Interlayer Cooling of 3D Stacked ICs - Microelectronic Systems ...
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Interlayer Cooling of 3D Stacked ICs - Microelectronic Systems ...
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Master Project<br />
<strong>Microelectronic</strong> <strong>Systems</strong> Laboratory<br />
<strong>Interlayer</strong> cooling <strong>of</strong> <strong>3D</strong> stacked IC<br />
<strong>3D</strong> Integration Strategies – Heat Transfer Stack<br />
January 2009<br />
Student: Supervisors: Pr<strong>of</strong>essor:<br />
Alexandre Pascarella Fengda Sun, Yuksel Temiz Yusuf Leblebici<br />
SMT LSM LSM
<strong>Interlayer</strong> cooling <strong>of</strong> <strong>3D</strong> stacked IC<br />
Abstract<br />
In a <strong>3D</strong> chip, power density must be taken in account as a major parameter. Thermal<br />
management inside <strong>of</strong> a <strong>3D</strong> stacked integrated circuit (<strong>of</strong>ten reported as <strong>3D</strong>-SIC) cannot be<br />
solved with actual external cooling techniques. To overcome this limitation, current<br />
researches lead to the use <strong>of</strong> a single phase or two-phase flow interlayer cooling directly<br />
integrated through the chip. The idea is to use thermal properties <strong>of</strong> liquids or two-phase<br />
flows to carry out the heat from the <strong>3D</strong> stack with the use <strong>of</strong> a structured interface between<br />
each tier and in a microscale level.<br />
This work is mainly dedicated to the design and fabrication <strong>of</strong> a test setup to characterize heat<br />
transfer capabilities <strong>of</strong> integrated interlayer cooling systems and to validate thermal models <strong>of</strong><br />
microstructured heat exchangers.<br />
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<strong>Interlayer</strong> cooling <strong>of</strong> <strong>3D</strong> stacked IC<br />
Table <strong>of</strong> contents:<br />
1 INTRODUCTION ....................................................................................................................................... 7<br />
1.1 <strong>3D</strong> INTEGRATION TECHNOLOGY AND STACKED LAYERS APPROACH........................................................... 8<br />
1.2 PROJECT DESCRIPTION ............................................................................................................................... 9<br />
2 CLEAN ROOM EQUIPMENTS .............................................................................................................. 10<br />
2.1 LASER LITHOGRAPHY SYSTEM - HEIDELBERG DWL200 .......................................................................... 10<br />
2.2 MASK AND THICK POSITIVE RESIST DEVELOPER - DV10 .......................................................................... 10<br />
2.3 WET BENCHES ......................................................................................................................................... 11<br />
2.4 AUTOMATIC RESIST PROCESSING CLUSTER – EVG 150 .......................................................................... 12<br />
2.5 DOUBLE SIDE MASK ALIGNER – MA6 ...................................................................................................... 12<br />
2.6 E-GUN AND THERMAL EVAPORATOR – LEYBOLD - OPTICS LAB 600 H ................................................... 12<br />
2.7 HIGH VACUUM SPUTTER CLUSTER SYSTEM – PFEIFFER SPIDER 600 ....................................................... 13<br />
2.8 PLASMA ETCHER - AMS 200 DSE (DIELECTRIC AND SILICON ETCHER) ................................................. 14<br />
2.9 MANUAL PROBER STATION – KARL SÜSS PM8 ....................................................................................... 16<br />
3 FIRST EXPERIMENTS IN <strong>3D</strong> DESIGNS ............................................................................................. 17<br />
3.1 HEATING <strong>3D</strong> STACKED CHIP .................................................................................................................... 17<br />
3.1.1 Microheaters ................................................................................................................................. 18<br />
3.1.2 Resistance Temperature Detectors (RTDs) ................................................................................... 20<br />
3.1.3 Layout design ................................................................................................................................ 21<br />
3.1.4 Materials, methods and processes ................................................................................................. 27<br />
3.1.5 Results ........................................................................................................................................... 31<br />
3.2 WAFER THINNING .................................................................................................................................... 35<br />
3.2.1 Grinding and polishing machine ................................................................................................... 35<br />
3.2.2 Thinning experiments .................................................................................................................... 36<br />
3.2.3 Results ........................................................................................................................................... 36<br />
4 HEAT TRANSFER SETUP ..................................................................................................................... 40<br />
4.1 HEAT TRANSFER STACK ........................................................................................................................... 41<br />
4.1.1 Heat transfer ................................................................................................................................. 42<br />
4.1.2 Layout design ................................................................................................................................ 43<br />
4.1.3 Materials, methods and processes ................................................................................................. 51<br />
4.2 PCB ......................................................................................................................................................... 55<br />
4.3 HOUSING COMPONENTS ........................................................................................................................... 58<br />
4.4 RESULTS .................................................................................................................................................. 59<br />
5 CONCLUSION .......................................................................................................................................... 66<br />
6 ACKNOWLEDGMENT ........................................................................................................................... 67<br />
7 BIBLIOGRAPHY ...................................................................................................................................... 68<br />
8 APPENDICES............................................................................................................................................ 70<br />
8.1 APPENDIX A: TEMPLATE FOR SCREEN PRINTING ...................................................................................... 70<br />
8.2 APPENDIX B: EPOXY ADHESIVE ............................................................................................................... 71<br />
8.3 APPENDIX C: HOUSING COMPONENTS DESIGN SKETCHES ........................................................................ 72<br />
8.4 APPENDIX D: FLUID CONNECTORS ........................................................................................................... 74<br />
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<strong>Interlayer</strong> cooling <strong>of</strong> <strong>3D</strong> stacked IC<br />
Table <strong>of</strong> figures:<br />
Figure 1.1 : Chip-to-chip interconnect length reduction with microchannel cooled <strong>3D</strong>-<strong>ICs</strong> [17]<br />
Sekar et al. .................................................................................................................................. 7<br />
Figure 1.2 : Model for one-dimensional thermal analysis <strong>of</strong> vertically integrated circuits. [9]<br />
Kleiner et al. ............................................................................................................................... 8<br />
Figure 1.3 : A microchannel cooled <strong>3D</strong> integrated circuit [17] Sekar et al. .............................. 9<br />
Figure 2.1 : DWL200 Laser lithography system ...................................................................... 10<br />
Figure 2.2 : Mask writing system ............................................................................................. 10<br />
Figure 2.3 : DV10 Mask and thick resist developer ................................................................. 10<br />
Figure 2.4 : Wet benches .......................................................................................................... 11<br />
Figure 2.5 : EVG150 Automatic resist processing cluster ....................................................... 12<br />
Figure 2.6 : MA6 Double side mask aligner ............................................................................ 12<br />
Figure 2.7 : LAB600H Evaporator ........................................................................................... 13<br />
Figure 2.8 : Room inside .......................................................................................................... 13<br />
Figure 2.9 : SPIDER 600 sputtering system ............................................................................ 13<br />
Figure 2.10 : AMS 200 Plasma etcher ..................................................................................... 14<br />
Figure 2.11 : AMS 200 User interface ..................................................................................... 14<br />
Figure 2.12 : Reaction chamber ............................................................................................... 15<br />
Figure 2.13 : Manual prober station ......................................................................................... 16<br />
Figure 3.1: Five tier <strong>3D</strong> heating stack ...................................................................................... 17<br />
Figure 3.2 : Microheater surrounded by a resistance temperature detector (RTD) with<br />
connecting wires ....................................................................................................................... 18<br />
Figure 3.3 : 3 wires microheater ............................................................................................... 19<br />
Figure 3.4 : 4-wire measurement method ................................................................................. 20<br />
Figure 3.5 : Wafer layout ......................................................................................................... 21<br />
Figure 3.6 : Devices configurations ......................................................................................... 22<br />
Figure 3.7 : Microheaters random configuration with surrounding RTDs............................... 23<br />
Figure 3.8 : Layer_1 ................................................................................................................. 23<br />
Figure 3.9 : Layer_2 ................................................................................................................. 23<br />
Figure 3.10 : Microheaters aligned configuration with surrounding RTDs ............................. 24<br />
Figure 3.11 : RTDs dots for temperature map ......................................................................... 25<br />
Figure 3.12 : 2D and <strong>3D</strong> temperature map ............................................................................... 25<br />
Figure 3.13 : Circular RTD ...................................................................................................... 26<br />
Figure 3.14 : Microheaters random configuration with circular RTDs .................................... 26<br />
Figure 3.15 : Process flow used for a first trial with Al metallization ..................................... 28<br />
Figure 3.16 : Pads opened in a silox bath ................................................................................. 29<br />
Figure 3.17 : Al surface after pad opening in a silox bath ....................................................... 29<br />
Figure 3.18 : Final wafer after processing steps ....................................................................... 29<br />
