High temperature operation of SiC transistors
Transcript of High temperature operation of SiC transistors
High temperature operation of SiC transistorsATW on Thermal Management, Los Gatos
Cyril BUTTAY1, Marwan ALI2, Oriol AVINO1,2,Hervé MOREL1, Bruno ALLARD1
1 Laboratoire Ampère, Lyon, France2 Labinal Power Systems, SAFRAN Group, France
23/9/15
1 / 32
Outline
Introduction
High-Temperature behaviour of SiC Devices
Packaging for high-temperature converters
Conclusion
2 / 32
Outline
Introduction
High-Temperature behaviour of SiC Devices
Packaging for high-temperature converters
Conclusion
3 / 32
Automotive
Vehicle Location Max Temp (°C)Drive train high temp location 177Floor 85Near radiator support structure 100Back of alternator 160Cooling circuit 120Exhaust manifold 649
Most data: Kassakian, J. G. et al. “The Future of Electronics in Automobiles”, ISPSD, 2001, p 15-19
I Low-cost, high-volume applications;I Moving to higher voltages (12V->300V for hybrids)I Little cooling headroom with silicon devices (TJ=150 to
175°C)
ß dedicated cooling circuit for power electronic systems
4 / 32
Automotive
Vehicle Location Max Temp (°C)Drive train high temp location 177Floor 85Near radiator support structure 100Back of alternator 160Cooling circuit 120Exhaust manifold 649
Most data: Kassakian, J. G. et al. “The Future of Electronics in Automobiles”, ISPSD, 2001, p 15-19
I Low-cost, high-volume applications;I Moving to higher voltages (12V->300V for hybrids)I Little cooling headroom with silicon devices (TJ=150 to
175°C)
ß dedicated cooling circuit for power electronic systems
4 / 32
Automotive
Vehicle Location Max Temp (°C)Drive train high temp location 177Floor 85Near radiator support structure 100Back of alternator 160Cooling circuit 120Exhaust manifold 649
Most data: Kassakian, J. G. et al. “The Future of Electronics in Automobiles”, ISPSD, 2001, p 15-19
I Low-cost, high-volume applications;I Moving to higher voltages (12V->300V for hybrids)I Little cooling headroom with silicon devices (TJ=150 to
175°C)
ß dedicated cooling circuit for power electronic systems
4 / 32
Aircraft
The trend:I Hydraulic, Pneumatic and Electric
networks co-exist in current systemsI More-electric aircraft should reduce
complexityI objective: 1 MW on-board electrical power
The environment:
I From mild to very harsh:I Some system are located in the cabinI Jet engine actuator will face -55°C to 225°C cyclingI Many systems are located in non-pressurised areas
I Long system life: around 30 yearsI Reliability is the main concern
5 / 32
Aircraft
The trend:I Hydraulic, Pneumatic and Electric
networks co-exist in current systemsI More-electric aircraft should reduce
complexityI objective: 1 MW on-board electrical power
The environment:I From mild to very harsh:
I Some system are located in the cabinI Jet engine actuator will face -55°C to 225°C cyclingI Many systems are located in non-pressurised areas
I Long system life: around 30 yearsI Reliability is the main concern
5 / 32
Aircraft
The trend:I Hydraulic, Pneumatic and Electric
networks co-exist in current systemsI More-electric aircraft should reduce
complexityI objective: 1 MW on-board electrical power
The environment:I From mild to very harsh:
I Some system are located in the cabinI Jet engine actuator will face -55°C to 225°C cyclingI Many systems are located in non-pressurised areas
I Long system life: around 30 yearsI Reliability is the main concern
5 / 32
Aircraft
The trend:I Hydraulic, Pneumatic and Electric
networks co-exist in current systemsI More-electric aircraft should reduce
complexityI objective: 1 MW on-board electrical power
The environment:I From mild to very harsh:
I Some system are located in the cabinI Jet engine actuator will face -55°C to 225°C cyclingI Many systems are located in non-pressurised areas
I Long system life: around 30 yearsI Reliability is the main concern
5 / 32
Aircraft
The trend:I Hydraulic, Pneumatic and Electric
networks co-exist in current systemsI More-electric aircraft should reduce
complexityI objective: 1 MW on-board electrical power
The environment:I From mild to very harsh:
I Some system are located in the cabinI Jet engine actuator will face -55°C to 225°C cyclingI Many systems are located in non-pressurised areas
I Long system life: around 30 yearsI Reliability is the main concern
5 / 32
Space Exploration
I NASA missions to Venus and JupiterI Venus surface temperature : up to 480°CI Pressure a few kilometres inside Jupiter: 100
bars, at 400°CI Strong thermal cycling, as temperature can drop
to 140K at night;I Other awful conditions: winds, corrosive
gases. . .
