FROM C4 PbSn FLIP CHIP TO LEAD-FREE µBUMP FLIP ... - VeMet
FROM C4 PbSn FLIP CHIP TO LEAD-FREE µBUMP FLIP ... - VeMet
FROM C4 PbSn FLIP CHIP TO LEAD-FREE µBUMP FLIP ... - VeMet
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<strong>FROM</strong> <strong>C4</strong> <strong>PbSn</strong> <strong>FLIP</strong> <strong>CHIP</strong> <strong>TO</strong><br />
<strong>LEAD</strong>-<strong>FREE</strong> µBUMP <strong>FLIP</strong> <strong>CHIP</strong><br />
ERIC BEYNE<br />
“VIJF JAAR LOODVRIJ SOLDEREN”<br />
22 SEPTEMBER 2011<br />
TNO, EINDHOVEN<br />
© IMEC 2011
OUTLINE<br />
o Introduction: Flip chip Scaling<br />
o µbump interconnect<br />
o Improving Bond quality<br />
o Die stacking strategies<br />
o Wafer-level underfill<br />
o Conclusion<br />
© IMEC 2011 E.BEYNE 2
SCALING <strong>FLIP</strong>-<strong>CHIP</strong> INTERCONNECTS<br />
IMC<br />
100µm pad diameter<br />
150-200µm bump pitch<br />
40µm pad Ø<br />
60µm pitch<br />
20µm pad<br />
40µm pitch<br />
10µm pad<br />
20µm pitch<br />
- With solder joint scaling, the intermetallics formed by<br />
UBM solder interaction are of increasing importance<br />
- For the smallest flip chip pitches : only intermetallic<br />
compounds after solder bump reflow<br />
© IMEC 2011<br />
ERIC BEYNE 3
MICRO-BUMP JOINING<br />
Si<br />
Si<br />
Si<br />
M<br />
Si<br />
M<br />
Solder<br />
M<br />
Si<br />
M<br />
Solder<br />
M<br />
Si<br />
M<br />
IMC<br />
M<br />
M<br />
Solder - IMC<br />
Similar to flip chip interconnect:<br />
▸ Low temperature melting solder metal, UBM metals.<br />
However:<br />
▸ Entire solder volume is transformed into intermetallic compounds<br />
▸ Small dimension : no solder „ball‟, typically < 10m thick<br />
▸ Connection by thermo/compression-reflow method<br />
▸ Requires improved control and flatness of the solder “bumps”<br />
© IMEC 2011<br />
ERIC BEYNE 4
APPLICATION SPACE µBUMP JOINING<br />
‣ Si-Si face-to-face bonding<br />
‣ 2.5D integration:<br />
Si chips to Si interposers<br />
DRAM<br />
Logic<br />
‣ 3D integration : chip stacking with TSV<br />
© IMEC 2011<br />
ERIC BEYNE 5
OUTLINE<br />
o Introduction: Flip chip Scaling<br />
o Baseline µbump interconnect<br />
o Improving Bond quality<br />
o Die stacking strategies<br />
o Wafer-level underfill<br />
o Conclusion<br />
© IMEC 2011 E.BEYNE 6
BASELINE µBUMPING SCHEME: Cu/Sn<strong>TO</strong> Cu<br />
Baseline µbump scheme<br />
▸ Die 1: Cu/Sn (5/3.5 µm)<br />
▸ Die 2: Cu (5 µm)<br />
µBump Ø: 25 down to 7.5 µm<br />
µBump pitch: 40 down to 20 µm<br />
Cu/Sn bump<br />
5µm Cu<br />
3.5µm Sn<br />
5µm Cu<br />
Top Si die<br />
Bottom Si die<br />
‣ Smooth side wall for<br />
Cu and Sn<br />
‣ No residues after<br />
seed layer etch<br />
© IMEC 2011<br />
ERIC BEYNE<br />
7
DEMONSTRATION OF COLLECTIVE<br />
TRANSIENT-LIQUID PHASE µBUMP BONDING<br />
Bonding procedure:<br />
• Pick & place die on wafer by Flip Chip bonding Tool, at<br />
room temperature<br />
• Collective Bonding in Wafer Bonder @ 250ºC<br />
© IMEC 2011 ERIC BEYNE 8
SOLID METAL BONDING:<br />
CuSn INTERMETALLIC BONDING @ 150ºC<br />
Ф 25m bump, 40/15m<br />
pitch/spacing<br />
Top die<br />
(Cu/Sn bump)<br />
Bottom wafer<br />