Figure 3.19 : Screen printer EKRA .......................................................................................... 30<br />
Figure 3.20 : Screen printing : principle .................................................................................. 30<br />
Figure 3.21 : <strong>3D</strong> stacked chip, configuration n°1 .................................................................... 31<br />
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<strong>Interlayer</strong> cooling <strong>of</strong> <strong>3D</strong> stacked IC<br />
Figure 3.22 : <strong>3D</strong> stacked chip, configuration n°3 .................................................................... 31<br />
Figure 3.23 : Test setup with prober station, power supplies and multimeter ......................... 32<br />
Figure 3.24 : Probes on a stacked chip during measurement ................................................... 32<br />
Figure 3.25 : RTD response to the heat provided by its linked microheater ............................ 33<br />
Figure 3.26 : Thinning equipments. (a) rotating plate with moving arm, (b) mechanical holder,<br />
(c) complete system .................................................................................................................. 35<br />
Figure 3.27 : Assembly pr<strong>of</strong>ile and holder ............................................................................... 36<br />
Figure 3.28 : 100µm thick thinned Si component with TSVs .................................................. 36<br />
Figure 3.29 : Holes dry etched in silicon and opened on the other side by thinning (depth:<br />
100µm, diameter 100µm) ........................................................................................................ 37<br />
Figure 3.30 : Holes dry etched in silicon and opened on the other side by thinning (depth:<br />
100µm, diameter 50µm) .......................................................................................................... 38<br />
Figure 3.31 : 50µm diameter hole opened by thinning ............................................................ 39<br />
Figure 4.1 : Heat transfer device with integrated fluid path (on the right: cross section in a<br />
fluid opening) ........................................................................................................................... 40<br />
Figure 4.2 : Heat transfer single layer. (a) Single die with microheater and fluid openings, (b)<br />
structured backside ................................................................................................................... 40<br />
Figure 4.3 : Pr<strong>of</strong>ile <strong>of</strong> the <strong>3D</strong> stacked heat transfer setup ........................................................ 41<br />
Figure 4.4 : In-line flow and corner flow configurations (orange: microheaters; blue: fluid<br />
paths) ........................................................................................................................................ 41<br />
Figure 4.5 : Schematic <strong>of</strong> the thermal circuit with a microchannel [16] Koo et al. ................. 42<br />
Figure 4.6 : 80Ω multi-wires rectangular microheater with RTD in the middle part for in-line<br />
flow configuration .................................................................................................................... 43<br />
Figure 4.7 : 80Ω multi-wires square microheater with RTD in the middle part for corner flow<br />
configuration ............................................................................................................................ 43<br />
Figure 4.8 : Layer 1 (top layer) for in-line flow heat transfer stack ......................................... 44<br />
Figure 4.9 : Layer 1 (top layer) for corner flow heat transfer stack ......................................... 45<br />
Figure 4.10 : Layer 2 with microheaters for in-line flow heat transfer stack ........................... 46<br />
Figure 4.11 : Layer 2 with microheaters for corner flow heat transfer stack ........................... 47<br />
Figure 4.12 : Pad configuration for a microheater and its sensor............................................. 48<br />
Figure 4.13 : Wafer layout for in-line flow heat transfer stack ................................................ 49<br />
Figure 4.14 : Wafer layout for corner flow heat transfer stack ................................................ 50<br />
Figure 4.15 : Front side and backside alignment marks ........................................................... 50<br />
Figure 4.16 : Process flow for microchannels, pin fin and fluid openings dry etching ........... 52<br />
Figure 4.17 : Recipes used for SiO 2 and Si dry etching with AMS 200 .................................. 53<br />
Figure 4.18 : Schematic process for polyimide bonding .......................................................... 54<br />
Figure 4.19 : Chip assembled to a small PCB and mounted on a larger one ........................... 55<br />
Figure 4.20 : Chip and connectors footprints on small PCB .................................................... 55<br />
Figure 4.21 : Connecting wires from bonding pads to connectors on small PCB. Red lines:<br />
PCB front side. Blue lines: PCB backside. .............................................................................. 55<br />
Figure 4.22 : Pads configuration. On the left : pads from stacked chip. On the right : pads<br />
from PCB .................................................................................................................................. 56<br />
Figure 4.23 : Wire bonding configuration for a microheater and its sensor ............................ 57<br />
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<strong>Interlayer</strong> cooling <strong>of</strong> <strong>3D</strong> stacked IC<br />
Figure 4.24 : Polymer components. (a) housing for in-line flow chip, (b) housing for corner<br />
flow chip, (c) housing for in-line flow chip with push-in fluid connections, (d) housing for<br />
corner flow chip with push-in fluid connections ...................................................................... 58<br />
Figure 4.25 : Aluminum evaporation on platinum thin film (400nm Al on 200nm Pt) ........... 59<br />
Figure 4.26 : Non-uniformity and delamination after oxide sputtering ................................... 59<br />
Figure 4.27 : Alternative layout for Al layer ............................................................................ 60<br />
Figure 4.28 : Al stripes on leads ............................................................................................... 60<br />
Figure 4.29 : Al stripes evaporation on platinum thin film (400nm Al on 200nm Pt) ............. 60<br />
Figure 4.30 : Al stripes on platinum thin film and 1mm 2 square Al single layer, both after<br />
oxide sputtering ........................................................................................................................ 61<br />
Figure 4.31 : Ti/Pt/Al/SiO2 and Al/SiO2 surfaces comparison ............................................... 61<br />
Figure 4.32 : 200µm deep microchannels dry etched on wafer backside and linked to the fluid<br />
opening ..................................................................................................................................... 62<br />
Figure 4.33 : 200µm high pillars dry etched on wafer backside and linked to the fluid opening<br />
.................................................................................................................................................. 62<br />
Figure 4.34 : Microchannels and fluid opening ....................................................................... 63<br />
Figure 4.35 : Pin fin and fluid opening .................................................................................... 63<br />
Figure 4.36 : Pillars network .................................................................................................... 64<br />
Figure 4.37 : Pillars with higher magnification ........................................................................ 64<br />
Figure 4.38 : Right-angled microchannels ............................................................................... 65<br />
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<strong>Interlayer</strong> cooling <strong>of</strong> <strong>3D</strong> stacked IC<br />
1 Introduction<br />
Meet the requirements ever more demanding needed for high performance chips while scaling<br />
down the dimensions brings new technological challenges. Indeed, miniaturization and<br />
density increase start to reach some limits with planar technology. Top-down micr<strong>of</strong>abrication<br />
technologies which are widely used nowadays are facing more and more to physical limits<br />
due to the scaling <strong>of</strong> the components as well as the resolution limits <strong>of</strong> photolithography<br />
processes; while bottom-up micro or nan<strong>of</strong>abrication technologies, whose some are probably<br />
promising, have not yet reached a sufficient stage <strong>of</strong> development. Therefore, exploiting the<br />
third dimension available by stacking some vertically interconnected layers seems to be a<br />
solution in the middle able to push away some limitations and <strong>3D</strong> integration technologies<br />
that are arising might become fundamental for next chips generations.<br />
This type <strong>of</strong> technology should enable to overlay the components and by the way to increase<br />
the density per “surface” unit, avoiding precisely to stay in one horizontal surface. But<br />
advantages are multiple, and one <strong>of</strong> the main is the opportunity to shorten the electrical<br />
connections, resulting in faster operations with logic and memory stacked one upon the other<br />
for example. Heterogeneous integration brings completely new approaches for system<br />
designs.<br />
Figure 1.1 : Chip-to-chip interconnect length reduction with<br />
microchannel cooled <strong>3D</strong>-<strong>ICs</strong> [17] Sekar et al.<br />
To go further in the development <strong>of</strong> devices with a very high integration level, heat<br />
dissipation must be taken in account as an essential parameter among other critical<br />
considerations. Potential powerful new architectures could be realized, but to make the most<br />
<strong>of</strong> <strong>3D</strong> integration, a suitable and reliable cooling solution must be implemented to remove the<br />
dissipated heat from the chip. Even more than in a common chip, high power densities will<br />
stand in a <strong>3D</strong>-IC stack and the dissipated heat must be pulled out as well from the center part<br />
<strong>of</strong> the chip as from the surfaces. Each die will dissipate heat that added on the same surface<br />
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<strong>Interlayer</strong> cooling <strong>of</strong> <strong>3D</strong> stacked IC<br />
cannot still be removed by standard air cooling systems. T.Brunschwiler et al. demonstrated<br />
the limitations <strong>of</strong> back-side heat removal for <strong>3D</strong> stacked layers and the necessity to use an<br />
advanced cooling system [15]. Then, to enhance heat transfer capabilities <strong>of</strong> a cooling system,<br />
it should be in this case directly integrated in the device instead <strong>of</strong> acting as an external<br />
interface. A conceivable way to cool down a multi-level chip or processor may be with the<br />
use <strong>of</strong> an interlayer fluid flow between the stack levels. Single-phase liquid or two-phase flow<br />
convective cooling directly through the chip might provide an efficient heat transfer.<br />
This project is mainly dedicated to the design and fabrication <strong>of</strong> a test setup for thermal<br />
modeling <strong>of</strong> <strong>3D</strong>-<strong>ICs</strong>.<br />
1.1 <strong>3D</strong> integration technology and stacked layers approach<br />
<strong>3D</strong> architectures can lead to powerful applications and have a great potential to increase<br />
electrical performances <strong>of</strong> miniaturized systems. To go further in high integration level and<br />
components miniaturization, stacked dies with vertical interconnections can be an issue to<br />
many technological limitations imposed by planar designs.<br />
Key technologies that must be developed and implemented to realize <strong>3D</strong> chips are mainly the<br />
vertical connections through silicon dies and the thermal management <strong>of</strong> the <strong>3D</strong> stack.<br />
Another concern is the fact that this kind <strong>of</strong> technology compels to work with very thin layers<br />
required for vertical interconnections.<br />
With miniaturization, power density increases and heat removal becomes less efficient. The<br />
heat has smaller thermally conducting paths to be extracted from dense power dissipating<br />