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Deep oil/gas extraction
I Continuous operation, relatively lowcycling
I Deep drilling: high ambient temperature(up to 225°C)
I Expected lifetime: 5 yearsI Main requirement: sensors and
dataloggingI Example of new applications: downhole
gas compressor
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Maximum operating temperature
0°C
500°C
1000°C
1500°C
2000°C
2500°C
3000°C
10 V 100 V 1 kV 10 kV 100 kV 1 MV
Junc
tion
tem
pera
ture
Breakdown voltage
Silicon3C−SiC6H−SiC4H−SiC
2H−GaNDiamond
Silicon operating temp is intrisically limited at high voltages.I 1200 V devices rated at <200 °C junction temperature
8 / 32
Outline
Introduction
High-Temperature behaviour of SiC Devices
Packaging for high-temperature converters
Conclusion
9 / 32
Test configuration
I High temperature test systemI Silver-sintered interconnectsI Ceramic substrate (DBC)I Copper-kapton leadframe
I DUT: 490 mΩ SiC JFET from SiCEDI characterization:
I Tektronix 371A curve tracerI Thermonics T2500-E conditionner
Source: Thermonics T-2500E Datasheet
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Test configuration
I High temperature test systemI Silver-sintered interconnectsI Ceramic substrate (DBC)I Copper-kapton leadframe
I DUT: 490 mΩ SiC JFET from SiCEDI characterization:
I Tektronix 371A curve tracerI Thermonics T2500-E conditionner
Source: Thermonics T-2500E Datasheet
10 / 32
Test configuration
I High temperature test systemI Silver-sintered interconnectsI Ceramic substrate (DBC)I Copper-kapton leadframe
I DUT: 490 mΩ SiC JFET from SiCEDI characterization:
I Tektronix 371A curve tracerI Thermonics T2500-E conditionner
Source: Thermonics T-2500E Datasheet
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Static Characterization of 490 mΩ JFET
Buttay et Al. “Thermal Stability of Silicon Carbide Power JFETs” IEEE transactions on Electron Devices, 2013, 60, 4191-4198
0 2 4 6 8 10 12Forward voltage [V]
0
2
4
6
8
10
12Fo
rwar
d cu
rren
t [A]
-50 C-10 C30 C70 C
110 C
150 C190 C230 C270 C300 C
VGS = 0 V , i.e. device fully-on11 / 32
Power dissipation as a function of the junction temp.
50 0 50 100 150 200 250 300
Junction temperature [C]
0
20
40
60
80
100
120
140D
issi
pate
d p
ow
er
[W]
2.0 A4.0 A6.0 A8.0 A10.0 A
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Thermal Run-away mechanism – Principle
I The device characteristicI Its associated cooling systemI In region A, the device
dissipates more than thecooling system can extract
I In region B, the devicedissipates less than thecooling system can extract
I Two equilibrium points: onestable and one unstable
I Above the unstable point,run-away occurs
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Thermal Run-away mechanism – Principle
I The device characteristicI Its associated cooling systemI In region A, the device
dissipates more than thecooling system can extract
I In region B, the devicedissipates less than thecooling system can extract
I Two equilibrium points: onestable and one unstable
I Above the unstable point,run-away occurs
13 / 32
Thermal Run-away mechanism – Principle
I The device characteristicI Its associated cooling systemI In region A, the device
dissipates more than thecooling system can extract
I In region B, the devicedissipates less than thecooling system can extract
I Two equilibrium points: onestable and one unstable
I Above the unstable point,run-away occurs
13 / 32
Thermal Run-away mechanism – Principle
I The device characteristicI Its associated cooling systemI In region A, the device
dissipates more than thecooling system can extract
I In region B, the devicedissipates less than thecooling system can extract
I Two equilibrium points: onestable and one unstable
I Above the unstable point,run-away occurs
13 / 32
Thermal Run-away mechanism – Principle
I The device characteristicI Its associated cooling systemI In region A, the device
dissipates more than thecooling system can extract
I In region B, the devicedissipates less than thecooling system can extract
I Two equilibrium points: onestable and one unstable
I Above the unstable point,run-away occurs
13 / 32
Thermal Run-away mechanism – examples
Always stable
Always unstable Becomming unstablewith ambient
temperature rise
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Thermal Run-away mechanism – examples
Always stable Always unstable
Becomming unstablewith ambient
temperature rise
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Thermal Run-away mechanism – examples
Always stable Always unstable Becomming unstablewith ambient
temperature rise
14 / 32
Power dissipation as a function of the junction temp.