(Cu bump)<br />
150°C/50MPa<br />
150C/150MPa<br />
150C/50MPa<br />
Ф 25m bump, 40/15m<br />
pitch/spacing<br />
with no-flow underfill<br />
© IMEC 2011 ERIC BEYNE 9
40 µm PITCH, Cu/Sn µBUMP DIE STACKING<br />
PTCM/N TEST <strong>CHIP</strong>S<br />
© IMEC 2011<br />
5x5mm PTCM,<br />
40 µm pitch<br />
µbumps,<br />
2 peripheral rows<br />
ERIC BEYNE<br />
8x8mm PTCN<br />
“landing”die<br />
Cu/Sn microbump samples:<br />
‣ 3.5 µm and 8µm thick Sn on 40µm pitch Cu bumps,<br />
100 µm thick Silicon<br />
‣ Si-Si assembly in BGA package and SMD on test board<br />
‣ Use of a no-flow underfill<br />
Package level reliability of TLP bumps demonstrated<br />
‣ >1800 temp cycles<br />
‣ >1000 hrs in electromigration tests<br />
‣ 96 hrs HAST<br />
PTCN/M stack wire<br />
bonded in BGA package<br />
10
Resistance [Ohm]<br />
Daisy chain Resistance (Ohm)<br />
Resistance [Ohm]<br />
Daisy chain Resistance (Ohm)<br />
Resistance [Ohm]<br />
Daisy chain Resistance (Ohm)<br />
THERMAL CYCLING 40 µm PITCH Cu/Sn<br />
µBUMP PTCM/N BGA ASSEMBLIES ON PCB<br />
180<br />
180<br />
THERMAL CYCLING (-45°C/125°C) – IN-SITU<br />
160<br />
140<br />
RESISTANCE MONI<strong>TO</strong>RING<br />
120<br />
In-situ measurement at 125°C<br />
170<br />
100<br />
80<br />
60<br />
40<br />
20<br />
8.0µm Sn bump DC<br />
3.5µm Sn bump DC<br />
160<br />
110<br />
In-situ R at 125°C<br />
0<br />
0 200 400 600 800 1000 1200 1400 1600 1800 2000<br />
Time (h) = # cycles Time -45°C/+125°C<br />
[h] = Cycles [#]<br />
In-situ resistance monitoring during<br />
30’ 45ºC/30’125ºC thermal cycling<br />
Cu/Sn microbump samples:<br />
▸ 3.5 µm and 8µm thick Sn on 40µm pitch<br />
Cu bumps, 100 µm thick Silicon<br />
▸ Use of a no-flow underfill (NCP)<br />
150<br />
3000 3100 3200 3300<br />
100<br />
90<br />
In-situ R @-45°C<br />
No failures up to 4000 cycles<br />
80<br />
2950 3050 3150 3250 3350<br />
© IMEC 2011<br />
ERIC BEYNE 11
AGEING BEHAVIOUR OF LOW T Cu/SnTLP<br />
µBUMP: VOID FORMATION<br />
• Shift over time from Cu 6 Sn 5 to Cu 3 Sn, due to the excess of Cu.<br />
• The difference in diffusion rates of Cu and Sn results in vacancies<br />
that aglomerate to form voids : Kirkendall voids.<br />
Initial state<br />
Cu<br />
Cu 3 Sn<br />
After ageing at 250ºC for 15’<br />
Cu<br />
Cu 3 Sn<br />
Cu 6 Sn 5<br />
Cu 3 Sn<br />
Cu<br />
Cu 6 Sn 5<br />
Cu 3 Sn<br />
Cu<br />
After ageing at 250ºC for<br />
45’<br />
Cu<br />
Cu 3 Sn<br />
Cu<br />
© IMEC 2011<br />
ERIC BEYNE 12
WHY FULL TRANSFORMATION <strong>TO</strong> IMC?<br />
When using low volume “mini-bumps” with excess Sn, the risk of<br />
electro-migration failure strongly increases<br />
EM reliability test comparison: 40 µm pitch Cu/Sn µbump packaged<br />
F2F chip assemblies on PCB<br />
Cu/Sn microbump samples:<br />
‣ 3.5 µm and 8µm thick Sn on 40µm pitch<br />
Cu bumps, 100 µm thick Silicon<br />
‣ Si-Si assembly in BGA package and SMD<br />
on test board<br />
‣ Use of a no-flow underfill<br />
EM test structure with build-in<br />
temperature monitor<br />
© IMEC 2011<br />
ERIC BEYNE<br />
13
No data<br />
WHY FULL TRANSFORMATION <strong>TO</strong> IMC?<br />
When using low volume “mini-bumps” with excess Sn, the risk of<br />