zones resulting in a higher thermal resistance. This concern becomes even more relevant<br />
when thinking about <strong>3D</strong> integration with several levels. And each die is composed <strong>of</strong> several<br />
material layers with different thermal conductivities. Silicon is much more conductive<br />
compared to SiO 2 . Then in an intermediate level <strong>of</strong> a CMOS <strong>3D</strong> chip, a thin silicon layer will<br />
be enclosed between two oxide layers with a lower thermal conductivity and acting as a<br />
barrier for heat transfer.<br />
Figure 1.2 : Model for one-dimensional thermal analysis <strong>of</strong> vertically<br />
integrated circuits. [9] Kleiner et al.<br />
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<strong>Interlayer</strong> cooling <strong>of</strong> <strong>3D</strong> stacked IC<br />
To solve this problem, current researches [15] [17] lead to the use <strong>of</strong> a single phase or twophase<br />
flow interlayer cooling directly integrated through the chip. The idea is to create a<br />
cooling interface between each single die to carry out the heat from the center part <strong>of</strong> the chip.<br />
This cooling interface must be compatible with electronic components and with a high density<br />
vertical interconnection network like TSVs that will be needed in a functional chip.<br />
Figure 1.3 : A microchannel cooled <strong>3D</strong> integrated<br />
circuit [17] Sekar et al.<br />
Another advantage <strong>of</strong> these kinds <strong>of</strong> integrated cooling systems is that they let the opportunity<br />
to use a larger area on the top surface <strong>of</strong> the chip for an optical or radio frequency access<br />
instead <strong>of</strong> using this surface for heat removal covered with a heat sink.<br />
1.2 Project description<br />
This project has been done in two phases. First, a design has been done to build a first <strong>3D</strong><br />
stack with microheaters and thermal sensors on each die. Microheaters were placed to emulate<br />
the power dissipated by a CMOS chip. The goal was to have heating elements on each level to<br />
characterize the heat distribution and spreading inside <strong>of</strong> the stack on each layer. These first<br />
experiments were also the opportunity to learn how to use equipments for micr<strong>of</strong>abrication<br />
steps and test the process flow on a wafer level. Stacking has then been done on a die level.<br />
Second part <strong>of</strong> the project was to build a heat transfer setup with an integrated fluid cooling<br />
system. The starting point to do this is the work <strong>of</strong> T. Brunschwiler et al. presented in the<br />
paper “Forced convective interlayer cooling in vertically integrated packages” [15]. This<br />
paper shows comparisons and heat transfer capabilities <strong>of</strong> microstructures suitable for<br />
interlayer cooling and compatible with vertical interconnections.<br />
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<strong>Interlayer</strong> cooling <strong>of</strong> <strong>3D</strong> stacked IC<br />
2 Clean Room Equipments<br />
Many steps <strong>of</strong> the project relating to micr<strong>of</strong>abrication and requiring clean room equipments<br />
have been done at the Center <strong>of</strong> MicroNanoTechnology (CMI) from EPFL. This section<br />
presents firstly an overview <strong>of</strong> the main tools used throughout the project in the clean room.<br />
For these machines, trainings have been <strong>of</strong>fered by the CMI’s staff to allow using them<br />
independently and in a safe and right manner.<br />
2.1 Laser lithography system - Heidelberg DWL200<br />
Figure 2.1 : DWL200 Laser lithography system<br />
Figure 2.2 : Mask writing system<br />
The DWL200 equipment allows patterning optically a surface by scanning it with a laser. This<br />
laser lithography system can be used to produce chromium masks for photolithographic<br />
processes. The machine is composed <strong>of</strong> a Kr blue laser light source (Gaussian beam – 413nm<br />
wavelength) providing the power for the exposure and allow to write structures down to<br />
800nm. All tables and the XY positioning table are made <strong>of</strong> granite to guarantee the thermal<br />
stability. The mask is loaded on the table by an automated arm. [23]<br />
2.2 Mask and thick positive resist developer - DV10<br />
DV10 equipment allows the development <strong>of</strong> the<br />
masks exposed with the laser lithography system.<br />
The development liquid (developer) is put on the<br />
surface and the mask rotate with an oscillating<br />
motion during reaction time. [23]<br />
Figure 2.3 : DV10 Mask and thick resist developer<br />
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<strong>Interlayer</strong> cooling <strong>of</strong> <strong>3D</strong> stacked IC<br />
2.3 Wet Benches<br />
Chromium etching, resist stripping, lift-<strong>of</strong>f and oxide wet etching have been done with wet<br />
benches.<br />
Wet bench for oxide and metal etch: this bench has among others a bath dedicated to wet<br />
etching <strong>of</strong> Cr and Cr oxide with photoresist mask. The bath is an acid/oxidizer solution <strong>of</strong><br />
perchloric acid, cerium ammonium nitrate and water (Formula: HClO 4 + Ce (NH 4 ) 2 (NO 3 ) 6 +<br />
H 2 O). Perchloric acid is a strong acid and cerium ammonium nitrate is an oxidizing agent. Cr-<br />
Etch bath is at 20°C.<br />
Wet bench for resist development and resist stripping: this<br />
bench has a bath for resist development that is a basic<br />
solution comprising tetramethylammonium hydroxide<br />
(TMAH, (CH 3 ) 4 NOH, strong base). This bath is at 20°C.<br />
The bench has two others bathes (“old” bath and “new”<br />
bath) dedicated to the photoresist stripping. They contain a<br />
solution <strong>of</strong> N-Methylpyrrolidone (NMP) that is a good<br />
solvent to dissolve polymers. These bathes are at 70°C.<br />
Wet bench for solvent: this bench has two baths dedicated<br />
to lift-<strong>of</strong>f. These baths are NMP solution (remover 1165) at<br />
room temperature. One is a static bath while the other has<br />
activation and an ultrasonic system.<br />
Wet bench for wet etching: this bench is dedicated to oxide<br />
and metal etch, it has among others a Silox (Pad etch) bath<br />
selective to Al that has been used for pad opening.<br />
Figure 2.4 : Wet benches<br />
On each wet bench, specific baskets are dedicated to rinse the samples. First rinse (Quik<br />
Dump and Rince - QDR) is cycles <strong>of</strong> a DI water shower and N 2 agitation. Final rinse (Ultra<br />
Clean - UC) is a bath <strong>of</strong> DI water with resistivity measurement <strong>of</strong> the bath.<br />
On some benches these baskets are FFR (Fast Fill Rinse) and TT (Trickle Tank).<br />
The drying <strong>of</strong> the samples can be done with a N 2 gun for masks and with spinners for wafers<br />
or with spin-rinse-dryer (SRD). [23]<br />
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<strong>Interlayer</strong> cooling <strong>of</strong> <strong>3D</strong> stacked IC<br />
2.4 Automatic Resist Processing Cluster – EVG 150<br />
This equipment is an automatic coater and<br />
developer system.<br />
The cluster comprises cassette carriers for loading<br />
unloading the wafers, an automated arm,<br />
hotplates, a coater module (spinner chuck with<br />
two resist dispense arms: resist lines or spray<br />
coating), a developer module and a coolplate. [23]<br />
2.5 Double side mask aligner – MA6<br />
Figure 2.5 : EVG150 Automatic resist processing<br />
cluster<br />
This tool allows the alignment between a mask<br />
and the top or back side <strong>of</strong> a wafer and the UV<br />
exposure <strong>of</strong> the photoresist to transfer the<br />
desired pattern.<br />
Figure 2.6 : MA6 Double side mask aligner<br />
Microscopes with cameras allow the alignment<br />
on a screen splitted into two parts for each side<br />
(left and right) <strong>of</strong> the wafer. Main parameters<br />
that can be set are the exposure time, the power<br />
<strong>of</strong> the UV source and the proximity (gap<br />
between mask and wafer) or contact mode. [23]<br />
2.6 E-gun and thermal evaporator – Leybold - Optics LAB 600 H<br />
Thin metallic or dielectric layers can be deposited on wafers with this equipment. Materials<br />
are evaporated by resistive thermal evaporation or by e-beam. High vacuum inside <strong>of</strong> the<br />
chamber (~1.10 -7 mbar) assures a very low contamination during the deposition.<br />
With the e-beam, metal is bombarded and evaporated by a high energy electrons beam. The<br />
source <strong>of</strong> electrons is created by heating a tungsten wire traveled by a current. A high voltage<br />
difference accelerates the electrons and these ones are deflected and guided by a magnetic<br />
field. Metal is excited by the beam focused on its surface, kinetic energy <strong>of</strong> the electrons is<br />
converted into heat at the impact point and allows the evaporation.<br />
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<strong>Interlayer</strong> cooling <strong>of</strong> <strong>3D</strong> stacked IC<br />
Figure 2.7 : LAB600H Evaporator<br />
Figure 2.8 : Room inside<br />
The distance between the evaporated material source and substrates is about 1m in high<br />
configuration, which makes this equipment especially suitable for “lift-<strong>of</strong>f” processes (but this<br />
distance can be shortened). Furthermore, substrates are rotated to ensure a good uniformity<br />
during the deposition.<br />
The preliminary step before deposition is to ensure a sufficient vacuum within the chamber.<br />
This pumping is part <strong>of</strong> the process that requires most <strong>of</strong> the time (several tens <strong>of</strong> minutes or<br />
hours for a high vacuum). The deposition itself takes a few minutes. [23]<br />
2.7 High vacuum sputter cluster system – Pfeiffer SPIDER 600<br />
SPIDER600 equipment is a multi-chamber sputtering<br />
system. It allows the deposition <strong>of</strong> metallic layers<br />
and dielectrics with good thickness uniformity. For<br />
the sputtering, a plasma is created (<strong>of</strong>ten with argon).<br />
First, vacuum is done in the chamber, then the gas is<br />
injected within it. For the deposition <strong>of</strong> metallic<br />
layers a DC potential is applied between two<br />
electrodes. Ions are accelerated by the electrical field<br />
and metallic atoms are then extracted from the target.<br />
Figure 2.9 : SPIDER 600 sputtering system<br />
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For the deposition <strong>of</strong> dielectric layers, radio frequency sputtering is used to have an<br />
alternation <strong>of</strong> the electrodes potentials that allow the deposition <strong>of</strong> an insulator.<br />
Physical sputtering and reactive sputtering (with N 2 or O 2 ) can be done depending on the<br />
application. [23]<br />
2.8 Plasma Etcher - AMS 200 DSE (Dielectric and Silicon Etcher)<br />
Figure 2.10 : AMS 200 Plasma etcher<br />
Figure 2.11 : AMS 200 User interface<br />
AMS 200 DSE is a plasma etching machine from the family <strong>of</strong> dry etching process. The<br />
technology used is a high density plasma <strong>of</strong> ICP type (Inductively Coupled Plasma) working<br />
in a temperature controlled chamber.<br />
The wafer transfer from the airlock to the plasma chamber is done automatically by an<br />
automated arm. This way enables to keep a secondary vacuum inside the reaction chamber<br />
during loading/unloading operations what saves time during process.<br />
Many kinds <strong>of</strong> specific process can be used with this plasma etcher. Parameters that can be<br />
adjusted are the followings: substrate polarization (Radio Frequency or pulsed Low<br />
Frequency), temperature (control <strong>of</strong> process stability and chamber contamination), process<br />
type, etc. All the parameters are edited through a computer interface.<br />
The center part <strong>of</strong> the machine is the reaction chamber mainly made up <strong>of</strong> an ICP source, a<br />
diffusion chamber and a substrate holder.<br />
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Figure 2.12 : Reaction chamber<br />
ICP source is composed <strong>of</strong> an antenna connected to a frequency generator placed around an<br />
alumina (dielectric, Al 2 O 3 ) cylinder. The power <strong>of</strong> the frequency generator (energy <strong>of</strong> the<br />
oscillating current, 13.56 MHz for RF mode) in the antenna induces an electromagnetic field<br />
inside <strong>of</strong> the alumina tube and thus is coupled to the plasma. The plasma is formed by<br />