50 0 50 100 150 200 250 300
Junction temperature [C]
0
20
40
60
80
100
120
140D
issi
pate
d p
ow
er
[W]
2.0 A4.0 A6.0 A8.0 A10.0 A
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Power dissipation as a function of the junction temp.
50 0 50 100 150 200 250 300
Junction temperature [C]
0
20
40
60
80
100
120
140D
issi
pate
d p
ow
er
[W]
1K/W
2K/W
4.5K/W
2.0 A4.0 A6.0 A8.0 A10.0 A
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High Temperature Thermal Management
Buttay et al. “Thermal Stability of Silicon Carbide Power JFETs”, IEEE Trans on Electron Devices, 2014
100 150 200 250 300 350time [s]
30
40
50
60
70
80
pow
er [W
]
current changed from 3.65 to 3.7 A
Run-awaySiC JFET:
I 490 mΩ, 1200 VI RThJA = 4.5 K/WI 135 °C ambientI On-state losses
High temperature capability 6= reduced cooling needs!SiC JFETs must be attached to a low-RTh cooling system.
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Conclusions on high-temp. behaviour of SiC JFETs
I SiC JFETs can operate at > 200 °CI RDSon dependent on temperature
Ü sensitive to thermal run-awayI Require efficient thermal management
I low thermal resistance (1-2 K/W)I low or high ambient temperature
(> 200 °C possible)
Falahi et Al. “High temperature, Smart Power Module for aircraft actuators”,HiTEN 2013
0 2 4 6 8 10 12Drain-to-Source voltage [V]
0
10
20
30
40
50
60
70
Dra
incu
rren
t[A
]
-50C -10C 27C 70C 107C
160C
196C
234C
270C
49.0 48.8 48.6 48.4time [µs]
50
0
50
100
150
200
250
Vout [
V]
0.2 0.0 0.2time [µs]
310°C
17 / 32
Conclusions on high-temp. behaviour of SiC JFETs
I SiC JFETs can operate at > 200 °CI RDSon dependent on temperature
Ü sensitive to thermal run-awayI Require efficient thermal management
I low thermal resistance (1-2 K/W)I low or high ambient temperature
(> 200 °C possible)
Falahi et Al. “High temperature, Smart Power Module for aircraft actuators”,HiTEN 2013
0 2 4 6 8 10 12Drain-to-Source voltage [V]
0
10
20
30
40
50
60
70
Dra
incu
rren
t[A
]
-50C -10C 27C 70C 107C
160C
196C
234C
270C
49.0 48.8 48.6 48.4time [µs]
50
0
50
100
150
200
250
Vout [
V]
0.2 0.0 0.2time [µs]
310°C
17 / 32
Conclusions on high-temp. behaviour of SiC JFETs
I SiC JFETs can operate at > 200 °CI RDSon dependent on temperature
Ü sensitive to thermal run-awayI Require efficient thermal management
I low thermal resistance (1-2 K/W)I low or high ambient temperature
(> 200 °C possible)
Falahi et Al. “High temperature, Smart Power Module for aircraft actuators”,HiTEN 2013
0 2 4 6 8 10 12Drain-to-Source voltage [V]
0
10
20
30
40
50
60
70
Dra
incu
rren
t[A
]
-50C -10C 27C 70C 107C
160C
196C
234C
270C
49.0 48.8 48.6 48.4time [µs]
50
0
50
100
150
200
250
Vout [
V]
0.2 0.0 0.2time [µs]
310°C
17 / 32
Conclusions on high-temp. behaviour of SiC JFETs
I SiC JFETs can operate at > 200 °CI RDSon dependent on temperature
Ü sensitive to thermal run-awayI Require efficient thermal management
I low thermal resistance (1-2 K/W)I low or high ambient temperature
(> 200 °C possible)
Falahi et Al. “High temperature, Smart Power Module for aircraft actuators”,HiTEN 2013
0 2 4 6 8 10 12Drain-to-Source voltage [V]
0
10
20
30
40
50
60
70
Dra
incu
rren
t[A
]
-50C -10C 27C 70C 107C
160C
196C
234C
270C
49.0 48.8 48.6 48.4time [µs]
50
0
50
100
150
200
250
Vout [
V]
0.2 0.0 0.2time [µs]
310°C
17 / 32
Outline
Introduction
High-Temperature behaviour of SiC Devices
Packaging for high-temperature converters
Conclusion
18 / 32
Double Side Cooling
I Standard packaging offers cooling through one side of thedie only
I “3-D” or “Sandwich” package offers thermal managementon both sides
I Requires suitable topside metal on the dieI Requires special features for topside contact
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Double Side Cooling
I Standard packaging offers cooling through one side of thedie only
I “3-D” or “Sandwich” package offers thermal managementon both sides
I Requires suitable topside metal on the dieI Requires special features for topside contact
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The proposed 3-D Structure
Vbus
OUT
GND
JH
JL
I Two ceramic substrates, in “sandwich” configurationI Two SiC JFET dies (SiCED)I assembled using silver sinteringI 25.4 mm×12.7 mm (1 in×0.5 in)