electro-migration failure strongly increases<br />
EM reliability test comparison: Early failures when using excess Sn<br />
(8 vs. 3.5 µm)<br />
voiding at Cu-Cu 3 Sn interface<br />
150 o C – 200 o C eff – 1.1mA/um 2<br />
NUF particle entrapment<br />
8.0µm Sn µbump<br />
3.5µm Sn µbump<br />
© IMEC 2011<br />
ERIC BEYNE<br />
14
OUTLINE<br />
o Introduction: Flip chip Scaling<br />
o Baseline µbump interconnect<br />
o Improving Bond quality<br />
o Die stacking strategies<br />
o Wafer-level underfill<br />
o Conclusion<br />
© IMEC 2011 E.BEYNE 15
INTERMETALLIC µBUMP CONNECTIONS<br />
Issues with pure Cu/Sn system:<br />
▸ CuSn intermetallics already form at low<br />
temperature: no elevated temperature<br />
processes between bump formation<br />
and assembly<br />
Sn<br />
Cu<br />
IMC<br />
voids<br />
• Cu and Sn form 2 intermetallic compounds: Cu 3 Sn and Cu 6 Sn 5<br />
• When soldering at high T: single Cu 3 Sn alloy can be obtained<br />
• Unfortunately, low bonding T is required (particularly for memory,<br />
even below 200ºC)<br />
• At practical assembly conditions : Cu 3 Sn and Cu 6 Sn 5 are formed<br />
• Over time this is transformed to Cu 3 Sn, causing Kirkendall void<br />
formation<br />
© IMEC 2011<br />
ERIC BEYNE<br />
16
µBUMPS WITH THIN Ni UBM<br />
Introduction of solder diffusion layer: Cu/Ni/Sn<br />
Sn<br />
Cu<br />
Ni<br />
Sn<br />
Ni<br />
Cu<br />
This resolves thermal stability of the µbump prior to<br />
assembly, it however does not avoid the formation of<br />
Cu 3 Sn intermetallics and Kirkendall voids upon ageing at<br />
Cu-bump side<br />
© IMEC 2011<br />
ERIC BEYNE<br />
17
AVOIDING KIRKENDALL VOIDS AND (Cu, Ni) 3 Sn<br />
FORMATION IN THE Ni/ Thin Cu/Sn SYSTEM<br />
Study using blanket layers and controlled thermal ageing at 200ºC<br />
Sn<br />
3.0 µm ECD Sn<br />
Sn<br />
200˚C/96h<br />
Cu<br />
Ni<br />
0.5 µm ECD Cu<br />
1.5 µm ECD Ni<br />
150 nm PVD Cu<br />
30 nm PVD Ti<br />
(Cu,Ni) 6 Sn 5<br />
Ni<br />
2.5h@200C 4h@200C 96h@200C<br />
Sn Sn Sn<br />
(Cu,Ni) 6 Sn 5 (Cu,Ni) 6 Sn 5<br />
(Cu,Ni) 6 Sn 5<br />
No Kirkendall voids and<br />
no cracks observed in the<br />
(Cu, Ni) 6 Sn 5 phase (all<br />
samples), even after long<br />
ageing at high temperature<br />
© IMEC 2011 ERIC BEYNE 18
NOVEL µBUMP SCHEME: Ni/Cu BI-LAYER UBM<br />
Top Si die<br />
Ni/Cu/Sn bump<br />
3-5 µm Ni<br />
0.5-1µm Cu<br />
3-4 µm Sn<br />
0.5-1µm Cu<br />
3-5 µm Ni<br />
Sn<br />
Cu<br />
Ni<br />
Ni/Cu bump<br />
Cu<br />
Bottom Si die<br />
Ni<br />
3-5 µm Ni bump can also be a Cu/Ni bump<br />
© IMEC 2011<br />
ERIC BEYNE<br />
19
THERMAL AGEING Ni/Cu/Sn<strong>TO</strong> Ni/Cu<br />
µBUMP CONNECTIONS<br />
After ageing at 150°C for 730 hours only a<br />
single phase (Cu,Ni)6Sn5 is observed<br />
150C/730h<br />
pt Ni Cu Sn Phase<br />
4<br />
Ni/Cu/Sn(2/1/4 um)<br />
1<br />
2<br />
3<br />
Ni<br />
1 9.23 39.73 51.04 ~(Cu, Ni) 6 Sn 5<br />
2 - 10.31 89.69 ~Sn (diff. Cu)<br />
3 8.54 41.80 49.66 ~(Cu, Ni) 6 Sn 5<br />
Ni/Cu(2.5/0.5 um)<br />
Ni<br />
4 - 8.65 91.35 ~Sn (diff. Cu)<br />
• Uniform (Cu, Ni) 6 Sn 5 no (Cu,Ni) 3 Sn<br />
• No Kirkendall voids in (Cu,Ni) 6 Sn 5<br />
