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1 Dept.: System Design & Integration RF & High-Speed System Design Group Head of Group: Dr.-Ing. Ivan Ndip Design and Modeling of Through-Silicon Vias for 3D Integration Ivan Ndip, Brian Curran, Gerhard Fotheringham, Jurgen Wolf, Stephan Guttowski, Herbert Reichl Fraunhofer IZM & BeCAP @ TU Berlin IEEE Workshop on Future Directions in IC and Package Design (FDIP) EPEP 2008, San Jose, CA 26 th October 2008 Design and Modeling of Through Design and Modeling of Through - - Silicon Vias for Silicon Vias for 3D Integration 3D Integration Ivan Ndip, Brian Curran, Gerhard Fotheringham, Jurgen Wolf, Step Ivan Ndip, Brian Curran, Gerhard Fotheringham, Jurgen Wolf, Step han han Guttowski, Herbert Reichl Guttowski, Herbert Reichl Fraunhofer IZM & BeCAP @ TU Berlin Fraunhofer IZM & BeCAP @ TU Berlin IEEE Workshop on Future Directions in IC and Package Design (FDI IEEE Workshop on Future Directions in IC and Package Design (FDI P) P) EPEP 2008, San Jose, CA EPEP 2008, San Jose, CA 26 26 th th October 2008 October 2008

Design and Modeling of Through-Silicon Vias for 3D … Ndip TSV attenuation Attenuation due to Si Attenuation due to conductor 0.001 0.01 0.1 ... Enhancing RF Performance of TSV in

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1Dept.: System Design & IntegrationRF & High-Speed System Design GroupHead of Group: Dr.-Ing. Ivan Ndip

Design and Modeling of Through-Silicon Vias for

3D Integration

Ivan Ndip, Brian Curran, Gerhard Fotheringham, Jurgen Wolf, Stephan

Guttowski, Herbert Reichl

Fraunhofer IZM & BeCAP @ TU Berlin

IEEE Workshop on Future Directions in IC and Package Design (FDIP)

EPEP 2008, San Jose, CA

26th October 2008

Design and Modeling of ThroughDesign and Modeling of Through--Silicon Vias for Silicon Vias for

3D Integration3D Integration

Ivan Ndip, Brian Curran, Gerhard Fotheringham, Jurgen Wolf, StepIvan Ndip, Brian Curran, Gerhard Fotheringham, Jurgen Wolf, Stephan han

Guttowski, Herbert ReichlGuttowski, Herbert Reichl

Fraunhofer IZM & BeCAP @ TU BerlinFraunhofer IZM & BeCAP @ TU Berlin

IEEE Workshop on Future Directions in IC and Package Design (FDIIEEE Workshop on Future Directions in IC and Package Design (FDIP)P)

EPEP 2008, San Jose, CA EPEP 2008, San Jose, CA

2626thth October 2008October 2008

2Dept.: System Design & IntegrationRF & High-Speed System Design GroupHead of Group: Dr.-Ing. Ivan Ndip

■ Motivation

■ Quantification of Some EMR Problems caused by TSVs

■ Methods for Enhancing RF Performance of TSVs in Low Resistivity Silicon

■ On-going Activities to Overcome TSV Design & Fabrication Challenges

Outline

3Dept.: System Design & IntegrationRF & High-Speed System Design GroupHead of Group: Dr.-Ing. Ivan Ndip

■ Motivation

■ Quantification of Some EMR Problems caused by TSVs

■ Methods for Enhancing RF Performance of TSVs in Low Resistivity Silicon

■ On-going Activities to Overcome TSV Design & Fabrication Challenges

Outline

4Dept.: System Design & IntegrationRF & High-Speed System Design GroupHead of Group: Dr.-Ing. Ivan Ndip

Motivation – 1/2

■ To meet consumer demands for miniaturized, high-performance and low-cost products, 3D chip-stacked packages are needed.

■ TSVs offer many advantages over conventional bonding techniques in facilitating 3D integration.

■ A range of applications are emerging in which TSVs will be implemented to develop stacked and miniaturized electronic systems.

