power delivery model of test probe cards

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June 5, 2005 2005 Southwest Test Workshop 1 POWER DELIVERY MODEL OF TEST PROBE CARDS Habib Kilicaslan ([email protected]) Bahadir Tunaboylu ([email protected]) Kulicke & Soffa Industries

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Page 1: POWER DELIVERY MODEL OF TEST PROBE CARDS

June 5, 2005 2005 Southwest Test Workshop 1

POWER DELIVERY MODEL OF TEST

PROBE CARDS

Habib Kilicaslan ([email protected])Bahadir Tunaboylu ([email protected])Kulicke & Soffa Industries

Page 2: POWER DELIVERY MODEL OF TEST PROBE CARDS

SWTW-2005June 5, 2005 2

Overall system view

Space transformer

PCB

Probes

Decoupling capacitor on PCB

Decoupling capacitor on ST Spring pinsPlane layers

Power supply

DUT (die)

Via

Power supply PCB Spring pins MLC Probes DUT

Page 3: POWER DELIVERY MODEL OF TEST PROBE CARDS

SWTW-2005June 5, 2005 3

Challenge

Assuming one of the latest generation processor is being tested

Power consumption:100WSupply voltage:1VWhat if DUT ramps from 0 A to 100 A in

5 ns having 20 A/ns slew rate [Ref1].Any resistance and inductance seen on the path will create voltage drop defined by Vdrop=Lpath*∆i/∆t+Rpath*I

Given maximum allowed voltage drop of 0.5V (0.25V inductance related + 0.25V resistance related)Maximum path inductance 12.5pHMaximum path resistance 2.5 mohm

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SWTW-2005June 5, 2005 4

Achievable?

Can 12.5 pH and 2.5 mohm be achievable?Assuming DUT has 1000 (500 VCC – 500 GND) probe

pads For given probe height (h)=200mil, probe

diameter(2*r)=80um, probe pitch (s)=200um.For given total system height (htot)

Probe + ST + Spring pin +PCB 200+100+100+200=600milsTotal inductance = 16.9 pHAssuming 70 percent of the path resistance is created by the contact resistance of probes, then Max contact resistance for each probe = 437 mohm

Rough calculations show that system requires careful analysis of each stage

0.2. . ln.µ µπ

− =

tot stot

h s rLn r

Page 5: POWER DELIVERY MODEL OF TEST PROBE CARDS

SWTW-2005June 5, 2005 5

Goal of the study

Modeling of each block from transient analysis perspective including 3D electromagnetic modeling

Observe transient voltages in each stage (subsystem)Determine highest voltage drop contributorsReduce voltage fluctuations by means of changing: design, routing and mechanical structure and/or developing new strategies.

Page 6: POWER DELIVERY MODEL OF TEST PROBE CARDS

SWTW-2005June 5, 2005 6

Distributed vs. lumped model

Major inductance components are height dependent and height of the system is small compared to wavelength/10

Second biggest contributor; contact resistance may be represented better by lumped model

For PCB and ST design, EM based simulation tools can be run such as PowerSI from Sigrity Inc. or Ansoft Q3D using distributed model [Ref 3]. Mechanical designs, spring pins and probes require special attention.

Lumped model representation has been selected for the reason of being faster and accurate in reasonable boundary.

What if each probe carries different amount of current?Current differences will be equalized on ST level (plane connection).