• Some remaining Sn<br />
© IMEC 2011<br />
ERIC BEYNE<br />
20
BUMP-PLANARIZATION<br />
DIAMOND BIT CUTTING TECHNIQUE<br />
As deposited bump structures<br />
Wafer<br />
Chuck table<br />
Cutting direction<br />
Cutting bit<br />
Fixed distance<br />
from chuck table<br />
Interconnect line<br />
Wafer<br />
Planarized bumps<br />
Cut Cu surface<br />
R a ~ 9nm / R z ~ 50nm<br />
in collaboration with DISCO<br />
© IMEC 2011 ERIC BEYNE 21
CU-BUMP FLY CUTTING RESULTS<br />
After plating :<br />
After fly-cutting:<br />
passivation opening<br />
• Ra = 0.5 µm<br />
• Rt = 1.7 µm<br />
• Within Die variation = 1.0 µm<br />
• Ra = 0.009 µm<br />
• Rt = 0.033 µm<br />
• Within Die variation = 0.020 µm<br />
in collaboration with DISCO<br />
© IMEC 2011 ERIC BEYNE 22
SN-BUMP FLY CUTTING RESULTS<br />
After plating :<br />
After fly-cutting:<br />
• Ra = 0.25 µm<br />
• Rt = 1.60 µm<br />
• Within Die variation = 0.7 µm<br />
in collaboration with DISCO<br />
• Ra = 0.01 µm<br />
• Rt = 0.05 µm<br />
• Within Die variation = 0.10 µm<br />
© IMEC 2011 ERIC BEYNE 23
CU/SN SOLID METAL BONDING @ 150ºC USING<br />
FLY-CUT CU AND CU/SN BUMPS<br />
Cu and Cu/Sn bumps:<br />
▸ 40 µm bump Ø<br />
▸ 15 µm bump spacing<br />
Bonding conditions:<br />
Cu<br />
▸ max. temperature 150ºC<br />
▸ Nom. pressure 50 MPa<br />
▸ Using a no-flow underfill<br />
Results:<br />
▸ Clear formation of an<br />
intermetallic bond<br />
▸ Very smooth interfaces<br />
after bonding<br />
▸ Some misalignment in this<br />
sample<br />
Cu<br />
Cu x Sn y<br />
© IMEC 2011 ERIC BEYNE 24
OUTLINE<br />
o Introduction: Flip chip Scaling<br />
o Baseline µbump interconnect<br />
o Improving Bond quality<br />
o Die stacking strategies<br />
o Wafer-level underfill<br />
o Conclusion<br />
© IMEC 2011 E.BEYNE 25
3D DIE STACKING APPROACHES<br />
1. Sequential Die-to-package-substrate stacking<br />
1<br />
2<br />
3<br />
- Close to standard packaging practice<br />
- Challenge: substrate warpage after first die assembly will limit µbump<br />
assembly capability for next tier die stacking<br />
1. Sequential Die-to-Wafer stacking, followed by stacked die-topackage<br />
stacking.<br />
2 2<br />
3<br />
1<br />
- Si-Si stacking : highest alignment accuracy, finest pitch and narrow gap between<br />
die possible.<br />
- Challenge: fragile thin TSV bottom wafer Wafer “reconstruction”<br />
© IMEC 2011<br />
ERIC BEYNE<br />
26
© IMEC 2011
WAFER-LEVEL UNDERFILL ASSEMBLY<br />
Wafer-level Spin Coated Underfill<br />
Wafer-level Laminated Film Underfill<br />
Stacking Assembly<br />
Die-to-Die Assembly<br />
Die-to-Wafer Assembly<br />
© IMEC 2011<br />
ERIC BEYNE 28
WAFER-LEVEL LAMINATED WLUF<br />
Good transparency of the WLUF film<br />
PTCM/PTCN stacks<br />
after Assembly<br />
Some (up to 100µm)<br />
underfill squeeze out:<br />
to be minimized<br />
CSAM<br />
T-SCAN<br />
Particle entrapment seen on some bumps seen.<br />
May be also due to bump topography<br />
Initial results:<br />
• Good electrical yields w/high bond force<br />
• Good material transparency<br />
• Good filling capability (no voids and delamination)<br />
© IMEC 2011<br />
SAM : No voids or<br />
delamination seen<br />