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Ceramic Substrates
SiC JFET
Alumina
0.2 mm
0,3 mm
0.16 mm
0,15 mm
Copper
0.15 mm Gate SourceSource
Drain0.3 mm
Scale drawing for 2.4×2.4 mm2 die
I Si3N4 identified previously forhigh temperature
I For development: use ofalumina
I Etching accuracy exceedsstandard design rules
I Double-step copper etching fordie contact
Ü Custom etching technique
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Bonding Material: Silver Sintering
Göbl, C. et al “Low temperature sinter technology Die attachment for automotivepower electronic applications” proc of APE, 2006
Silver PasteI Based on micro-scale silver
particles (Heraeus LTS-117O2P2)I Low temperature (240 °C) sinteringI Low pressure (2 MPa) process
No liquid phase involved:I No movement of the dieI No bridging across terminalsI No height compensation thanks to
wetting
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Preparation of the Substrates
plain DBC board
I Final patterns within 50 µm of desired sizeI Two designs, for 2.4×2.4 mm2 and 4×4 mm2 diesI Total copper thickness 300 µm, ≈ 150 µm per step
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Preparation of the Substrates
plain DBC board 1a - Photosensitive resin coating
I Final patterns within 50 µm of desired sizeI Two designs, for 2.4×2.4 mm2 and 4×4 mm2 diesI Total copper thickness 300 µm, ≈ 150 µm per step
23 / 32
Preparation of the Substrates
plain DBC board 1a - Photosensitive resin coating
1b - Exposure andDevelopment
I Final patterns within 50 µm of desired sizeI Two designs, for 2.4×2.4 mm2 and 4×4 mm2 diesI Total copper thickness 300 µm, ≈ 150 µm per step
23 / 32
Preparation of the Substrates
plain DBC board 1a - Photosensitive resin coating
1b - Exposure andDevelopment
2 - Etching
I Final patterns within 50 µm of desired sizeI Two designs, for 2.4×2.4 mm2 and 4×4 mm2 diesI Total copper thickness 300 µm, ≈ 150 µm per step
23 / 32
Preparation of the Substrates
plain DBC board 1a - Photosensitive resin coating
1b - Exposure andDevelopment
2 - Etching 3a - resin coating
I Final patterns within 50 µm of desired sizeI Two designs, for 2.4×2.4 mm2 and 4×4 mm2 diesI Total copper thickness 300 µm, ≈ 150 µm per step
23 / 32
Preparation of the Substrates
plain DBC board 1a - Photosensitive resin coating
1b - Exposure andDevelopment
2 - Etching 3a - resin coating
3b - Exposure and Developpment
I Final patterns within 50 µm of desired sizeI Two designs, for 2.4×2.4 mm2 and 4×4 mm2 diesI Total copper thickness 300 µm, ≈ 150 µm per step
23 / 32
Preparation of the Substrates
plain DBC board 1a - Photosensitive resin coating
1b - Exposure andDevelopment
2 - Etching 3a - resin coating
3b - Exposure and Developpment
4a - Photosentive filmlaminating
I Final patterns within 50 µm of desired sizeI Two designs, for 2.4×2.4 mm2 and 4×4 mm2 diesI Total copper thickness 300 µm, ≈ 150 µm per step
23 / 32
Preparation of the Substrates
plain DBC board 1a - Photosensitive resin coating
1b - Exposure andDevelopment
2 - Etching 3a - resin coating
3b - Exposure and Developpment
4a - Photosentive filmlaminating
4b - Exposure andDevelopment
I Final patterns within 50 µm of desired sizeI Two designs, for 2.4×2.4 mm2 and 4×4 mm2 diesI Total copper thickness 300 µm, ≈ 150 µm per step
23 / 32
Preparation of the Substrates
plain DBC board 1a - Photosensitive resin coating
1b - Exposure andDevelopment
2 - Etching 3a - resin coating
3b - Exposure and Developpment
4a - Photosentive filmlaminating
4b - Exposure andDevelopment
5 - Etching
I Final patterns within 50 µm of desired sizeI Two designs, for 2.4×2.4 mm2 and 4×4 mm2 diesI Total copper thickness 300 µm, ≈ 150 µm per step
23 / 32
Preparation of the Substrates
plain DBC board 1a - Photosensitive resin coating
1b - Exposure andDevelopment
2 - Etching 3a - resin coating
3b - Exposure and Developpment
4a - Photosentive filmlaminating
4b - Exposure andDevelopment
5 - Etching6 - Singulating
I Final patterns within 50 µm of desired sizeI Two designs, for 2.4×2.4 mm2 and 4×4 mm2 diesI Total copper thickness 300 µm, ≈ 150 µm per step
23 / 32
Preparation of the Substrates
I Final patterns within 50 µm of desired sizeI Two designs, for 2.4×2.4 mm2 and 4×4 mm2 diesI Total copper thickness 300 µm, ≈ 150 µm per step