Page 7: POWER DELIVERY MODEL OF TEST PROBE CARDS

SWTW-2005June 5, 2005 7

HCDPS (High current device power supply)

Modeling is based on short term transient response. (<1 uS)During simulation duration power supply correction loop is nonfunctional (existing power supply closed system bandwidth is limited to kHz region )[Ref 2]

POWER SUPPLY

SENSE LINES

PROBE CARDDUT

Page 8: POWER DELIVERY MODEL OF TEST PROBE CARDS

SWTW-2005June 5, 2005 8

PCB

Main contributors : Via inductance , plane layer inductance.Number of vias can be increased to reduce via inductance

effects to negligible levelPCB area has enough space to put decoupling capacitors to

compensate inductance effects. For decoupling capacitors via effects should be minimized.Better ESL and ESR decoupling capacitors should be usedDue to space convenience PCB contribution to overall

system voltage drop budget can be minimized easily (<3%)

2 22 20 ln( ) ( )

2.µπ

+ += + − +

via

h r hL h r r hr0µ µ=layer s

dL lw

Page 9: POWER DELIVERY MODEL OF TEST PROBE CARDS

SWTW-2005June 5, 2005 9

PCB model

Different capacitor values are used to lower impedance on different frequency spots

Re1mΩ

Cp1uF

Le1nH

Rh1MΩxHz

Ri1GΩ

LcvianH

LpvianH

SECD1 SECD2

RcviamΩ

SEcvia

RpviamΩ

SEpvia

LgvianH

RgviamΩ

SEgvia

Re2mΩ

Cp2uF

Le2nH

Rh2MΩxHz

Ri2GΩ

LcvianH

RcviamΩ

SEcvia

Page 10: POWER DELIVERY MODEL OF TEST PROBE CARDS

SWTW-2005June 5, 2005 10

Spring pins

Main contributors: Pin inductance, contact resistance.Pin inductance could be reduced by making shorter and

increasing pin diameter. Contact resistance can be minimized by solidly fixing one side

of the pogo pin such soldering etc. which is a tradeoff with mechanical replaceability

Each path models the half of the loop inductance including partial inductance and mutual inductance. Values are acquired from 3D electromagnetic simulator.

LenH

RemΩ

SEspp

LenH

RemΩ

SEgpp

Page 11: POWER DELIVERY MODEL OF TEST PROBE CARDS

SWTW-2005June 5, 2005 11

Space transformer (ST)

Main contributors : Via inductance and plane layer inductance.Increasing number of vias is troublesome because it has limited area for additional vias, also tied by design rules

Generally LTCC ceramics are used for base material and via spacing rules are wider due to shrinkage during sintering, limiting maximum via number

Limited amount of decoupling capacitors could be added (backplane space limitation)

For decoupling capacitors low ESL capacitors are used (IVX).Voltage drop contribution of space transformer is quite large (~25%)

Page 12: POWER DELIVERY MODEL OF TEST PROBE CARDS

SWTW-2005June 5, 2005 12

Re1mΩ

Cp1uF

Le1nH

Ri1GΩ

LcvianH

LpvianH

SECD1 SECD2

RcviamΩ

SEcvia

RpviamΩ

SEpvia

LgvianH

RgviamΩ

SEgvia

Re2mΩ

Cp2uF

Le2nH

Rh2MΩxHz

Ri2GΩ

LcvianH

RcviamΩ

SEcvia

LpvianH

RpviamΩ

SEpvia

LgvianH

RgviamΩ

SEgvia

ST model

Via effects are shared before and after decoupling capacitors

Page 13: POWER DELIVERY MODEL OF TEST PROBE CARDS

SWTW-2005June 5, 2005 13

Probe

Probe inductance and contact resistance are the main contributors.

Inductance could be lowered by reducing probe height and increasing diameter of the probes, tradeoff with mechanical deflection and forces

Contact resistance could be decreased by using one sided mounted probes.

Could be modeled with partial inductance and mutual inductance

Page 14: POWER DELIVERY MODEL OF TEST PROBE CARDS

SWTW-2005June 5, 2005 14

Probe modelMutual inductance lowers the total inductance by 20 percent

for given pitch. Although smaller pitch reduces probe inductance, crosstalk becomes worse.

LenH

RemΩ

SEsp

LenH

RemΩ

SEgp

RcmΩ

RcmΩ

LmutnH

Page 15: POWER DELIVERY MODEL OF TEST PROBE CARDS

SWTW-2005June 5, 2005 15

DUT

Ondie capacitance created by supply line routing and device parasitics improves short term transient response.