ERIC BEYNE 29
<strong>TO</strong>POGRAPHY AFTER DIE-<strong>TO</strong>-WAFER STACKING<br />
25µm thin ETNA test die stacked on DRAM-Die:<br />
Dispensed<br />
NUF (single point)<br />
NO underfill<br />
Laminated WLUF<br />
Sample #1 Sample #2<br />
Significant topography after stacking:<br />
NUF process requires multiple point dispense & accurate volume control.<br />
WLUF allows for flattest assembly, even flatter than when not using<br />
underfill during stacking<br />
May be a problem for multi-tier stacking<br />
Expected to be less severe with thicker die (Die bending stiffness t 3 )<br />
© IMEC 2011 ERIC BEYNE 30
ASSEMBLY MODULE<br />
SUCCESSFUL LOGIC-ON-DRAM STACKING W. FILM-WLUF<br />
SAM: No UF Voids<br />
Topo by optical<br />
profilometry < 2μm<br />
© IMEC 2011 ERIC BEYNE 31
OUTLINE<br />
o Introduction: Flip chip Scaling<br />
o Baseline µbump interconnect<br />
o Improving Bond quality<br />
o Die stacking strategies<br />
o Wafer-level underfill<br />
o Conclusion & Outlook<br />
© IMEC 2011 E.BEYNE 32
CONCLUSIONS<br />
‣ Flip chip scaling results in an increased<br />
importance of the intermetallic phases.<br />
‣ µbump flip-chip for Silicon-to-Silicon relies<br />
on full transformation of the solder joint<br />
into intermetallics<br />
‣ This allows for an improved<br />
electromigration resistance<br />
‣ Requires „bump engineering‟ to<br />
avoid Kirkenadll voiding<br />
‣ What are the pitch limits<br />
µbump solder joining?<br />
© IMEC 2011 E.BEYNE 33
BUMP SIZE DEFINED BY BUMP ALIGNMENT<br />
Contact/no contact and/or contact area reduction<br />
H Sn<br />
Optimum condition : Bump<br />
diameter Ø b = Pad spacing S p<br />
Ø b<br />
Ø P<br />
P<br />
S p<br />
P<br />
Before reaching an open<br />
connection, the bump to pad<br />
contact area is reduced,<br />
resulting in an increase in<br />
contact resistance<br />
Non-contact<br />
area<br />
Non-contact<br />
area<br />
Ø p >Ø b : Capture Solder squeeze-out<br />
Misalignment <br />
Misalignment <br />
H Sn<br />
Ø b<br />
Ø P<br />
Ø’ b<br />
H’ Sn<br />
‣ Ø p ≥ Ø b SQRT(H Sn /H‟ Sn )<br />
‣ Therefore : S = P/(1+SQRT(H Sn /H‟ Sn ))<br />
If e.g. (H Sn /H‟ Sn ) max is 4 : S= P/3<br />
© IMEC 2011<br />
34<br />
Eric<br />
beyne
St.dev. alignment (µm)<br />
SCALING ROADMAP<br />
ALIGNMENT ACCURACY REQUIREMENTS<br />
Required alignment accuracy for a maximum increase in contact resistance<br />
of 100% and a Yield of 99.9999 (4N)<br />
5<br />
4.5<br />
4<br />
3.5<br />
3<br />
2.5<br />
2<br />
1.5<br />
1<br />
0.5<br />
0<br />
R/Rn < 2<br />
Y = 4N<br />
P=10µm<br />
0 5 10 15 20 25 30 35 40<br />
© IMEC 2011<br />
P=20µm<br />
P=40µm<br />
Pad Diameter, Dp (µm)<br />
ERIC BEYNE 35<br />
5<br />
10<br />
15<br />
20<br />
25<br />
5<br />
10<br />
3<br />
4<br />
5<br />
Db (µm)<br />
for<br />
P=40µm<br />
Db (µm)<br />
for<br />
P=20µm<br />
Db (µm)<br />
for<br />
P=10µm
ACKNOWLEDGEMENT<br />
3D SYSTEM INTEGRATION PROGRAM<br />
Logic IDM Memory IDM<br />
Foundries<br />
FABLESS<br />
3D Program<br />
SAT<br />
Material Suppliers<br />
EDA<br />
Equipment Suppliers<br />
Lam<br />
RESEARCH<br />
© IMEC 2011 3D SYSTEM INTEGRATION PROGRAM 36
© IMEC 2011