collisions <strong>of</strong> energetic electrons excited by the oscillations <strong>of</strong> the electromagnetic field with<br />
neutral atoms creating ions. Only some mobile electrons are excited because the ions are too<br />
heavy to follow the variations <strong>of</strong> the magnetic field. Gases are injected in the alumina<br />
chamber and the pressure is controlled. A coil around the source generates a magnetic field to<br />
imprison the plasma and avoid losses on the walls.<br />
The diffusion chamber allows to enhance the uniformity <strong>of</strong> the plasma. Permanents magnets<br />
around the chamber generate a constant magnetic field to keep the plasma inside <strong>of</strong> it. The<br />
temperature inside the diffusion chamber is controlled (heating) for the process stability and<br />
to avoid chamber contamination.<br />
The substrate holder where the wafer is placed is controlled in temperature (-20°C to ambient<br />
temp.) which is an important parameter depending on the process used.<br />
When the etching is not operating vacuum (about 10 -7 mb) is hold inside <strong>of</strong> the chamber by<br />
pumps. During the process these pumps allows to control the pressure and thus the gas flow<br />
knowing that a high gas flow can in some cases increase the etching speed.<br />
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Gases in the reaction chamber can be the followings: (with their flow measurement in<br />
"standard cubic centimeters per minute")<br />
• SF 6 [0-1000 sccm]<br />
• C 4 F 8 [0-400 sccm]<br />
• C 4 F 8 [0-100 sccm]<br />
• CH 4 [0-100 sccm]<br />
• O 2 [0-100 sccm]<br />
• Ar [0-200 sccm]<br />
• He [0-200 sccm]<br />
During the etching a laser beam can be used to measure the etching speed <strong>of</strong> transparent<br />
layers (like SiO 2 or Si 3 N 4 ) and therefore the depth etched and to detect the end <strong>of</strong> the etching<br />
when another layer is reached (other material). Technique used is the interferometry. The<br />
laser directed on the surface (905nm) is reflected and its measured intensity is modulated<br />
depending on the layer thickness that decreases during the etching process. Thus the<br />
interferences evolve during the time creating an oscillating signal. When the transparent layer<br />
is totally etched the beam is then reflected without interferences and the intensity becomes<br />
constant showing the end <strong>of</strong> the process. [23]<br />
2.9 Manual Prober Station – Karl Süss PM8<br />
Electrical measurements have been done with a prober station. Test setup comprises<br />
micromanipulators to position thin tungsten tips on the sample surface with the help <strong>of</strong> a<br />
microscope. Tips are held at the micromanipulators arms extremity and provide the electrical<br />
contact with the sample. Micromanipulators allow moving the tips in the three axes. The table<br />
that holds the sample with a vacuum and the microscope can also be moved in every<br />
direction. [23]<br />
Figure 2.13 : Manual prober station<br />
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3 First experiments in <strong>3D</strong> designs<br />
3.1 Heating <strong>3D</strong> stacked chip<br />
The departure point <strong>of</strong> this project was to create a multi-level chip, build by stacking silicon<br />
layers one upon the other. This first stack should represent or extrapolate the thermal<br />
properties <strong>of</strong> a <strong>3D</strong> chip, without considering here its functional properties.<br />
Power dissipated in a chip is not uniform on its surface. Some elements <strong>of</strong> a microprocessor<br />
unit dissipate much more power than others. MPU hot spots per example can dissipate<br />
between 200 to 300W/cm 2 while memory only dissipates about 10W/cm 2 . [15]<br />
On each layer microheaters are placed with different configurations to simulate the heat<br />
dissipated by the integrated components <strong>of</strong> a circuit design that stands in a useful chip. Some<br />
thermal sensors are also placed in specific places as detector devices to monitor the<br />
temperature inside <strong>of</strong> the stack and check the heat dissipated and the heat interactions between<br />
neighboring microheaters. In a further setup design, these sensors should allow to observe the<br />
heat transfer capabilities <strong>of</strong> integrated cooling systems.<br />
Figure 3.1: Five tier <strong>3D</strong> heating stack<br />
The chip consists <strong>of</strong> a 1cm 2 stack made <strong>of</strong> 5 layers. Depending on the level, under layers are<br />
larger on one side, making steps, to allow to connect the heaters and sensors by wire bonding<br />
on a PCB. All pads are then on one side <strong>of</strong> the chip. This configuration enables to align the<br />
layers easily for a manual stacking with a corner angle on the opposite side.<br />
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3.1.1 Microheaters<br />
Microheaters are placed on the surface <strong>of</strong> each layer to provide heat to the device. The shape<br />
<strong>of</strong> these heaters is a serpentine wire made with thin-film technologies. Platinum has been<br />
chosen as a suitable material for its capability to operate at very high temperature, for its longterm<br />
stability and because it’s also the appropriate material for the temperature sensors which<br />
enables to manufacture these two components at the same time in a single step during the<br />
process.<br />
Figure 3.2 : Microheater surrounded by a resistance temperature detector (RTD) with connecting wires<br />
Microheaters have been designed to correspond to hot spots at the surface <strong>of</strong> the chip which<br />
represent a value <strong>of</strong> 300 W/cm 2 . Then each one <strong>of</strong> the 1mm 2 heater should dissipate 3W.<br />
Power dissipation:<br />
Resistances are designed using:<br />
= <br />
= <br />
With a platinum “bulk” resistivity <strong>of</strong>: = 10.6 ∙ 10 Ω ∙ .<br />
In this configuration, RTDs are placed around the heaters. These RTDs are designed for a<br />
value <strong>of</strong> 100 Ohm (Pt100) and are driven with a current <strong>of</strong> 1mA. External wires are placed at<br />
the end points <strong>of</strong> the RTD to measure the voltage while the two others supply the 1mA<br />
current.<br />
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Figure 3.3 : 3 wires microheater<br />
For each kind <strong>of</strong> chip on the layout a modification has been made by separating the heaters in<br />
many wires to avoid hot spots in the corners <strong>of</strong> the serpentine and enhance the temperature<br />
uniformity. With a single wire, electrons follow the shorter path due to the potential gradient<br />
in the wire and current density is larger near inside corners <strong>of</strong> the serpentine increasing power<br />
dissipation at these small areas. By separating the single wire in several others, current will be<br />
forced to follow parallel different paths and dissipate power more regularly on the surface.<br />
We can notice that the length, width (and <strong>of</strong> course thickness) <strong>of</strong> each separated wire is the<br />
same, so total current is divided by the number <strong>of</strong> wires for the same potential. Total<br />
resistance can be considered like a single wire by taking in account the spacing (subtracting)<br />
in the total metal width or like several higher resistances in parallel. On the layout, sizes and<br />
configurations are the same as those in single wire microheaters.<br />
Each group <strong>of</strong> layers on the wafer denominated with “n°a” on Figure 3.6 have this kind <strong>of</strong><br />
heaters.<br />
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3.1.2 Resistance Temperature Detectors (RTDs)<br />
Thermal sensors that have been used on each layer are Resistance Temperature Detectors<br />
(RTDs).<br />
The resistivity temperature dependence <strong>of</strong> platinum is described by the following equation:<br />
(only for positive temperatures, for negative temperatures an additional term must be<br />
included)<br />
= (1 + + )<br />
With R T the resistance at temperature T, R 0 the nominal resistance at 0 °C, α = 3.9083e -3 °C -1<br />
and β = -5.775e -7 °C -2 .<br />
Constant β is very low which means that the resistivity temperature dependence is nearly a<br />
linear characteristic (resistivity increase with temperature) making this material very suitable<br />
for sensing. Furthermore, it has a fast response time, a low drift, and can operate in a wide<br />
range <strong>of</strong> temperature.<br />
Normalized 100Ω platinum (Pt100) have been designed. In Pt100 standard, 100 Ω represents<br />
the nominal resistance at 0°C. The resistance at 20°C is then 107.8 Ω.<br />
A 4-wire measurement method has been used to sense the temperature only in the active part<br />
and to avoid the influence <strong>of</strong> the connecting wires. This method consists in measuring the<br />
voltage with two other wires at both extremities <strong>of</strong> the resistive sensor because for a voltage<br />
measurement no current flows in these wires.<br />
V<br />
I<br />
R sensor<br />
Figure 3.4 : 4-wire measurement method<br />
Pt100 can be driven by a current <strong>of</strong> 1mA.<br />
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3.1.3 Layout design<br />
Design has been done with the s<strong>of</strong>tware “CleWin” that is a computer-aided design tool.<br />
All the dimensioning has been done for a 500nm layer <strong>of</strong> platinum (which is not the metal that<br />
has been deposited in the end during the micr<strong>of</strong>abrication process).<br />
Wafer layout:<br />
Figure 3.5 : Wafer layout<br />
The wafer layout comprise three different kinds <strong>of</strong> chips with various configurations for the<br />
heaters and sensors, each one has 5 layers. For each kind <strong>of</strong> chip, a duplicate with the same<br />
design but with the multi-wires heaters as shown in Figure 3.3 is set on the layout. Finally, six<br />
chips can be done by stacking these layers; their configurations are shown in Figure 3.6.<br />
Chips must be properly aligned on the wafer to allow the dicing. The cuts are straights from<br />
one side to another. The chips must be arranged in an orthogonal network and dedicated<br />
alignment marks (crosses) must be placed regularly on the layout at the desired cutting<br />
location.<br />
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3<br />
1<br />
1a<br />
2<br />
3a<br />
2a<br />
Figure 3.6 : Devices configurations<br />
Configuration n°1: Heaters are placed randomly on the layer surface, an alternation <strong>of</strong> two<br />
random configurations allows to misalign also vertically the heaters from one layer to another.<br />
Sensors are surrounding the heaters. 1a has the same configuration but with the multi-wires<br />
heaters as shown in Figure 3.3.<br />
Configuration n°2: Heaters are aligned in the plane but also vertically out <strong>of</strong> the plane when<br />
stacking the layers. Sensors are surrounding the heaters. 2a has the same configuration but<br />
with the multi-wires heaters as shown in Figure 3.3.<br />
Configuration n°3: Heaters are placed randomly, a different random configuration has been<br />
done for each layer, so the heaters are placed randomly in the whole chip’s volume. The<br />
sensors are small dots on the surface to have a temperature map. 3a has the same<br />
configuration but with the multi-wires heaters as shown in Figure 3.3.<br />
These configurations are shown more in details in the next pages.<br />
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Configuration n°1: (random_surrounding_RTD)<br />
Figure 3.7 : Microheaters random configuration with surrounding RTDs<br />
Each layer <strong>of</strong> chip n°1 comprises 10 heaters <strong>of</strong> 1mm square (to be quite similar to small<br />
processing elements) that are filling 10% <strong>of</strong> the total surface (10x10mm 2 ). The first layer (top<br />
layer) <strong>of</strong> the chip is shown here.<br />
The heaters have been placed randomly on layer_1 and randomly on layer_2 at different<br />
places, then on the 3 rd layer, same layout than on layer_1 is again used and so on… in<br />
alternation until layer 5.<br />
Figure 3.8 : Layer_1<br />
Figure 3.9 : Layer_2<br />
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Configuration n°2: (aligned_surrounding_RTD)<br />
Figure 3.10 : Microheaters aligned configuration with surrounding RTDs<br />
Each layer <strong>of</strong> chip n°2 comprises also 10 heaters <strong>of</strong> 1mm square that are filling 10% <strong>of</strong> the<br />
total surface (10x10mm 2 ). The first layer (top layer) <strong>of</strong> the chip is shown here.<br />
Here the heaters are aligned in 3 vertical lines. The 5 layers <strong>of</strong> the stack have the same<br />