23 / 32
Preparation of the Dies
I Standard aluminium topside finishnot compatible with silver sintering
I Ti/Ag PVD on contact areasI Need for a masking solution
Ü jig with locating pockets.
DieMask
PVD
24 / 32
Preparation of the Dies
I Standard aluminium topside finishnot compatible with silver sintering
I Ti/Ag PVD on contact areasI Need for a masking solution
Ü jig with locating pockets.
DieMask
PVD
Before PVD 24 / 32
Preparation of the Dies
I Standard aluminium topside finishnot compatible with silver sintering
I Ti/Ag PVD on contact areasI Need for a masking solution
Ü jig with locating pockets.
DieMask
PVD
Before PVD After Ti/Ag PVD 24 / 32
Assembly
Screen printing
I Ceramic laser-cut jigs for precise alignment of dies andsubstrate
I Two sintering steps using the same temperature profile
25 / 32
Assembly
Screen printing 2- Mounting in alignment jig
I Ceramic laser-cut jigs for precise alignment of dies andsubstrate
I Two sintering steps using the same temperature profile
25 / 32
Assembly
Screen printing 2- Mounting in alignment jig
3- Die-alignment jig, dies and spacer placing
I Ceramic laser-cut jigs for precise alignment of dies andsubstrate
I Two sintering steps using the same temperature profile
25 / 32
Assembly
Screen printing 2- Mounting in alignment jig
3- Die-alignment jig, dies and spacer placing
4 - First sintering step
I Ceramic laser-cut jigs for precise alignment of dies andsubstrate
I Two sintering steps using the same temperature profile
25 / 32
Assembly
Screen printing 2- Mounting in alignment jig
3- Die-alignment jig, dies and spacer placing
4 - First sintering step 5 - Removal of die-alignment jig
I Ceramic laser-cut jigs for precise alignment of dies andsubstrate
I Two sintering steps using the same temperature profile
25 / 32
Assembly
Screen printing 2- Mounting in alignment jig
3- Die-alignment jig, dies and spacer placing
4 - First sintering step 5 - Removal of die-alignment jig
6 - Screen printing on "drain" substrate
I Ceramic laser-cut jigs for precise alignment of dies andsubstrate
I Two sintering steps using the same temperature profile
25 / 32
Assembly
Screen printing 2- Mounting in alignment jig
3- Die-alignment jig, dies and spacer placing
4 - First sintering step 5 - Removal of die-alignment jig
6 - Screen printing on "drain" substrate
7 - Mounting in alignment jig
I Ceramic laser-cut jigs for precise alignment of dies andsubstrate
I Two sintering steps using the same temperature profile
25 / 32
Assembly
Screen printing 2- Mounting in alignment jig
3- Die-alignment jig, dies and spacer placing
4 - First sintering step 5 - Removal of die-alignment jig
6 - Screen printing on "drain" substrate
7 - Mounting in alignment jig
8 - Second sintering step
I Ceramic laser-cut jigs for precise alignment of dies andsubstrate
I Two sintering steps using the same temperature profile
25 / 32
Assembly
Screen printing 2- Mounting in alignment jig
3- Die-alignment jig, dies and spacer placing
4 - First sintering step 5 - Removal of die-alignment jig
6 - Screen printing on "drain" substrate
7 - Mounting in alignment jig
8 - Second sintering stepResult
I Ceramic laser-cut jigs for precise alignment of dies andsubstrate
I Two sintering steps using the same temperature profile
25 / 32
Some results
Size: 25×25 mm226 / 32
Some results
26 / 32
Some results
0.9 1.0 1.1 1.2time [µs]
50
0
50
100
150
200
Vout [
V]
49.9 50.0 50.1 50.2time [µs]
200°C
I 300 Ω Resistive load, 0.5 A current (no cooling system used)I oscillations dues to external layout
26 / 32
Outline
Introduction
High-Temperature behaviour of SiC Devices
Packaging for high-temperature converters
Conclusion
27 / 32
Conclusion
I SiC JFET able to operate continuously at high temperature(> 200 °C)I Must be provided with efficient thermal management (RTh =1–2 K/W)I Proposition: introduce dual-side coolingI 3D structure using only high-temperature-rated materials
I Should be able to operate continuously at 300 °C, including passivation(parylene HT or F)
I Proposed etching technique offers satisfying resolutionI Silver sintering used for the interconnects, reliability to be investigated
I Package for demonstration of technology, no cooling attempted yet!