5Dept.: System Design & IntegrationRF & High-Speed System Design GroupHead of Group: Dr.-Ing. Ivan Ndip

Top part of

antenna

module

Bottom part of

antenna

moduleMetal layer (patch ground) for vertical shielding

50 Ω feeding point

Solder bump for interconnection to substrate

Electrical interconnect and horizontal shielding

Through silicon vias

Glass support

for handlingMetal Patch

Source: 3DASSM Consortium

Motivation – 2/2

■ Example of Application: 60 GHz Antenna Module for WLAN Applications based on Wafer Level Packaging

6Dept.: System Design & IntegrationRF & High-Speed System Design GroupHead of Group: Dr.-Ing. Ivan Ndip

■ Motivation

■ Quantification of Some EMR Problems caused by TSVs

■ Methods for Enhancing RF Performance of TSVs in Low Resistivity Silicon

■ On-going Activities to Overcome TSV Design & Fabrication Challenges

Outline

7Dept.: System Design & IntegrationRF & High-Speed System Design GroupHead of Group: Dr.-Ing. Ivan Ndip

■ Electromagnetic Reliability (EMR) Problems due to Lossy Nature of Silicon

■ At microwave frequencies, lossy nature of Si leads to severe signal attenuation and other signal/power integrity issues as well as EMI problems.

Typical EMR Problems Associated with TSVs

S

8Dept.: System Design & IntegrationRF & High-Speed System Design GroupHead of Group: Dr.-Ing. Ivan Ndip

■ Geometrical and Material Parameters Considered

■ TSV diameter = separation distance between signal TSV and ground TSV = 40 µm; Er = 11.9, bulk conductivity = VARIABLE

■ Used Analytical Approximations and 3D full-wave Simulations

Si Conductivity from which Si Losses Dominate Conductor Losses – 1/4

Return-current TSVSignal TSV

Silicon substrate

3D model of signal and return-current TSVs

9Dept.: System Design & IntegrationRF & High-Speed System Design GroupHead of Group: Dr.-Ing. Ivan Ndip

■ Using Analytical Approximations

■ Signal & return-current TSVs can be approximated as 2 conductor TML

■ Per-unit length parameters are given as

■ By setting G=0 & neglecting losses due to radiation & proximity effect, signal attenuation due to conductor & dielectric may be approximately considered separately.

Signal TSV

( ' ')( ' ')R j L G j C

' sRR

a 2' ln / 2 ( / 2 ) 1

uL d a d a

2

'ln / 2 ( / 2 ) 1

Gd a d a

2'

ln / 2 ( / 2 ) 1C

d a d a

dReturn-current TSV

Si Conductivity from which Si Losses Dominate Conductor Losses – 2/4

10Dept.: System Design & IntegrationRF & High-Speed System Design GroupHead of Group: Dr.-Ing. Ivan Ndip

Attenuation due to Si Attenuation due to conductorTSV attenuation

0.001 0.01 0.1 1 10 1000.00001

0.0001

0.001

0.01

0.1

Bulk Conductivity (S/m)

Att

enua

tion

(dB

/um

)

0.001 0.01 0.1 1 10 1000.00001

0.0001

0.001

0.01

0.1

Bulk Conductivity (S/m)A

tten

uati

on (

dB/u

m)

Attenuation @ 20 GHz

0.12 S/m predicted “corner conductivity”

Attenuation @ 60 GHz

0.25 S/mpredicted “corner conductivity”

■ Using Analytical Approximations

■ Signal & return-current TSVs can be approximated as 2 conductor TML

Si Conductivity from which Si Losses Dominate Conductor Losses – 3/4

11Dept.: System Design & IntegrationRF & High-Speed System Design GroupHead of Group: Dr.-Ing. Ivan Ndip

The Insertion loss obtained using full-wave simulations shows same effect as predicted with analytical approximations

Transmission Coefficient vs. Conductivity

-8

-7

-6

-5

-4

-3

-2

-1

0

-5,0 -4,0 -3,0 -2,0 -1,0 0,0 1,0 2,0

Bulk Conductivity (S/m)

Tran

smis

sio

n C

oef

fici

ent,

S12

5 GHz

300 MHz

60 GHz

77 GHz

leveling off in the S-parameters

0.00001 0.0001 0.001 0.01 0.1 1 10 100

■ Using Full-wave Simulations

Si Conductivity from which Si Losses Dominate Conductor Losses – 4/4

12Dept.: System Design & IntegrationRF & High-Speed System Design GroupHead of Group: Dr.-Ing. Ivan Ndip

Impact of Resistivity on RF Performance of TSVs – 1/2

■ Intensity of EMR Problems caused by TSVs depends on Si Resistivity

■ Approximate range obtained from vendors

■ Low Resistivity Silicon (LRS) = > 100 S/m, (< 1 Ohm cm)

