at.% phase
1 95.1 0.0 4.9 (Cu,Ni)
2 0.0 100.0 0.0 Sn
3 50.7 45.1 4.2
50 µm
Cu+5at.% Ni
Cu+5at.% Ni
(Cu1-xNix)6Sn5
Sn
1
2
3
50 µmCu+5at.% Ni
(Cu1-xNix)6Sn5
Sn
260°C / 10 minafter selectively etching away the Sn
e[Cu3Sn] WAS NOT OBSERVED
50 µm
50 µm 50 µm
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250°C / 10 min
250°C / 60 min
Cu/Sn/Cu vs. Cu+5at.%Ni/Sn/Cu+5at.%Ni joints
Cu/Sn/Cu Cu+5at.%Ni/Sn/Cu+5at.%Ni
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Cu+5at% Ni
substrate
Reaction zone
1 µm
Cu+5at%Ni
Reaction zoneSn L Cu K Ni K
400 nm
Reaction zone
1
2
0002
2110
[0110] Cu6Sn52
0111
[1210] Cu6Sn51
1101
250 °C / 60 min
Cu+5at.%Ni/Sn/Cu+5at.%Ni interconnection [(Cu1-xNix)6Sn5]
Ni enrichment
zone-possible
reason that no
e[Cu3Sn] formed
KPMI Fall Meeting, 13-14 November 2014, Yeosu, South Korea
Paweł Zięba, Anna Wierzbicka-Miernik Diffusion soldering- fundamentals and application
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in general: x=ktn
the widith of the
phase interlayer
Growth rate constant
time
* for n=0.5: parabolic growth,
controlled by the volume diffusion
* for n=1: linear growth,
controlled by the chemical
reaction at the phase boundary
Rate controlling factor of IPs growth
There are two important advantages of linear growth from the
diffusion soldering process point of view:
1. faster formation of the intermetallic phase,
2. shorter time needed to create a joint.
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S. Bader, W. Gust, H. Hieber, Acta Metall. Mater. 43, 329 (1995)
Growth kinetics and ε phases in Cu/Sn/Cu joint
phase n
240 C 0.21
300 C 0.26
ε phase n
240 C 0.45
300 C 0.49
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Growth kinetics and d phases in Cu/In-48Sn/Cu joint
phase n
180 C 0.40 ± 0.02
200 C 0.20 ± 0.03
220 C 0.31 ± 0.09
d phase n
300 C 1.08 ± 0.04
325 C 1.10 ± 0.08
350 C 0.91 ± 0.04
d at 300 C
0
4
8
12
16
20
0 0,2 0,4 0,6 0,8 1 1,2
t [h]
x [
um
]
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S=ktn
the area of the phase
Growth rate constant
time
* for n=1: controlled by the volume
diffusion
* for n<1: controlled by the grain
boundary diffusion
Rate controlling factor of IPs growth
in Cu+5at.%Ni/Sn/Cu+5at.%Ni joints
Wierzbicka-Miernik A., Miernik K., Wojewoda-Budka J., Filipek R., Lityńska-Dobrzyńska L., Kodentsov A., Zieba P. (2013): Growth kinetics of the intermetallic phase in diffusion-soldered Cu+5at.%Ni)/Sn/(Cu+5at.%Ni) interconnections, Materials Chemistry and Physics 142, 682-685.
KPMI Fall Meeting, 13-14 November 2014, Yeosu, South Korea
Paweł Zięba, Anna Wierzbicka-Miernik Diffusion soldering- fundamentals and application
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Growth kinetics phase in Cu+5at.%Ni/Sn/Cu+5at.%Ni joint
phase n coeficient
240 C 0.27 ± 0.08
250 C 0.24 ± 0.08
260 C 0.15 ± 0.09
n<1: grain boundary diffusion
at 250 C
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The proces can be even more efficient if:
• the growth kinetics of IPs is controlled either by chemical
reactions at the interfaces or grain boundary diffusion
processes,
• The substrate is doped with other elements preventing
growth of undesired IPs like ε-Cu3Sn and accelerating
growth kinetics due to change of formation mechanism of
IPs (see (Cu1-xNix)6Sn5.
The diffusion soldering is a novel interconnection technology. It
is characterized by the low joining temperature (comparable
with Pb-Sn eutectic solders) combined with the service
temperature, which can be higher by several hundred degrees
than the joining temperature. For these reasons, diffusion
soldering is a very attractive method for certain types of
electronic application.
Conclusions