configuration so the alignment <strong>of</strong> the heaters appears also out <strong>of</strong> the plane.<br />
In this configuration, RTDs are still placed around the heaters.<br />
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Configuration n°3: (random_circular_RTD)<br />
Figure 3.11 : RTDs dots for temperature map<br />
For the 3 rd chip the sensors are small dots on the surface to give a temperature map. They are<br />
exactly at the same position on the 5 layers.<br />
A circular repartition <strong>of</strong> 9 sensors has been done to sense the temperature from the center part<br />
toward the externals.<br />
This configuration results in a <strong>3D</strong> grid map:<br />
Figure 3.12 : 2D and <strong>3D</strong> temperature map<br />
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These small dots are circular RTDs. They have been designed for a value <strong>of</strong> 100 Ω. Again a<br />
4-points measurement method is used.<br />
Figure 3.13 : Circular RTD<br />
Each layer <strong>of</strong> chip n°3 comprises also 10 heaters <strong>of</strong> 1mm square that are filling 10% <strong>of</strong> the<br />
total surface (10x10mm 2 ). The first layer (top layer) <strong>of</strong> the chip is shown here. In this design,<br />
heaters are placed randomly on the surface and their locations are different for each <strong>of</strong> the 5<br />
layers.<br />
Figure 3.14 : Microheaters random configuration with circular RTDs<br />
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3.1.4 Materials, methods and processes<br />
Masks used for photolithographic steps are “Chrome Blank 5'' Nan<strong>of</strong>ilm”. It’s a 5x5 inch<br />
square plate glass covered on one side by a thin chromium layer and a thin photoresist layer.<br />
Two masks are needed, the first one for microheaters and sensors (in blue in the layout) and<br />
the second for PADs opening (in black in the layout).<br />
They have been patterned with the laser lithography system (DWL200) and developed with<br />
the DV10 equipment. Then the chromium has been etched in the bath dedicated to wet<br />
etching <strong>of</strong> chromium. Masks are designed for positive photoresists.<br />
Wafers used were 100 ± 0.5 mm in diameter and 525 ± 25 µm thick. They have been oxidized<br />
(200nm wet oxide) as an insulation layer for the heaters and sensors. If these components<br />
were deposited directly on the silicon surface some current may flow in the semiconductor<br />
choosing non-appropriate way through the material (not following the metallic path) with an<br />
energy loss at the desired place. Other influences like Schottky diode effects may appear.<br />
For microheaters and sensors, all the design and dimensioning have been done for a 500nm<br />
platinum evaporation on the surface. These structures are created using a lift-<strong>of</strong>f process<br />
which involves a low-pressure vapor deposition (evaporation must be done instead <strong>of</strong><br />
sputtering). To do this, a large distance between source and substrates is needed for a lift-<strong>of</strong>f<br />
process (what is the case with LAB600H equipment) and then a larger amount <strong>of</strong> material is<br />
used (what is not welcome here due to high cost <strong>of</strong> platinum). As 500nm is quite large for a<br />
platinum deposition, then for a first trial aluminum has been evaporated instead <strong>of</strong> platinum to<br />
try the process.<br />
The process flow that has been used in the end is the following:<br />
Step Process description Cross-section after process<br />
01<br />
Substrate: Si 525µm<br />
Wet Oxidation<br />
Machine: Centrotherm<br />
Thickness: 200nm<br />
02<br />
Photolithography<br />
Machine: EVG 150<br />
PR : AZ1512<br />
Recipe : LOR-AZ1512 700nm<br />
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03/04<br />
Metal Evaporation + Lift-<strong>of</strong>f<br />
Machine: LAB 600 H<br />
Metal: Ti / Al<br />
Thickness: 10 nm / 0.5 µm<br />
+ Remover<br />
05<br />
Oxide sputtering<br />
Machine: SPIDER 600<br />
Thickness: 1.3 µm<br />
(0.8 µm more than Al layer)<br />
06<br />
Coating (Back Side)<br />
Oxide protection<br />
Machine: EVG 150<br />
PR : AZ1512 – 1.5µm<br />
07<br />
Photolithography<br />
Machine: EVG 150<br />
PR : AZ1512 – 1.5µm<br />
80 µm<br />
PAD<br />
100 µm<br />
08<br />
Oxide Wet Etch (SILOX)<br />
Material : Si02<br />
Machine: Wet bench SILOX<br />
Depth : 0.8 µm<br />
+ Resist Strip<br />
PAD<br />
Figure 3.15 : Process flow used for a first trial with Al metallization<br />
Aluminum is suitable for wire bonding, if platinum would have been evaporated as planed at<br />
the beginning, a s<strong>of</strong>t metal must be evaporated on it in the pad location.<br />
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First wafers have been processed with the following steps and recipes:<br />
Photolithography: AZ1512_on_LOR_700nm with EVG.<br />
Aluminum metallization with titanium adhesion layer: 10nm Ti + 500nm Al with LAB600<br />
and Lift-<strong>of</strong>f / RT / No_IS parameters.<br />
Oxide sputtering with SPIDER600. Recipe SiO2-1, duration: 30min at 42.3 nm/min.<br />
Coating backside: AZ1512 1um5_NoEBR<br />
Front side photolithography: AZ1512 1um5<br />
(Start from the backside to avoid having two times the s<strong>of</strong>tbake <strong>of</strong> useful side and recipe<br />
without solvent on the backside during coating on EVG)<br />
Wet etching in SILOX bath (pad etch) with activation.<br />
Figure 3.16 : Pads opened in a silox bath<br />
Figure 3.17 : Al surface after pad opening in a silox bath<br />
Measured resistances (with manual prober station) for Al devices:<br />
Microheater 1wire: 24.6 Ω<br />
Microheater 3wires: 24 Ω<br />
RTD surrounding: 39 Ω<br />
RTD circular: 34.7 Ω<br />
(measurements include leads<br />
resistances)<br />
Figure 3.18 : Final wafer after processing steps<br />
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Single chips have been diced with a diamond-tipped blade by an automatic dicing saw<br />
(DISCO DAD321).<br />
Stacking:<br />
To build the stack, single layers have been glued on top <strong>of</strong><br />
each other. To have a thin uniform thickness, glue has<br />
been deposited by screen printing. To do this, a semiautomatic<br />
machine (EKRA) dedicated to thick layers<br />
fabrication and suitable also for gluing has been used.<br />
These steps have been done at LPM (“Laboratoire de<br />
Production Microtechnique”) - Thick-film technology<br />
group [25].<br />
Figure 3.19 : Screen printer EKRA<br />
Figure 3.20 : Screen printing : principle<br />
The technique consists <strong>of</strong> applying the glue through a screen (a metallic grid) with the desired<br />
shape. After the removal <strong>of</strong> this screen, an array <strong>of</strong> small paste dots stands on the surface.<br />
With glue, this array changes into a uniform thin layer coating the surface.<br />
The screen must first be prepared, for this a layout with the desired shape is needed. This<br />
layout has been done simply by printing a square (on a transparent sheet to transfer it for the<br />
screen production) with the right dimensions (square dimensions just a bit smaller than the<br />
chip surface to avoid overflowing on the edges <strong>of</strong> the stack). The layout used is shown in<br />
appendix A.<br />
An epoxy resist has been used. To avoid the creation <strong>of</strong> a thermal insulating layer at the<br />
interface, the resist has been filled with alumina particles (Al 2 O 3 ) to lower the thermal<br />
resistance. Thickness deposited is around 20 - 30µm. Datasheet <strong>of</strong> the epoxy resist is shown in<br />
appendix B.<br />
Stacking itself has been done manually. For the alignment, layers have been leaned against a<br />
corner angle.<br />
Stacks have been cured 2 hours at 150°C.<br />
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3.1.5 Results<br />
Figure 3.21 : <strong>3D</strong> stacked chip, configuration n°1<br />
Figure 3.22 : <strong>3D</strong> stacked chip, configuration n°3<br />
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After the baking in an oven, first samples <strong>of</strong> <strong>3D</strong> chips are ready.<br />
The connecting side is somewhat sloping because for a first try a 525µm thick wafer has been<br />
used. (Then stacked chips are 5x525µm thick).<br />
Here, the wire bonding connection <strong>of</strong> many pads seems to be quite difficult, then some tests<br />
have been done with a prober station.<br />
Multimeter<br />
Power supply<br />
Figure 3.23 : Test setup with prober station, power supplies and<br />
multimeter<br />
Resistance temperature dependence <strong>of</strong> a sensor has been tested on the chip. As aluminum has<br />
been evaporated instead <strong>of</strong> platinum, sensor resistance is much lower than the 100Ohm<br />
expected with platinum. These tests have been done on a chip where sensors are surrounding<br />
the heaters.<br />
For the experiment, a 1mA constant current is set to drive the sensor while the voltage is<br />
measured with the two others wires at both ends <strong>of</strong> the resistance. A current from zero to 1A<br />
is set in the microheater. Then several probes are needed to do the measurements for one<br />
device.<br />
Figure 3.24 : Probes on a stacked chip during measurement<br />
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V sensor functions <strong>of</strong> I heater :<br />
V sensor [mV]<br />
40<br />
35<br />
30<br />
25<br />
20<br />
15<br />
10<br />
5<br />
0<br />
Al RTD<br />
50<br />
100<br />
150<br />
200<br />
250<br />
300<br />
350<br />
400<br />
450<br />
500<br />
550<br />
600<br />
650<br />
700<br />
750<br />
800<br />
850<br />
900<br />
950<br />
1000<br />
I heater [mA]<br />
Figure 3.25 : RTD response to the heat provided by its linked microheater<br />
The evolution <strong>of</strong> the resistance can be read directly on the voltage scale because the sensor is<br />
driven by a 1mA current. We can see that as expected the resistance increases with the<br />
temperature (typical curve for a metal). Heat provided by the microheater is the power<br />
dissipated as a function <strong>of</strong> the resistance multiplied by the square <strong>of</strong> the current:<br />
= <br />
So, increasing linearly the current increase the power dissipated as a square function and<br />
temperature variation can be considered as defined in ref. [4]:<br />
Heat generation - Heat dissipation = Change in internal energy<br />
Heat generation:<br />
= <br />
Heat dissipation: = ( )<br />
<br />
= ∆<br />
<br />
with R th : thermal resistance<br />
Change in internal energy:<br />
Equation becomes:<br />
= <br />
<br />
<br />
− ∆<br />
<br />
= <br />
<br />
<br />
with the steady state solution:<br />
∆ = ∙ <br />
Then, temperature increase also as a square function following the power dissipated.<br />
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We can notice that during this experiment, resistance <strong>of</strong> the microheater increases too with the<br />
temperature.<br />
For temperature measurement, the sensor should first be calibrated with an external heat<br />
source (a setup with a hotplate and a controlled temperature bath per example) in the range<br />
where it will be used. Meaning the creation <strong>of</strong> a table with incremented temperatures values<br />
matched to resistance values. This calibration has not been done due to lack <strong>of</strong> connections to<br />
the chip pads. Only simple measurements with the prober station were possible at that time.<br />
In Figure 3.25 the graph shows that without considering calibration and non-linearities, the<br />
resistance <strong>of</strong> the sensor increases with a curve shape corresponding to the equation for the<br />
temperature evolution as a square function <strong>of</strong> the current in the heater.<br />
In these first <strong>3D</strong> stacked chips, temperature sensors are <strong>of</strong>ten placed around the microheaters.<br />
Due to the higher thermal conductivity <strong>of</strong> silicon compared to SiO 2 , heat spreads much more<br />
in the silicon layer. The temperature pr<strong>of</strong>ile under the microheater is a radial gradient (a<br />
conduction shape factor can be defined for the thermal resistance to the substrate) and the<br />
highest temperature is in the middle <strong>of</strong> the microheater surface. Then in further setups,<br />
temperature sensors will be placed in the middle <strong>of</strong> the microheater surface to measure the<br />
maximal value <strong>of</strong> the hot spot, that will be the limit for the acceptable value in a functional<br />
chip.<br />
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3.2 Wafer thinning<br />
