from c4 pbsn flip chip to lead-free µbump flip chip · - si-si stacking : highest alignment...

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© IMEC 2011 FROM C4 PbSn FLIP CHIP TO LEAD-FREE μBUMP FLIP CHIP ERIC BEYNE “VIJF JAAR LOODVRIJ SOLDEREN” 22 SEPTEMBER 2011 TNO, EINDHOVEN

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© IMEC 2011

FROM C4 PbSn FLIP CHIP TO

LEAD-FREE µBUMP FLIP CHIPERIC BEYNE

“VIJF JAAR LOODVRIJ SOLDEREN”

22 SEPTEMBER 2011

TNO, EINDHOVEN

© IMEC 2011 E.BEYNE 2

o Introduction: Flip chip Scaling

o µbump interconnect

o Improving Bond quality

o Die stacking strategies

o Wafer-level underfill

o Conclusion

OUTLINE

© IMEC 2011

SCALING FLIP-CHIP INTERCONNECTS

- With solder joint scaling, the intermetallics formed by UBM solder interaction are of increasing importance

- For the smallest flip chip pitches : only intermetalliccompounds after solder bump reflow

ERIC BEYNE 3

100µm pad diameter

150-200µm bump pitch

10µm pad

20µm pitch

40µm pad Ø

60µm pitch

20µm pad

40µm pitch

IMC

© IMEC 2011

MICRO-BUMP JOINING

Similar to flip chip interconnect:

▸ Low temperature melting solder metal, UBM metals.

However:

▸ Entire solder volume is transformed into intermetallic compounds

▸ Small dimension : no solder „ball‟, typically < 10m thick

▸ Connection by thermo/compression-reflow method

▸ Requires improved control and flatness of the solder “bumps”

ERIC BEYNE 4

M

Si

Solder

M

Si

M

Si

Solder

M

Si

M

Si

M

Si

IMC

M

M

Solder - IMC

© IMEC 2011

APPLICATION SPACE µBUMP JOINING

Si-Si face-to-face bonding

2.5D integration:

Si chips to Si interposers

3D integration : chip stacking with TSV

ERIC BEYNE 5

DRAM Logic

© IMEC 2011 E.BEYNE 6

o Introduction: Flip chip Scaling

o Baseline µbump interconnect

o Improving Bond quality

o Die stacking strategies

o Wafer-level underfill

o Conclusion

OUTLINE

© IMEC 2011

BASELINE µBUMPING SCHEME: Cu/SnTO Cu

Baseline µbump scheme

▸ Die 1: Cu/Sn (5/3.5 µm)

▸ Die 2: Cu (5 µm)

µBump Ø: 25 down to 7.5 µm

µBump pitch: 40 down to 20 µm

Smooth side wall for

Cu and Sn

No residues after

seed layer etch

Cu/Sn bump

Bottom Si die

Top Si die

5µm Cu

5µm Cu

3.5µm Sn

7ERIC BEYNE

© IMEC 2011 ERIC BEYNE 8

DEMONSTRATION OF COLLECTIVE

TRANSIENT-LIQUID PHASE µBUMP BONDING

Bonding procedure:

• Pick & place die on wafer by Flip Chip bonding Tool, at

room temperature

• Collective Bonding in Wafer Bonder @ 250ºC

© IMEC 2011 ERIC BEYNE 9

SOLID METAL BONDING:

CuSn INTERMETALLIC BONDING @ 150ºC

Top die

(Cu/Sn bump)

Bottom wafer

(Cu bump)

150C/50MPa

with no-flow underfill

Ф 25m bump, 40/15m

pitch/spacing

150C/150MPa150°C/50MPa

Ф 25m bump, 40/15m

pitch/spacing

© IMEC 2011

40 µm PITCH, Cu/Sn µBUMP DIE STACKING

PTCM/N TEST CHIPS

10ERIC BEYNE

5x5mm PTCM,

40 µm pitch

µbumps,

2 peripheral rows8x8mm PTCN

“landing”die

PTCN/M stack wire

bonded in BGA package

Cu/Sn microbump samples:

3.5 µm and 8µm thick Sn on 40µm pitch Cu bumps,

100 µm thick Silicon

Si-Si assembly in BGA package and SMD on test board

Use of a no-flow underfill

Package level reliability of TLP bumps demonstrated

>1800 temp cycles

>1000 hrs in electromigration tests

96 hrs HAST

© IMEC 2011

THERMAL CYCLING 40 µm PITCH Cu/Sn

µBUMP PTCM/N BGA ASSEMBLIES ON PCB

THERMAL CYCLING (-45°C/125°C) – IN-SITU

RESISTANCE MONITORING

In-situ resistance monitoring during

30’ 45ºC/30’125ºC thermal cyclingCu/Sn microbump samples:

▸ 3.5 µm and 8µm thick Sn on 40µm pitch

Cu bumps, 100 µm thick Silicon

▸ Use of a no-flow underfill (NCP)

No failures up to 4000 cycles

ERIC BEYNE 11

0

20

40

60

80

100

120

140

160

180

0 200 400 600 800 1000 1200 1400 1600 1800 2000

Time [h] = Cycles [#]

Res

ista

nce

[O

hm

]

8.0µm Sn bump DC

3.5µm Sn bump DC

80

90

100

110

2950 3050 3150 3250 3350 3450 3550 3650 3750 3850 3950 4050

Time [h]R

esis

tan

ce [

Oh

m]

150

160

170

180

3000 3100 3200 3300 3400 3500 3600 3700 3800 3900 4000

Time [h]

Resi

stan

ce [O

hm]

In-situ R @-45°C

In-situ measurement at 125°C

Da

isy c

ha

in R

esis

tan

ce

(O

hm

)

Time (h) = # cycles -45°C/+125°C

Da

isy c

ha

in R

esis

tan

ce

(O

hm

)

In-situ R at 125°C

Dais

y c

hain

Resis

tan

ce (

Oh

m)

© IMEC 2011

AGEING BEHAVIOUR OF LOW T Cu/SnTLP

µBUMP: VOID FORMATION

Shift over time from Cu6Sn5 to Cu3Sn, due to the excess of Cu.

The difference in diffusion rates of Cu and Sn results in vacancies

that aglomerate to form voids : Kirkendall voids.

ERIC BEYNE 12

Cu

Cu

Cu3Sn

Cu

Cu

Cu6Sn5

Cu3Sn

Cu3Sn

Cu6Sn5

Cu3Sn

Cu3Sn

Cu

Cu

Initial stateAfter ageing at 250ºC for 15’

After ageing at 250ºC for

45’

© IMEC 2011

WHY FULL TRANSFORMATION TO IMC?

When using low volume “mini-bumps” with excess Sn, the risk of

electro-migration failure strongly increases

EM reliability test comparison: 40 µm pitch Cu/Sn µbump packaged

F2F chip assemblies on PCB

EM test structure with build-in

temperature monitor

Cu/Sn microbump samples:

3.5 µm and 8µm thick Sn on 40µm pitch

Cu bumps, 100 µm thick Silicon

Si-Si assembly in BGA package and SMD

on test board

Use of a no-flow underfill

13ERIC BEYNE

© IMEC 2011

WHY FULL TRANSFORMATION TO IMC?

When using low volume “mini-bumps” with excess Sn, the risk of

electro-migration failure strongly increases

EM reliability test comparison: Early failures when using excess Sn

(8 vs. 3.5 µm)

150 oC – 200oCeff – 1.1mA/um2

No d

ata

8.0µm Sn µbump

3.5µm Sn µbump

NUF particle entrapment

voiding at Cu-Cu3Sn interface

14ERIC BEYNE

© IMEC 2011 E.BEYNE 15

o Introduction: Flip chip Scaling

o Baseline µbump interconnect

o Improving Bond quality

o Die stacking strategies

o Wafer-level underfill

o Conclusion

OUTLINE

© IMEC 2011

INTERMETALLIC µBUMP CONNECTIONS

Issues with pure Cu/Sn system:

▸ CuSn intermetallics already form at low

temperature: no elevated temperature

processes between bump formation

and assembly

Cu

Sn IMC

voids

• Cu and Sn form 2 intermetallic compounds: Cu3Sn and Cu6Sn5

• When soldering at high T: single Cu3Sn alloy can be obtained

• Unfortunately, low bonding T is required (particularly for memory,

even below 200ºC)