■ Medium Resistivity Silicon (MRS) = 5 – 10 S/m, (10 – 20 Ohm cm)

■ High Resistivity Silicon (HRS) = < 5 S/m, (> 20 Ohm cm)

■ LRS is far more cheaper than MRS & HRS

■ Values considered

■ LRS = 100 S/m

■ MRS = 10 S/m

■ HRS = 0.2 S/m

13Dept.: System Design & IntegrationRF & High-Speed System Design GroupHead of Group: Dr.-Ing. Ivan Ndip

0.00 10.00 20.00 30.00 40.00 50.00 60.00 70.00 80.00Freq [GHz]

-6.00

-5.00

-4.00

-3.00

-2.00

-1.00

0.00T

ran

smis

sio

n C

oe

ffic

ien

t, S

12

(d

B)

Ansoft Corporation HFSSDesign2XY Plot 1

0.2 S/m

10 S/m

100 S/m

Impact of Resistivity on RF Performance of Unshielded TSVs – 2/2

■ Geometrical Parameters Considered

■ TSV diameter = separation distance between signal TSV and ground TSV = 40 µm; TSV length =200 µm

■ Insertion Loss considered as example

Challenge: To use LRS (which is far more cheaper than MRS & HRS, but extremely

lossy) to design high performance silicon-based system modules

14Dept.: System Design & IntegrationRF & High-Speed System Design GroupHead of Group: Dr.-Ing. Ivan Ndip

0.00 10.00 20.00 30.00 40.00 50.00 60.00 70.00 80.00Freq [GHz]

-40.00

-35.00

-30.00

-25.00

-20.00

-15.00

-10.00

Ne

ar

En

d C

ross

-ta

lk, S

13

(d

B)

Ansoft Corporation HFSSDesign1XY Plot 2

Decrease in the conductivity of the silicon results in:

A nearly 50% decrease in the losses

BUT, nearly no change in the cross-talk

0.00 10.00 20.00 30.00 40.00 50.00 60.00 70.00 80.00Freq [GHz]

-1.60

-1.50

-1.40

-1.30

-1.20

-1.10

-1.00

-0.90

-0.80

-0.70

-0.60

-0.50

Tra

nsm

issi

on

Co

effi

cie

nt,

S1

2 (

dB

)

Ansoft Corporation HFSSDesign1XY Plot 1

5 S/m10 S/m

5 S/m10 S/m

TSV Cross-talk continues to be a problem,

even when losses are manageable.

Cross-talk in TSVs

G

GS

R

15Dept.: System Design & IntegrationRF & High-Speed System Design GroupHead of Group: Dr.-Ing. Ivan Ndip

■ Motivation

■ Quantification of Some EMR Problems caused by TSVs

■ Methods for Enhancing RF Performance of TSVs in Low Resistivity Silicon

■ On-going Activities to Overcome TSV Design & Fabrication Challenges

Outline

16Dept.: System Design & IntegrationRF & High-Speed System Design GroupHead of Group: Dr.-Ing. Ivan Ndip

H-field intensity in Si around Coax-TSV from

10MHz to 1 GHz

Enhancing RF Performance of TSV in Low Resistivity Silicon – 1/4

■ Concept of Coax-TSVs

Coax-TSV

E

H

ts

1P S.ds

2 t

s

1P S.ds

2

S E H

3D model of Coax TSV

17Dept.: System Design & IntegrationRF & High-Speed System Design GroupHead of Group: Dr.-Ing. Ivan Ndip

■ Coax-TSV (Si-filled) Vs Coax-TSV (Mixed-filled)

■ Coax-TSV (Si-filled): If Si is used as dielectric, there will be no improvement in RF performance

■ Coax-TSV (Mixed-filled): RF Performance is greatly enhanced if Si is partly replaced by low-loss dielectric e.g., BCB

Si

Si

Reference

S/P

0.00 10.00 20.00 30.00 40.00 50.00 60.00 70.00 80.00Freq [GHz]

-8.00

-7.00

-6.00

-5.00

-4.00

-3.00

-2.00

-1.00

0.00

Tra

nsm

issi

on

Co

eff

icie

nt,

S1

2 (

dB

)

Ansoft Corporation One_ViaXY Plot 1

BCB

Si

S/P

Si

Coax-TSV (Mixed-filled)

Coax-TSV (Si-filled)

Coax-TSV (Mixed-filled)

Coax-TSV (Si-filled)

Enhancing RF Performance of TSV in Low Resistivity Silicon – 2/4

18Dept.: System Design & IntegrationRF & High-Speed System Design GroupHead of Group: Dr.-Ing. Ivan Ndip

■ Coax-TSV (Mixed-filled)

■ Enhancement of RF performance depends on ratio of Silicon to BCB

■ 3 different ratios were examined.