Building a stack to create a <strong>3D</strong> chip to take advantage <strong>of</strong> an additional dimension involves<br />
interconnections between these levels. This <strong>3D</strong> concept saves surface space but foremost<br />
shorten the length <strong>of</strong> the connections. Then multi-layer vertical interconnections must be<br />
created directly through the silicon to link the levels, requiring therefore very thin layers.<br />
Thinning experiments have been done on chip level to reduce the thickness <strong>of</strong> small cleaved<br />
silicon parts from a wafer where TSV shapes were previously dry etched. The goal was to<br />
check the feasibility <strong>of</strong> opening the holes in an experimental way by thinning the backside <strong>of</strong><br />
the silicon sample to reach the bottom holes and make real vias.<br />
3.2.1 Grinding and polishing machine<br />
To thin the silicon sample, a grinding and polishing machine has been used. This machine is<br />
composed <strong>of</strong> a rotating plate, a moving arm and a cylindrical mechanical system.<br />
(a) (b) (c)<br />
Figure 3.26 : Thinning equipments. (a) rotating plate with moving arm, (b) mechanical holder, (c) complete system<br />
The sample is held in the center part under the mechanical system with a polishing resist. A<br />
spring allows to adjust the force applied with which the sample is pressed on the rotating<br />
plate. The sample is thinned and polished on a silicon carbide paper. Several grain sizes can<br />
be used progressively during the process. Lubrication is done with water.<br />
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3.2.2 Thinning experiments<br />
The goal was to thin a small silicon part down to 100µm to open the holes etched on its<br />
surface. To hold the sample a polishing resist is used, this resist is hard at room temperature<br />
and must be s<strong>of</strong>ten to be applied. To do this, it’s the metallic holder that has been heated with<br />
a hotplate (set at 150°C). A first test has been done by gluing the sample on the holder with<br />
the polishing resist that has shown significant erosion due to water lubrication and stress on<br />
the material. To avoid this, the sample has been prepared to be more protected during the<br />
thinning. First, it has been laid on “blue tape” to protect the holes. Then to hold it, a resist<br />
frame has been set to maintain the blue tape and to protect the edges <strong>of</strong> the sample. Like this,<br />
no resist remains under the sample, which enhances flatness.<br />
Holder<br />
Figure 3.27 : Assembly pr<strong>of</strong>ile and holder<br />
Original sample thickness was 525mµ.<br />
Thicknesses have been measured throughout the grinding and polishing process on five<br />
different points <strong>of</strong> the sample (center and corners) with a digital dial gauge. Thinning speed<br />
depends on grain size, spring force (a counterweight can be used to fasten the process at the<br />
beginning) and table rotation speed. The rates were situated between some µm / 10 min and<br />
45 µm / 10 min.<br />
3.2.3 Results<br />
The result is a very thin silicon slice. The surface is shiny and reflecting. A 100µm thickness<br />
has been reached with openings on both sides making an array <strong>of</strong> through silicon vias.<br />
Figure 3.28 : 100µm thick thinned Si component with TSVs<br />
Holes are shown more in details in the next pages.<br />
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Holes diameter: 100µm<br />
Frontside<br />
Backside (thinned side)<br />
Figure 3.29 : Holes dry etched in silicon and opened on the other side by thinning (depth: 100µm, diameter 100µm)<br />
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Holes diameter: 50µm<br />
Frontside<br />
Backside (thinned side)<br />
Figure 3.30 : Holes dry etched in silicon and opened on the other side by thinning (depth: 100µm, diameter 50µm)<br />
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<strong>Interlayer</strong> cooling <strong>of</strong> <strong>3D</strong> stacked IC<br />
Figure 3.31 : 50µm diameter hole opened by thinning<br />
A zoom on a 50µm diameter hole shows that it is a bit more affected by the polishing than a<br />
100µm hole. However, the general shape and functionality is still preserved.<br />
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4 Heat Transfer Setup<br />
To build a heat transfer setup with an integrated cooling system, a new design has been done.<br />
Figure 4.1 : Heat transfer device with integrated fluid path (on the<br />
right: cross section in a fluid opening)<br />
The setup is composed <strong>of</strong> the chip stack glued and wire bonded to a printed circuit board.<br />
Microheaters provide the heat while backside microstructured cooling paths are integrated to<br />
study their heat transfer capabilities when dies are stacked in a complete system. A polymer<br />
housing component with fluid inlet/outlet and fluid connections will be placed on the top <strong>of</strong><br />
the stack to lead the cooling fluid directly through the chip. Fluid openings are integrated in<br />
the chip. Structured interlayer opens on these fluid inlets/outlets.<br />
(a)<br />
(b)<br />
Figure 4.2 : Heat transfer single layer. (a) Single die with microheater and fluid openings, (b) structured backside<br />
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<strong>Interlayer</strong> cooling <strong>of</strong> <strong>3D</strong> stacked IC<br />
4.1 Heat transfer stack<br />
Figure 4.3 : Pr<strong>of</strong>ile <strong>of</strong> the <strong>3D</strong> stacked heat transfer setup<br />
The stack is composed <strong>of</strong> five layers. The three layers in the middle have microheaters and<br />
sensors on one side and microstructured cooling pattern on the other side. The top layer is<br />
only structured on the backside but without heaters on the front side while the bottom layer is<br />
only the base <strong>of</strong> the stack.<br />
Two kinds <strong>of</strong> chips have been designed, one with a straight fluid path and another with a fluid<br />
path making a bend on the surface to carry the flow from one side to the perpendicular side <strong>of</strong><br />
the chip.<br />
Figure 4.4 : In-line flow and corner flow configurations (orange: microheaters; blue: fluid paths)<br />
The heat transfer area is 10x10mm 2 and the haters are placed in line for the straight flow and<br />
in square for the corner flow. To sense the temperature, RTDs are again set, this time in the<br />
center <strong>of</strong> each heater.<br />
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<strong>Interlayer</strong> cooling <strong>of</strong> <strong>3D</strong> stacked IC<br />
For each kind <strong>of</strong> chip, two cooling patterns are placed on the backside <strong>of</strong> the 10x10mm 2 heat<br />
transfer area. One is parallel microchannels, the other is a pillar array (pin fin). These patterns<br />
are microstructured by dry etching.<br />
Each layer comprises four heaters. Total area covered by the heaters is 4x10% = 40% <strong>of</strong> the<br />
heat transfer area. (4x10mm 2 )<br />
Power density wanted for these hot zones is 200W/cm 2 . Then, the power <strong>of</strong> each 10mm 2<br />
heater is 20W (80W per level, 240W per stack).<br />
4.1.1 Heat transfer<br />
Heat transfer model <strong>of</strong> the stack involves heat sources from the CMOS layers, various thermal<br />
resistances for each layer and interface (here Si, SiO 2 and cooling fluids). Conductive and<br />
convective heat transfer must be taken in account in the model. Koo et al. investigate a one<br />
dimensional heat transfer analysis for a microchannel interlayer cooling with the previously<br />
mentioned parameters [16].<br />
Figure 4.5 : Schematic <strong>of</strong> the thermal circuit with a<br />
microchannel [16] Koo et al.<br />
Heat transfer capabilities <strong>of</strong> the microstructured interlayer patterns are dependant <strong>of</strong> structures<br />
geometries. As presented in the paper “Forced convective interlayer cooling in vertically<br />
integrated packages” [15] from IBM, in-line pin fin has shown interesting heat transfer<br />
properties. Chip with perpendicular fluid openings and in line pin fin has been designed to<br />
have a test setup for their new ongoing porous media approach researches. The 10x10mm 2<br />
heat transfer area has been chosen to be in accordance with the thermal model.<br />
Single-phase liquid or two-phase flow advanced cooling techniques can be used. Heat transfer<br />
efficiency will depend on many parameters that are not exactly defined at this stage <strong>of</strong> the<br />
project. De-ionized water or specific refrigerants may be used.<br />
Dimensions <strong>of</strong> structures must also be taken in account for pressure drop considerations and<br />
flow rate.<br />
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4.1.2 Layout design<br />
The new design mainly comprises the microheaters, thermal sensors and the fluid paths. For<br />
the heating and sensing elements, all the dimensioning has been done for a 200nm layer <strong>of</strong><br />
platinum.<br />
Microheaters and RTDs (PT100) are set on three layers in the middle <strong>of</strong> the stack. Heaters are<br />
designed as a 80 Ohm resistance for a voltage up to 40V and a current <strong>of</strong> 0.5A per heater. The<br />
serpentine wire is divided into five lines to avoid hot spots in the corners.<br />
The sensor is located in heater center with its 4 connecting wires on the side.<br />
Figure 4.6 : 80Ω multi-wires rectangular microheater with RTD in the middle part for in-line flow configuration<br />
For devices with a straight flow, 80Ω rectangular heaters are placed on the surface.<br />
Dimensions are 2x5mm 2 .<br />
Figure 4.7 : 80Ω multi-wires square microheater with RTD in the middle part for corner flow configuration<br />
For devices with a corner flow, 80Ω square heaters are placed on the surface. Dimensions are<br />
3.16x3.16mm 2 .<br />
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<strong>Interlayer</strong> cooling <strong>of</strong> <strong>3D</strong> stacked IC<br />
Layer 1 (top layer) in_line_flow: (layouts are shown here for microchannels, same layouts<br />
have been done for pin fin)<br />
20mm<br />
16mm<br />
Opening in<br />
housing<br />
Fluid connection diameter:<br />
2.4mm<br />
Nut diameter (<strong>of</strong><br />
fluid connection)<br />
Figure 4.8 : Layer 1 (top layer) for in-line flow heat transfer stack<br />
Light-blue is the fluid inlet/outlet. This layer is etched through the whole wafer thickness. In<br />
blue: microchannels (width: 50µm, pitch: 100µm). They cover the 10x10mm 2 heat transfer<br />
area and overlap a bit these openings to guarantee the channels opening. Other marks give<br />
only information about the housing component that covers the stack for the fluid circuit.<br />
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<strong>Interlayer</strong> cooling <strong>of</strong> <strong>3D</strong> stacked IC<br />
Layer 1 (top layer) corner_flow:<br />
20mm<br />
20mm<br />
Fluid barrier<br />
Opening in housing<br />
(tool diameter: 4mm)<br />
M5<br />
Fluid connection diameter:<br />
2.4mm<br />
Nut diameter (<strong>of</strong><br />
fluid connection)<br />
Figure 4.9 : Layer 1 (top layer) for corner flow heat transfer stack<br />
In the second layout, microchannels (width: 50µm, pitch: 100µm) make straight-angles<br />
between the two perpendicular openings.<br />
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<strong>Interlayer</strong> cooling <strong>of</strong> <strong>3D</strong> stacked IC<br />
Layer 2 in_line_flow:<br />
Figure 4.10 : Layer 2 with microheaters for in-line flow heat transfer stack<br />
Leads have been designed as large as possible to avoid power dissipation on other zones than<br />
on desired areas. Doing this for the platinum layer, two leads are still 10% (8Ω) <strong>of</strong> the total<br />
heater resistance. To decrease this value, aluminum can be evaporated on the leads (dark<br />
layer). Heat transfer area (10x10mm 2 ) is delimited by the microchannels in the center part<br />
(blue lines).<br />
Next two under layers have the same design but pads are shifted on the right (800µm) for<br />
stacking with a stair shape.<br />
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<strong>Interlayer</strong> cooling <strong>of</strong> <strong>3D</strong> stacked IC<br />
Layer 2 corner_flow:<br />
Figure 4.11 : Layer 2 with microheaters for corner flow heat transfer stack<br />
On the second layout, the four microheaters are placed in a square arrangement. Sensors are<br />
again placed in the middle <strong>of</strong> the heaters surfaces. Fluid openings are smaller to separate them<br />
at the corner down on the left. Heat transfer area (10x10mm 2 ) is delimited by the<br />
microchannels (blue lines). Leads and pads are larger than in the in-line chip.<br />