• At practical assembly conditions : Cu3Sn and Cu6Sn5 are formed

• Over time this is transformed to Cu3Sn, causing Kirkendall void

formation

16ERIC BEYNE

© IMEC 2011

µBUMPS WITH THIN Ni UBM

Introduction of solder diffusion layer: Cu/Ni/Sn

This resolves thermal stability of the µbump prior to

assembly, it however does not avoid the formation of

Cu3Sn intermetallics and Kirkendall voids upon ageing at

Cu-bump side

Cu

Sn

NiCu

Sn

Ni

17ERIC BEYNE

© IMEC 2011 ERIC BEYNE 18

No Kirkendall voids and

no cracks observed in the

(Cu, Ni)6Sn5 phase (all

samples), even after long

ageing at high temperature

AVOIDING KIRKENDALLVOIDS AND (Cu, Ni)3Sn

FORMATION IN THE Ni/ Thin Cu/Sn SYSTEM

(Cu,Ni)6Sn5

Sn

Ni

200˚C/96h

2.5h@200C 4h@200C 96h@200C

(Cu,Ni)6Sn5 (Cu,Ni)6Sn5 (Cu,Ni)6Sn5

Sn Sn Sn

0.5 µm ECD Cu

1.5 µm ECD Ni

3.0 µm ECD Sn

Study using blanket layers and controlled thermal ageing at 200ºC

150 nm PVD Cu

30 nm PVD Ti

Sn

Ni

Cu

© IMEC 2011

NOVEL µBUMP SCHEME: Ni/Cu BI-LAYER UBM

3-5 µm Ni bump can also be a Cu/Ni bump

Ni/Cu bump

Ni

Cu

Ni

Sn3-5 µm Ni

0.5-1µm Cu

3-4 µm Sn

Bottom Si die

Top Si die

0.5-1µm Cu

3-5 µm Ni

Ni/Cu/Sn bump

Cu

19ERIC BEYNE

© IMEC 2011

THERMAL AGEING Ni/Cu/SnTO Ni/Cu

µBUMP CONNECTIONS

After ageing at 150°C for 730 hours only a

single phase (Cu,Ni)6Sn5 is observed

• Uniform (Cu, Ni)6Sn5 no (Cu,Ni)3Sn

• No Kirkendall voids in (Cu,Ni)6Sn5

• Some remaining Sn

pt Ni Cu Sn Phase

1 9.23 39.73 51.04 ~(Cu, Ni)6Sn5

2 - 10.31 89.69 ~Sn (diff. Cu)

3 8.54 41.80 49.66 ~(Cu, Ni)6Sn5

4 - 8.65 91.35 ~Sn (diff. Cu)

1

342

150C/730h

Ni/Cu/Sn(2/1/4 um)

Ni/Cu(2.5/0.5 um)

Ni

Ni

20ERIC BEYNE

© IMEC 2011 ERIC BEYNE 21

BUMP-PLANARIZATION

DIAMOND BIT CUTTING TECHNIQUE

Wafer

Cutting bitCutting direction

Fixed distance from chuck table

Planarized bumps

Chuck table

Wafer

As deposited bump structures

Ra ~ 9nm / Rz ~ 50nm

Interconnect line

Cut Cu surface

in collaboration with DISCO

© IMEC 2011 ERIC BEYNE 22

CU-BUMP FLY CUTTING RESULTS

After plating : After fly-cutting:

passivation opening

• Ra = 0.009 µm

• Rt = 0.033 µm

• Within Die variation = 0.020 µm

• Ra = 0.5 µm

• Rt = 1.7 µm

• Within Die variation = 1.0 µmin collaboration with DISCO

© IMEC 2011 ERIC BEYNE 23

SN-BUMP FLY CUTTING RESULTS

After plating : After fly-cutting:

• Ra = 0.01 µm

• Rt = 0.05 µm

• Within Die variation = 0.10 µm

• Ra = 0.25 µm

• Rt = 1.60 µm

• Within Die variation = 0.7 µmin collaboration with DISCO

© IMEC 2011 ERIC BEYNE 24

CU/SN SOLID METAL BONDING @ 150ºC USING

FLY-CUT CU AND CU/SN BUMPS

Cu and Cu/Sn bumps:

▸ 40 µm bump Ø

▸ 15 µm bump spacing

Bonding conditions:

▸ max. temperature 150ºC

▸ Nom. pressure 50 MPa

▸ Using a no-flow underfill

Results:

▸ Clear formation of an intermetallic bond

▸ Very smooth interfaces after bonding

▸ Some misalignment in this sample

Cu

Cu

CuxSny

© IMEC 2011 E.BEYNE 25

o Introduction: Flip chip Scaling

o Baseline µbump interconnect

o Improving Bond quality

o Die stacking strategies

o Wafer-level underfill

o Conclusion

OUTLINE

© IMEC 2011

3D DIE STACKING APPROACHES

1. Sequential Die-to-package-substrate stacking

- Close to standard packaging practice

- Challenge: substrate warpage after first die assembly will limit µbump

assembly capability for next tier die stacking

1. Sequential Die-to-Wafer stacking, followed by stacked die-to-

package stacking.

