27.01.2015 Views

Online proceedings - EDA Publishing Association

Online proceedings - EDA Publishing Association

Online proceedings - EDA Publishing Association

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

close already to the literature value of a theoretically<br />

possible 420 W/mK for pure silver.<br />

To estimate the accuracy of the method, we have<br />

calculated its sensitivity first. This can then be compared to<br />

the mean accuracy of the temperature measurement δT fitted<br />

for the three sensor values along the Cu-bar.<br />

The sensitivity of the method is expected to depend on the<br />

BLT of the TIM. The simulated curves are given in<br />

figure 21 for different TIM-conductivities and BLTs.<br />

Naturally the sensitivity is higher for the larger BLT and<br />

yields the value of S = 0.0046 mK 2 /W. With δT = 0.045 K<br />

we obtain a resolution of around δλ = ± 10 K for the thicker<br />

BLT.<br />

7-9 October 2009, Leuven, Belgium<br />

introduced by the technological modifications. The accuracy<br />

obtainable at low bond-line thicknesses and highly<br />

conductive interface materials is evaluated and commented<br />

on. More results will follow and be presented soon in<br />

another paper, encompassing also reliability aspects of the<br />

new technologies.<br />

ACKNOWLEDGMENTS<br />

The authors appreciate the support of the EU FP 7<br />

Integrated Project “Nanopack”. Further thanks go to the<br />

authors’ Fraunhofer colleagues A. Gollhardt, S. Huber,<br />

M. Koch, K.-F. Becker, T. Braun and M. von Suchodolez.<br />

∆T [K]<br />

0.12<br />

0.10<br />

0.08<br />

0.06<br />

0.04<br />

0.02<br />

0.00<br />

-0.02<br />

-0.04<br />

BLT = 28 µm<br />

BLT = 71 µm<br />

390 395 400 405 410 415 420<br />

λ Ag<br />

[W/mK]<br />

Fig 21: Sensitivity of measurements for two different BLT<br />

For the thinner BLT we obtain δλ = ± 20 W/mK. This<br />

means that preferably thick BLTs should be used during<br />

characterisation. However, large BLTs of Ag powder are<br />

difficult to realise technologically.<br />

CONCLUSIONS & OUTLOOK<br />

In this paper we have stressed the need for advanced<br />

thermal interface technology and presented two approaches<br />

to process and characterize theses structures. A so-called<br />

“nano-sponge” technology has been introduced with<br />

interesting structural, mechanical and thermal features to<br />

enhance heat transfer across the interface. Nanoindentation<br />

has been used to verify the increased deformability of the<br />

sponge to possibly allow enhanced contact to filler particles.<br />

A second technology using Ag-powder on Ag surface<br />

metallisation has been presented and tested successfully<br />

thermally and mechanically.<br />

It has also been pointed out that usually a variety of<br />

characterisation methods is made necessary as each new<br />

interface technology has to be thermally measured as<br />

processed in the real device. In this vein two test stands have<br />

been designed and developed to measure the effect<br />

REFERENCES<br />

[1] R. Viswanath, V. Wakharkar, A. Watwe and V.<br />

Lebonheur. Thermal Performance Requirements from<br />

Silicon to Systems. Intel Technology Journal Q3, pp. 1-<br />

16, 2000.<br />

[2] S.V. Garimella, Y.K. Joshi, A. Bar-Cohen, R. Mahajan,<br />

K.C. Toh, V.P. Baelmans, J. Lohan, B. Sammakia, and<br />

F. Andros. Thermal challenges in next generation<br />

electronic systems – summary of panel presentations<br />

and discussions. IEEE Trans. Components and<br />

Packaging Technologies, 25(4), pp. 569–575, 2002.<br />

[3] Liu, Y., S. Irving, T. Luk, and D. Kinzer. Trends of<br />

Power Electronics Packaging and Modeling. Proc. 10th<br />

EPTC, 2008.<br />

[4] M. Rencz. Testing interface thermal resistance, Proc.<br />

9th EPTC, 2007.<br />

[5] R. Schacht, D. May, B. Wunderle, O. Wittler, A.<br />

Gollhardt, B. Michel and H. Reichl. Characterization of<br />

Thermal Interface Materials to Support Thermal<br />

Simulation. Proc. 12th Therminic 2006, Sep 27-29,<br />

Nice, Côte d’Azur, France, 2006.<br />

[6] B. Wunderle, J. Kleff, D. May, M. Abo Ras, R. Schacht,<br />

H. Oppermann, J. Keller and B. Michel. In-situ<br />

measurement of various thin Bond-Line-Thickness<br />

Thermal Interface Materials with Correlation to<br />

Structural Features. Proc 14 th Therminic 2008, Rome,<br />

Sept 24-26 2008<br />

[7] R. Kempers, P. Kolodner, A. Lyons and A.J. Robinson.<br />

Development Of A High-Accuracy Thermal Interface<br />

Material Tester. Proc. 10 th Itherm Conf. 2008.<br />

[8] A. Devos, J.-F. Robillard, R. Côte et P. Emery. High<br />

Laser-Wavelength Sensitivity of the Picosecond<br />

Ultrasonic Response in Transparent Thin Films,<br />

Physical Review B 74, 6, 064114, 2006<br />

[9] R. J. Linderman, T. Brunschwiler, U. Kloter, H. Toy,<br />

B.Michel, Hierarchical Nested Surface Channels for<br />

Reduced Particle Stacking and Low-Resistance Thermal<br />

Interfaces, Proc. 23st IEEE SEMI-THERM Symp.,<br />

2007, pp. 87-94.<br />

[10] D.F. Rae and P. Borgesen. Optimising the automated<br />

assembly process for filled polymer-based themal<br />

bondlines. APEX 2009.<br />

[11] B. Wunderle and B. Michel. Lifetime Modeling for<br />

Microsystems Integration – from Nano to Systems. J. of<br />

©<strong>EDA</strong> <strong>Publishing</strong>/THERMINIC 2009 231<br />

ISBN: 978-2-35500-010-2

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!