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<strong>Interlayer</strong> cooling <strong>of</strong> <strong>3D</strong> stacked IC<br />
Connections and pads are on the right side: (example for one heater and its sensor on<br />
in_line_flow layout)<br />
1mA<br />
500mA<br />
800µm<br />
Figure 4.12 : Pad configuration for a<br />
microheater and its sensor<br />
The width <strong>of</strong> the pad is a critical dimension because it must provide a sufficient area for the<br />
wire bonding. Many wires must be bonded to handle a 500mA current needed for the heater.<br />
All pads are addressable individually.<br />
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<strong>Interlayer</strong> cooling <strong>of</strong> <strong>3D</strong> stacked IC<br />
Final layouts:<br />
Four kinds <strong>of</strong> chips have been designed:<br />
- In_line_flow with microchannels<br />
- In_line_flow with pin fin<br />
- Corner_flow with microchannels<br />
- Corner_flow with pin fin<br />
Each chip has four layers that need to be processed on a wafer. These layers have been placed<br />
on two wafers because <strong>of</strong> lack <strong>of</strong> space on a single wafer. For the dicing back-end step, the<br />
layers must be aligned in an orthogonal network. They have also been oriented to place the<br />
useful areas as much as possible in the center part <strong>of</strong> the wafer.<br />
First wafer comprises the “in_line_flow_microchannels” chip on the left column and the<br />
“in_line_flow_pin_fin” chip on the right column.<br />
Figure 4.13 : Wafer layout for in-line flow heat transfer stack<br />
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<strong>Interlayer</strong> cooling <strong>of</strong> <strong>3D</strong> stacked IC<br />
Figure 4.14 : Wafer layout for corner flow heat transfer stack<br />
Second wafer comprises the “corner_flow_microchannels” chip on the left column and the<br />
“corner_flow_pin_fin” chip on the right column.<br />
Dedicated front side and backside alignment<br />
marks must be placed corresponding to each<br />
layer and ordered in accordance with the<br />
process.<br />
To facilitate the alignment a border<br />
surrounding the marks can be placed to have<br />
an open window to find wafer crosses more<br />
easily through the mask.<br />
Figure 4.15 : Front side and backside alignment marks<br />
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<strong>Interlayer</strong> cooling <strong>of</strong> <strong>3D</strong> stacked IC<br />
4.1.3 Materials, methods and processes<br />
To process the wafers, a complete set <strong>of</strong> 10 masks has been done (5 masks per layout)<br />
- n°1: PR patterning for Ti/Pt evaporation<br />
- n°2: PR patterning for Al evaporation<br />
- n°3: PR patterning for pad opening<br />
- n°4: PR patterning for microchannels and pin fin dry etching<br />
- n°5: PR patterning for fluid inlet/outlet dry etching<br />
Wafers used were 100 ± 0.2 mm in diameter, 380 ± 10 µm thick and both side polished. They<br />
have been oxidized (200nm wet oxide on both sides) as an insulation layer for the heaters and<br />
sensors.<br />
Process flow that has been used for metallization, oxide sputtering, pad opening, etc. is the<br />
same kind <strong>of</strong> process that has been done for the first chip stack but with some additional steps.<br />
Steps and recipes for both layouts:<br />
Photolithography: AZ1512_on_LOR_400nm with EVG.<br />
Platinum metallization with titanium adhesion layer: 10nm Ti + 200nm Pt with LAB600 and<br />
Lift-<strong>of</strong>f / RT / No_IS parameters.<br />
Aluminum metallization: 400nm Al with EVA 600 (E-gun and Joule effect evaporator).<br />
To facilitate lift-<strong>of</strong>f for metallization, more openings should be placed on vacant area on the<br />
layout to shorten the required time <strong>of</strong> the process.<br />
Oxide sputtering with SPIDER600. Recipe SiO2 - wait - SiO2 – 1<br />
1µm - wait 15min - 1µm speed : 50nm/min<br />
Oxide sputtering has been done with a 15min break between two 1µm depositions to try to<br />
avoid pin holes on the surface that could lead to short circuit with the liquid through the<br />
oxide. The 15min break let time to the sample to cool down and release strain. Then second<br />
deposition is made directly on the surface with assumption that potential cracks may appear at<br />
other locations. To check this, a test wafer has been made with dummy Al heaters and with<br />
this method. After having protected the pads with tape, 3µm <strong>of</strong> aluminum have been sputtered<br />
on the surface to fill these potential pin holes. Measurement with prober station has shown no<br />
conductivity between a heater pad and aluminum sputtered surface.<br />
Coating backside: AZ1512 1um5_NoEBR<br />
Front side photolithography: AZ1512 1um5<br />
(Start from the backside to avoid having two times the s<strong>of</strong>tbake <strong>of</strong> useful side and recipe<br />
without solvent on the backside during coating on EVG)<br />
Wet etching in SILOX bath (pad etch) with activation (6min).<br />
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Process flow for microchannels, pin fin and fluid openings dry etching:<br />
Step Process description Cross-section after process<br />
1<br />
Photolithography (Back<br />
Side)<br />
Machine: EVG 150, MA6<br />
PR : AZ9260 – 5µm<br />
2<br />
Dry Etch<br />
Microchannels and pin fin<br />
etching<br />
Material : Si02 & Si<br />
Machine: AMS 200<br />
Depth : 200µm<br />
3 Resist stripping<br />
4<br />
Photolithography (Front<br />
Side)<br />
Machine: EVG 150, MA6<br />
PR : AZ9260 – 8µm<br />
5<br />
Dry Etch – Front Side<br />
Fluid inlet/outlet opening<br />
Material : Si02 & Si<br />
Machine: AMS 200<br />
Depth : 380µm<br />
(through all)<br />
90° rotation:<br />
Figure 4.16 : Process flow for microchannels, pin fin and fluid openings dry etching<br />
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Dry etching has been done with AMS 200 plasma etcher. Two processes have been used:<br />
Configuration:<br />
Materials to<br />
etch and<br />
Temperature<br />
Process<br />
• Distance ICP source<br />
- substrate holder<br />
• Substrate<br />
polarization (RF or<br />
pulsed LF)<br />
Mask<br />
Selectivity /<br />
mask<br />
Etching<br />
speed<br />
(µm/min)<br />
SiO 2 @ 0°C<br />
SiO2_PR_1:1<br />
200mm<br />
RF polarization<br />
PR =1:1 0.3<br />
Si deep<br />
anisotropic<br />
etching @ 20°C<br />
SOI_accurate<br />
++<br />
200mm<br />
Pulsed LF polarization<br />
PR<br />
SiO 2<br />
> 75:1 for PR<br />
> 150:1 for SiO 2<br />
(SiO 2 etching speed<br />
= 20nm/min)<br />
4.3<br />
Figure 4.17 : Recipes used for SiO 2 and Si dry etching with AMS 200<br />
To etch microchannels, pin fin and fluid openings, as we can see on the process flow, first the<br />
top oxide must be removed then a deep anisotropic etching <strong>of</strong> silicon must be done to create<br />
the heat transfer structures with a high aspect ratio. Microchannels and pillars should be<br />
etched with sidewalls as vertical as possible.<br />
Plasma etching that has been used is a physical-chemical process as a combination <strong>of</strong> ionic<br />
bombardment and chemical reactions at the surface. For these two processes etchant species<br />
are created in the gas <strong>of</strong> the plasma. These species react with the sample surface and products<br />
from the reaction (substrate change into another material by chemical reaction) detach and<br />
diffuse again into the gas. To etch the silicon oxide layer, the process (SiO2_PR_1:1) starts<br />
with a thermalization at 0°C <strong>of</strong> the substrate. Substrate is polarized with a radio frequency<br />
(13.56MHz). Gas injected in the chamber is C 4 F 8 with a flow rate <strong>of</strong> 15sccm and a pressure <strong>of</strong><br />
8.0E-3mbar.<br />
For Si deep etching, a Bosch process is used. It’s a pulsed process with etching and<br />
passivation in alternation. Sidewalls are protected by species from the reaction (organic<br />
compounds) that redeposit on these surfaces and avoid undercutting. Ionic bombardment<br />
removes this layer on horizontal surfaces while only a few particles hit the sides. Two gases<br />
are injected in alternation in the chamber. First C 4 F 8 with a flow rate <strong>of</strong> 150sccm during 2sec.<br />
then SF 6 with a flow rate <strong>of</strong> 300sccm during 7sec. Substrate is polarized with a pulsed low<br />
frequency and etching is done at room temperature (thermalization at 20°C).<br />
Microchannels and pin fin have been etched with following parameters:<br />
SiO2_PR_1:1 duration: 50sec. (0.2µm oxide)<br />
SOI_accurate++ duration: 47min. (200µm Si)<br />
Fluid inlet/outlet have been etched with following parameters:<br />
SiO2_PR_1:1 duration: 8min 30sec. (2.2µm oxide)<br />
SOI_accurate++ duration: 75min.<br />
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Stacking:<br />
To stack the layers, two ways have been considered: polyimide bonding <strong>of</strong> the dies or gold tin<br />
metal soldering.<br />
For polyimide bonding, a 4µm layer is structured with another photoresist and dry etched at<br />
the same time than other structures (equipment: STS Multiplex ICP). Then, the stack can be<br />
cured to do the bonding.<br />
Figure 4.18 : Schematic process for polyimide bonding<br />
For AuSn metal soldering, a wetting layer (100nm Ti / 50nm Pt) must be evaporated on both<br />
surfaces to be bonded. Then on one side a 4µm AuSn (80/20) is deposited. For the bonding,<br />
the sample is heated while a pressure is applied on the stack [15].<br />
These two bonding methods have not been tested before project term.<br />
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<strong>Interlayer</strong> cooling <strong>of</strong> <strong>3D</strong> stacked IC<br />
4.2 PCB<br />
<strong>3D</strong> chips can be glued with underfill (low viscosity adhesive) on a small PCB where the stack<br />
will be wire bonded and with male header connections all around the chip. Like this, this<br />
device can be plugged/unplugged on a larger PCB with female header connections and with<br />
larger jack connectors for power supplies and analyzers. Like this only one large PCB is<br />
needed and no wires are needed between the two PCBs.<br />
Chip<br />
Small PCB<br />
Large PCB<br />
Figure 4.19 : Chip assembled to a small PCB and mounted on a larger one<br />
For small PCBs both sides are used. Some connecting wires from bond pads to header<br />
footprint can be placed on the backside. Red lines are on PCB front side and blue lines are on<br />
PCB backside.<br />
Figure 4.20 : Chip and connectors footprints on small<br />
PCB<br />
Figure 4.21 : Connecting wires from bonding pads to<br />
connectors on small PCB. Red lines: PCB front side.<br />
Blue lines: PCB backside.<br />
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Connection zone for the stack (for in_line_flow chip):<br />
800µm<br />
Figure 4.22 : Pads configuration. On the left : pads from stacked chip. On the right : pads from PCB<br />
Vias in PCB pads middle column are placed to connect some wires on the backside due to<br />
short spacing available for the wires. Minimal dimensions for wires width and spacing that<br />
can be realized at EPFL are 100µm, limiting components density.<br />
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Connection zone for one heater and one sensor:<br />
Figure 4.23 : Wire bonding configuration for a microheater and its sensor<br />
For wire bonding, several wires must be bonded for the heaters. Current in the heater should<br />
reach 500mA. A 25µm gold wire can handle about 200mA. Pads from both sides must be<br />
placed close to each other to shorten the wires length. 4 small pads are dedicated to the sensor<br />
while 2 others act as readouts for the heater. So, one wire from the heater large pad must be<br />
connected to a small one.<br />
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4.3 Housing components<br />
(a)<br />
(b)<br />
(c)<br />
(d)<br />
Figure 4.24 : Polymer components. (a) housing for in-line flow chip, (b) housing for corner flow chip, (c)<br />
housing for in-line flow chip with push-in fluid connections, (d) housing for corner flow chip with pushin<br />
fluid connections<br />
Housing components have been made for the fluid circuit. Two fluid connections can be<br />
screwed on top and two chambers are machined on the other side for the fluid inlet/outlet.<br />
Design sketches are shown in appendix C. Manufacturing has been done by the mechanical<br />
workshop using PMMA. (PC has higher thermal properties, but wasn’t available in supply at<br />
that time)<br />
Fluid connections (Festo QSML-M5-4) can be 360° rotated. A 4mm diameter tube can be<br />
plugged in these push-in components. More details are shown in appendix D.<br />