0.00 10.00 20.00 30.00 40.00 50.00 60.00 70.00 80.00Freq [GHz]

-0.45

-0.40

-0.35

-0.30

-0.25

-0.20

-0.15

-0.10

-0.05

0.00

Tra

nsm

issi

on

Co

effi

cie

nt,

S1

2 (

dB

)

Ansoft Corporation One_ViaXY Plot 2 2.5 m – 15 m – 2.5 m

5 m – 10 m – 5 m

10 m – 5 m – 10 m

BCB

Si

S/P

Si

Coax-TSV (Mixed-filled)

Enhancing RF Performance of TSV in Low Resistivity Silicon – 3/4

19Dept.: System Design & IntegrationRF & High-Speed System Design GroupHead of Group: Dr.-Ing. Ivan Ndip

■ Coax-TSV (Low-loss dielectric-filled)

0.00 10.00 20.00 30.00 40.00 50.00 60.00 70.00 80.00Freq [GHz]

-8.00

-7.00

-6.00

-5.00

-4.00

-3.00

-2.00

-1.00

0.00

Tra

nsm

issi

on

Co

effi

cie

nt,

S1

2 (

dB

)

Ansoft Corporation One_ViaXY Plot 1

Coax-TSV (Mixed-filled)

Coax-TSV (Si-filled)

Coax-TSV (Lo-loss dielectric-filled)

BCB

Si

Si

Si

S/P

BCB

Si

S/P

Si

Coax-TSV (Mixed-filled)

Coax-TSV (Si-filled)

Coax-TSV (Low-loss dielectric-filled)

Enhancing RF Performance of TSV in Low Resistivity Silicon – 4/4

20Dept.: System Design & IntegrationRF & High-Speed System Design GroupHead of Group: Dr.-Ing. Ivan Ndip

■ Motivation

■ Quantification of Some EMR Problems caused by TSVs

■ Methods for Enhancing RF Performance of TSVs in Low Resistivity Silicon

■ On-going Activities to Overcome TSV Design & Fabrication Challenges

Outline

21Dept.: System Design & IntegrationRF & High-Speed System Design GroupHead of Group: Dr.-Ing. Ivan Ndip

Consortium on 3D All Silicon System Module (3DASSM)

■ Goal of 3D ASSM

■ Miniaturization of the entire electronic system using Si for ICs, packages, and boards. This approach is expected to result in high system performance at low cost and high reliability.

■ Academic Partners

■ Georgia Tech (USA)

■ KAIST (Korea)

■ Fraunhofer IZM (Germany)

■ Proposing 20+ Projects & 3 Test Vehicles

■ Thrusts

■ Electrical Design & Test

■ Silicon Substrate with Multilayer Wiring

■ Low-cost TSV & Stack Bonding

■ Embedded Thin Film Actives & Passives

■ System Interconnects

■ More Information: http://www.prc.gatech.edu/events/3dassm/index.htm

22Dept.: System Design & IntegrationRF & High-Speed System Design GroupHead of Group: Dr.-Ing. Ivan Ndip

■ Electrical Design & Test Thrust

■Objectives: Explore and develop design methodologies to enable ultra-miniaturization and low cost hetero-integration addressing the challenges with the electrical properties of silicon.

Consortium on 3D All Silicon System Module (3DASSM)

Project Previous Approach

Proposed Approach

Project A-1: Design of Interposer with Zero SSN

Minimize Noise using decaps and planes

Eliminate noise with power trans. lines and TSV

Project A-2: Design of Stack Bond with Vertical Shielding

Non-coaxial TSVCPW

Coaxial TSVSWLSMagnetic Film

Project A-3: Hybrid Equalization for over 10Gbps High Speed Channel

Either active or passive Active and passive

23Dept.: System Design & IntegrationRF & High-Speed System Design GroupHead of Group: Dr.-Ing. Ivan Ndip

Thank you very much

for your attention!