High slew rate ramping modeled by step current source.

RemΩ

CenF

IpAA/ns

Page 16: POWER DELIVERY MODEL OF TEST PROBE CARDS

SWTW-2005June 5, 2005 16

Combined model

Vpcbn

Vpcbp

SPRING PIN

Vdutn

Vdutp

DUT

Vpow

POWER SUPPLY PCB ST PROBE

Vstn

Vstp

Vpgn

Vpgp

PRCPRCcd1

PRCPRCcd2

SRLSRLcd2

SRLSRLvia2

SRLSRLcd1

SRLSRLvia1

MutualMutual1

MUTIND

RR9

RR8

RR7

ItPulseSRC5

Fall=5 nsecRise=5 nsecEdge=linearDelay=5 nsecI_High=100 AI_Low=0 A

CC5

SRLSRL2

SRLSRL1

V_DCSRC6Vdc=1 V

SRLSRL24

SRLSRL23

SRLSRL18

SRLSRL13SRL

SRLvia5

SRLSRLcd5

PRCPRCcd5

SRLSRL12

SRLSRL7

SRLSRL20

SRLSRL19

PRCPRCcd4

SRLSRLcd4

SRLSRLvia4

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SWTW-2005June 5, 2005 17

Transient response

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SWTW-2005June 5, 2005 18

AC impedance seen by load

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Improvements

Number of probes are increased. (different versions are simulated including two times the existing probe number and fullpopulated version)

Space transformer thickness optimizedDifferent probe height versions have been experimented Space transformer design improved by means of increased

via number and decoupling capacitors

Page 20: POWER DELIVERY MODEL OF TEST PROBE CARDS

SWTW-2005June 5, 2005 20

After improvements

Page 21: POWER DELIVERY MODEL OF TEST PROBE CARDS

SWTW-2005June 5, 2005 21

New technologies

New probe designs can be developed using reduced heightProbe tip design and material can be optimized to reduce contact resistance

Capacitors may be formed by dielectric layers close to probe tips reducing probe inductance effects (patent pending)

On space transformer or PCB, fast transient feedback voltage regulator can be developed [Ref 4].

Page 22: POWER DELIVERY MODEL OF TEST PROBE CARDS

SWTW-2005June 5, 2005 22

Dielectric layer

Space transformer

PCB

High dielectric coefficient material

Decoupling capacitor on PCB

Decoupling capacitor on ST Spring pinsPlane layers

Power supply

DUT (die)

Plane vias

Signal pin drill size

VCC or GND pin drill size

*patent pending

Page 23: POWER DELIVERY MODEL OF TEST PROBE CARDS

SWTW-2005June 5, 2005 23

Conclusions

High slew rate (~nS range) DUT power changes create voltage fluctuations on supply lines affecting test performance and speeds.

Power delivery improvements are possible by means of careful design of each stage

Improvement methods mainly trades with mechanical restrictions

New technologies require more elaborate research

Page 24: POWER DELIVERY MODEL OF TEST PROBE CARDS

SWTW-2005June 5, 2005 24

References[1] Y. Ren, K. Yao, Ming Xu and Fred C. Lee

“Analysis of the power delivery path from the 12-V VR to the microprocessor”IEEE transactions on power electronics, Vol 19, No.6,November 2004, pp 1507-1514.

[2] J. Mallet“High current DPS architecture for sort test challenge”2002 ITC international test conference, pp 913-922.

[3] O. Mandhana, Z. Jin. “Power delivery system performance optimization of a printed circuit board with multiple microprocessor” 2004 Electronic Components and Technology Conference, pp 581-588.

[4] L. Amoroso, M. Donati, X. Zhou and Fred C. Lee“Single shot transient suppressor (SSTS) for high current high slew rate microprocessor”in Proc, Applied Power electronics conf. expo, 1999, pp, 284-288.

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Questions

Thank you for your interest and listening.