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4.4 Results<br />
Figure 4.25 : Aluminum evaporation on platinum thin film (400nm Al on 200nm Pt)<br />
Evaporation <strong>of</strong> 400nm Al on 200nm Pt has given good results.<br />
Figure 4.26 : Non-uniformity and delamination after oxide sputtering<br />
After oxide sputtering, aluminum layer suffered from some problems. Oxide uniformity and<br />
adhesion were not suitable. This step was critical to go on with the processes to have a<br />
functional stack. After some time and processes, aluminum layer unstuck from platinum layer.<br />
Oxide sputtering step seems to have damaged the samples. Width and flatness <strong>of</strong> the leads<br />
could be involved. To try to avoid this problem and identify the causes <strong>of</strong> the delamination,<br />
another mask for the aluminum layer deposition with a patterned structured layer has been<br />
done (Figure 4.27).<br />
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Figure 4.27 : Alternative layout for Al layer<br />
Figure 4.28 : Al stripes on leads<br />
On this layout, Al stripes have been placed to have a structured layer on the leads for the<br />
oxide sputtering step. Al resistance on one lead is still less than 1Ω with this configuration.<br />
Squares have also been placed on unused areas <strong>of</strong> the wafer to enhance the lift-<strong>of</strong>f process and<br />
to check if the adhesion problem occurs because <strong>of</strong> the large surface <strong>of</strong> the leads.<br />
Figure 4.29 : Al stripes evaporation on platinum thin film (400nm Al on 200nm Pt)<br />
As the first time, evaporation <strong>of</strong> 400nm Al on 200nm Pt has given good results.<br />
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Figure 4.30 : Al stripes on platinum thin film and 1mm 2 square Al single layer, both after oxide sputtering<br />
After oxide sputtering, aluminum surface <strong>of</strong> the stripes deposited on platinum change to a<br />
rougher surface while this effect doesn’t appear on the large square which is a single<br />
aluminum layer.<br />
Figure 4.31 : Ti/Pt/Al/SiO2 and Al/SiO2 surfaces comparison<br />
At the same scale level, we can see on Figure 4.31 that the two surfaces are significantly<br />
different and that superimposition <strong>of</strong> Al on Pt seems to be more involved than the width <strong>of</strong> the<br />
leads. Differences can be due to atomic diffusion that can create intermetallic compounds<br />
(platinum aluminides). Diverse stress levels in the layers during deposition (that are also<br />
dependant <strong>of</strong> the temperature <strong>of</strong> the deposition) can also lead to delamination.<br />
At this point, first electrical properties <strong>of</strong> the heaters and sensors should be measured (as the<br />
layer is stable). In case <strong>of</strong> non-conformity with the application, titanium or titanium nitride<br />
interdiffusion barriers can be deposited between these layers and also on top to avoid<br />
oxidation <strong>of</strong> aluminum.<br />
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In the next SEM pictures, microchannels, pin fin and fluid openings that have been dry etched<br />
are shown in details.<br />
Figure 4.32 : 200µm deep microchannels dry etched on wafer backside and linked to the fluid opening<br />
Figure 4.33 : 200µm high pillars dry etched on wafer backside and linked to the fluid opening<br />
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Figure 4.34 : Microchannels and fluid opening<br />
Figure 4.35 : Pin fin and fluid opening<br />
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Figure 4.36 : Pillars network<br />
Figure 4.37 : Pillars with higher magnification<br />
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Figure 4.38 : Right-angled microchannels<br />
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5 Conclusion<br />
<strong>3D</strong> integration strategies have great potential for many technological applications. Multi-level<br />
devices and stacked layers may overcome many limitations. This promising technology for<br />
increasing integration density opens many research fields concerning its elaboration like<br />
vertical connections (Through Silicon Vias), wafer thinning, heterogeneous integration or heat<br />
transfer.<br />
<strong>Stacked</strong> layers can lead to faster, less power consuming and much more efficient integrated<br />
circuit by reducing the length <strong>of</strong> the interconnections. However, power management becomes<br />
a major parameter for their functionality because the power density per volume unit becomes<br />
very important with stacked chips. A suitable and reliable cooling system must be integrated<br />
to overcome these power limitations.<br />
During this project, first experiments have been done to manufacture a <strong>3D</strong> stacked chip with<br />
heat sources and thermal sensors on each die to emulate the power dissipated by active<br />
components in a CMOS chip and to sense the temperature inside <strong>of</strong> the <strong>3D</strong> stack. Chip<br />
thinning experiments have shown the feasibility <strong>of</strong> thinning a single die down to 100µm.<br />
Then, a heat transfer setup with an integrated fluid cooling system has been designed. Dies to<br />
be stacked have been made on a wafer level with micr<strong>of</strong>abrication processes. Some effects<br />
that appeared after oxide sputtering on Pt/Al thin layers must still be more investigated and<br />
tested if electrical measurements are not as expected (this has not been tested yet). Titanium<br />
or titanium nitride interdiffusion barriers could be implemented in further devices to avoid the<br />
formation <strong>of</strong> intermetallic compounds. Deep reactive ion etching (DRIE) <strong>of</strong> backside<br />
microstructures and fluid openings has given good results with anisotropic etching process in<br />
silicon with straight vertical walls for microchannels and pillars. Polymer components have<br />
been designed and produced to integrate the full system in a fluid loop for further heat transfer<br />
measurements. Printed circuit boards have been designed with dedicated pads to make<br />
connections to the microheaters and sensors by wire bonding. These PCBs can be produced to<br />
try the wire bonding <strong>of</strong> multi-level chips and have useful connections for the measurements<br />
instead <strong>of</strong> using a prober station.<br />
This highly-multidisciplinary project involves thermal modeling, micr<strong>of</strong>abrication, single<br />
phase and two-phase flow heat transfer and <strong>3D</strong> design <strong>of</strong> new types <strong>of</strong> architectures. All these<br />
fields should interact and stand in a near future, highly integrated in a <strong>3D</strong> chip with advanced<br />
cooling technologies.<br />
Lausanne, January 2009<br />
___________________<br />
Alexandre Pascarella<br />
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6 Acknowledgment<br />
I would like to thank Fengda Sun, Yuksel Temiz and Pr<strong>of</strong>. Leblebici for their precious help<br />
throughout this project; Thomas Brunschwiler and Bruno Michel from IBM (Zurich Research<br />
Laboratory - Advanced Thermal Packaging) for the presentation <strong>of</strong> their research work and<br />
laboratory, for having answered to many <strong>of</strong> my questions and shared their knowledge.<br />
Thanks to CMI staff for their great and very helpful help in many situations and for the<br />
trainings on modern and powerful processing machines.<br />
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7 Bibliography<br />
Books and Lecture Notes:<br />
[1] M.J. Madou, Fundamentals <strong>of</strong> micr<strong>of</strong>abrication, CRC Press LLC, Boca Raton – Florida, 2002<br />
(Second Edition).<br />
[2] J.G. Collier, J.R. Thome, Convective boiling and condensation, Oxford science publications,<br />
1996 (Third Edition).<br />
[3] S. Mostafa Ghiaasiaan, Two-phase flow, boiling and condensation, Cambridge University<br />
Press, New York, 2008.<br />
[4] P. Renaud, H. Shea, Scaling in MEMS, lecture notes, EPFL, 2007.<br />
[5] M.A.M Gijs, Technologie des microstructures I+II, lecture notes, EPFL, 2005.<br />
[6] P. Renaud, Capteurs I+II, lecture notes, EPFL. 2005.<br />
Journal Papers:<br />
<strong>3D</strong> integration:<br />
[7] Koester, S. J., Young, A. M., Yu, R. R., Purushothaman, S., Chen, K.-N., La Tulipe Jr., D. C.,<br />
Rana, N., Shi, L., Wordeman, M. R., & Sprogis, E. J. (2008). Wafer-level <strong>3D</strong> integration<br />
technology. IBM J. RES. & DEV. VOL. 52 NO. 6, 583 - 597.<br />
[8] Souri, S. J., Banerjee, K., Mehrota, A., & Saraswat, K. C. (2000). Multiple si layers <strong>ICs</strong>:<br />
Motivation, performance analysis, and design implications. Paper presented at the 213-220.<br />
[9] Kleiner, M. B., Kuehn, S. A., Ramm, P., & Weber, W. (1995). Thermal analysis <strong>of</strong> vertically<br />
integrated circuits. Paper presented at the 487-490.<br />
[10] Schaper, L., Burkett, S., Gordon, M., Cai, L., Liu, Y., Jampana, G., et al. (2007). Integrated<br />
system development for 3-D VLSI. Paper presented at the 853-857.<br />
[11] Schaper, L. W., Burkett, S. L., Spiesshoefer, S., Vangara, G. V., Rahman, Z., & Polamreddy,<br />
S. (2005). Architectural implications and process development <strong>of</strong> 3-D VLSI Z-axis<br />
interconnects using through silicon vias. IEEE Transactions on Advanced Packaging, 28(3),<br />
356-366.<br />
Wafer thinning:<br />
[12] Chen, C. -. A., & Hsu, L. -. (2008). A process model <strong>of</strong> wafer thinning by diamond grinding.<br />
Journal <strong>of</strong> Materials Processing Technology, 201(1-3), 606-611.<br />
[13] Sandireddy, S., & Jiang, T. (2005). Advanced wafer thinning technologies to enable multichip<br />
packages. Paper presented at the , 2005 24-27.<br />
[14] Jindal, A., Lu, J. -., Kwon, Y., Rajagopalan, G., McMahon, J. J., Zeng, A. Y., et al. (2003).<br />
Wafer thinning for monolithic <strong>3D</strong> integration. Paper presented at the , 766 21-26.<br />
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Heat transfer and cooling technologies:<br />
[15] Brunschwiler, T., Michel, B., Rothuizen, H., Kloter, U., Wunderle, B., Oppermann, H.,<br />
Reichl, H. (2008). Forced convective interlayer cooling in vertically integrated packages.<br />
11th Intersociety Conference on Thermal and Thermomechanical Phenomena in Electronic<br />
<strong>Systems</strong>, pp.1114-1125.<br />
[16] Koo, J. -., Im, S., Jiang, L., & Goodson, K. E. (2005). Integrated microchannel cooling for<br />
three-dimensional electronic circuit architectures. Journal <strong>of</strong> Heat Transfer, 127(1), 49-58.<br />
[17] Sekar, D., King, C., Dang, B., Spencer, T., Thacker, H., Joseph, P., et al. (2008). A <strong>3D</strong>-IC<br />
technology with integrated microchannel cooling. Paper presented at the 13-15.<br />
[18] Agostini, B., Thome, J. R., Fabbri, M., Michel, B., Calmi, D., Kloter, U., & Michel, B. (2006).<br />
High heat flux flow boiling in silicon multi-microchannels - part I: Materials and Methods,<br />
Heat Transfer Characteristics. Preprint submitted to Elsevier.<br />
[19] Agostini, B., Thome, J. R., Fabbri, M., Michel, B., Calmi, D., & Kloter, U. (2008). High heat<br />
flux flow boiling in silicon multi-microchannels - part II: Heat transfer characteristics <strong>of</strong><br />
refrigerant R245fa. International Journal <strong>of</strong> Heat and Mass Transfer.<br />
[20] Agostini, B., Fabbri, M., Park, J. E., Wojtan, L., Thome, J. R., & Michel, B. (2007). State <strong>of</strong><br />
the art <strong>of</strong> high heat flux cooling technologies. Heat Transfer Engineering, 28(4), 258-281.<br />
[21] Morini, G. L. (2004). Single-phase convective heat transfer in microchannels: A review <strong>of</strong><br />
experimental results. International Journal <strong>of</strong> Thermal Sciences, 43(7), 631-651.<br />
[22] Lee, P. -., Garimella, S. V., & Liu, D. (2005). Investigation <strong>of</strong> heat transfer in rectangular<br />
microchannels. International Journal <strong>of</strong> Heat and Mass Transfer, 48(9), 1688-1704.<br />
Websites:<br />
[23] http://cmi.epfl.ch<br />
[24] http://www.zurich.ibm.com/<br />
[25] http://lpm.epfl.ch/<br />
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8 Appendices<br />
8.1 Appendix A: Template for screen printing<br />
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8.2 Appendix B: Epoxy adhesive<br />
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8.3 Appendix C: Housing components design sketches<br />
PC_in_line_flow:<br />
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PC_corner_flow:<br />
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8.4 Appendix D: Fluid connectors<br />
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