- Si-Si stacking : highest alignment accuracy, finest pitch and narrow gap between

die possible.

- Challenge: fragile thin TSV bottom wafer Wafer “reconstruction”

ERIC BEYNE

1 32

31

2 2

26

© IMEC 2011

© IMEC 2011

WAFER-LEVEL UNDERFILL ASSEMBLY

ERIC BEYNE 28

Wafer-level Laminated Film Underfill

Wafer-level Spin Coated Underfill

Die-to-Die Assembly

Die-to-Wafer Assembly

Sta

ck

ing A

ssem

bly

© IMEC 2011

Good transparency of the WLUF film

WAFER-LEVEL LAMINATED WLUF

ERIC BEYNE 29

PTCM/PTCN stacks

after Assembly

SAM : No voids or

delamination seen

CSAM

T-SCAN

Particle entrapment seen on some bumps seen.

May be also due to bump topographyInitial results:

• Good electrical yields w/high bond force

• Good material transparency

• Good filling capability (no voids and delamination)

Some (up to 100µm)

underfill squeeze out:

to be minimized

© IMEC 2011 ERIC BEYNE 30

25µm thin ETNA test die stacked on DRAM-Die:

Significant topography after stacking:NUF process requires multiple point dispense & accurate volume control.

WLUF allows for flattest assembly, even flatter than when not using

underfill during stacking

May be a problem for multi-tier stacking

Expected to be less severe with thicker die (Die bending stiffness t3)

TOPOGRAPHY AFTER DIE-TO-WAFER STACKING

Dispensed

NUF (single point) NO underfill Laminated WLUF Sample #1 Sample #2

© IMEC 2011 ERIC BEYNE 31

SAM: No UF Voids

Topo by optical

profilometry < 2μm

ASSEMBLY MODULESUCCESSFUL LOGIC-ON-DRAM STACKING W. FILM-WLUF

© IMEC 2011 E.BEYNE 32

o Introduction: Flip chip Scaling

o Baseline µbump interconnect

o Improving Bond quality

o Die stacking strategies

o Wafer-level underfill

o Conclusion & Outlook

OUTLINE

© IMEC 2011 E.BEYNE 33

CONCLUSIONS

Flip chip scaling results in an increased

importance of the intermetallic phases.

µbump flip-chip for Silicon-to-Silicon relies

on full transformation of the solder joint

into intermetallics

This allows for an improved

electromigration resistance

Requires „bump engineering‟ to

avoid Kirkenadll voiding

What are the pitch limits

µbump solder joining?

© IMEC 2011

BUMP SIZE DEFINED BY BUMP ALIGNMENT

Contact/no contact and/or contact area reduction

34Eric

beyne

Optimum condition : Bump

diameter Øb = Pad spacing Sp

Non-contact

area

Non-contact

area

Misalignment Misalignment

Before reaching an open

connection, the bump to pad

contact area is reduced,

resulting in an increase in

contact resistance

Øp≥ Øb SQRT(HSn/H‟Sn)

Therefore : S = P/(1+SQRT(HSn/H‟Sn))

If e.g. (HSn/H‟Sn )max is 4 : S= P/3

Øb

ØP

HSn

H’Sn

Ø’b

Øp >Øb : Capture Solder squeeze-out

Øb

ØP

HSn

Sp

P

P

© IMEC 2011

SCALING ROADMAP

ALIGNMENT ACCURACY REQUIREMENTSRequired alignment accuracy for a maximum increase in contact resistance

of 100% and a Yield of 99.9999 (4N)

ERIC BEYNE 35

0

0.5

1

1.5

2

2.5

3

3.5

4

4.5

5

0 5 10 15 20 25 30 35 40

St.d

ev.

ali

gnm

en

t (µ

m)

Pad Diameter, Dp (µm)

5

10

15

20

25

5

10

3

4

5

Db (µm) for

P=40µm

Db (µm)for

P=20µm

Db (µm)for

P=10µm

P=40µm

P=20µm

P=10µm

R/Rn < 2

Y = 4N

© IMEC 2011 3D SYSTEM INTEGRATION PROGRAM 36

ACKNOWLEDGEMENT

3D SYSTEM INTEGRATION PROGRAM

3D Program

LamRESEARCH

Foundries

SAT

Memory IDM

EDA

FABLESS

Equipment Suppliers

Logic IDM

Material Suppliers

© IMEC 2011