28 / 32
Conclusion
I SiC JFET able to operate continuously at high temperature(> 200 °C)I Must be provided with efficient thermal management (RTh =1–2 K/W)I Proposition: introduce dual-side coolingI 3D structure using only high-temperature-rated materials
I Should be able to operate continuously at 300 °C, including passivation(parylene HT or F)
I Proposed etching technique offers satisfying resolutionI Silver sintering used for the interconnects, reliability to be investigated
I Package for demonstration of technology, no cooling attempted yet!
28 / 32
Conclusion
I SiC JFET able to operate continuously at high temperature(> 200 °C)I Must be provided with efficient thermal management (RTh =1–2 K/W)I Proposition: introduce dual-side coolingI 3D structure using only high-temperature-rated materials
I Should be able to operate continuously at 300 °C, including passivation(parylene HT or F)
I Proposed etching technique offers satisfying resolutionI Silver sintering used for the interconnects, reliability to be investigated
I Package for demonstration of technology, no cooling attempted yet!
28 / 32
Conclusion
I SiC JFET able to operate continuously at high temperature(> 200 °C)I Must be provided with efficient thermal management (RTh =1–2 K/W)I Proposition: introduce dual-side coolingI 3D structure using only high-temperature-rated materials
I Should be able to operate continuously at 300 °C, including passivation(parylene HT or F)
I Proposed etching technique offers satisfying resolutionI Silver sintering used for the interconnects, reliability to be investigated
I Package for demonstration of technology, no cooling attempted yet!
28 / 32
Conclusion
I SiC JFET able to operate continuously at high temperature(> 200 °C)I Must be provided with efficient thermal management (RTh =1–2 K/W)I Proposition: introduce dual-side coolingI 3D structure using only high-temperature-rated materials
I Should be able to operate continuously at 300 °C, including passivation(parylene HT or F)
I Proposed etching technique offers satisfying resolutionI Silver sintering used for the interconnects, reliability to be investigated
I Package for demonstration of technology, no cooling attempted yet!
28 / 32
This work was funded by Euripides-Catrenes under the grant name“THOR” and FRAE under the grant name “ETHAER”.
29 / 32
Credits
I picture of the Airbus A350: airbus
I picture of the thrust reverser: Hispano-Suizahttp://www.hispano-suiza-sa.com/spip.php?rubrique48
I picture of the Toyota Prius: Picture by Pawel Golsztajn, CC-SA,available on Wikimedia Commons http:
//commons.wikimedia.org/wiki/File:Toyota_Prius.2.JPG
I downhole gas compressor: http://www.corac.co.uk/products/downhole-gas-compressor
I picture of Jupiter: NASAhttp://en.wikipedia.org/wiki/File:PIA04866_modest.jpg
I MOSFET wafers from Mitsubishihttp://compoundsemiconductor.net/cws/article/fab/
38238/1/siliconcarbidewafers
30 / 32
Static and Dynamic Characterization of 60 mΩ JFET
Falahi et Al. “High temperature, Smart Power Module for aircraft actuators”, HiTEN 2013
0 2 4 6 8 10 12Drain-to-Source voltage [V]
0
10
20
30
40
50
60
70
Dra
incu
rren
t[A
]
-50C -10C 27C 70C 107C
160C
196C
234C
270C
49.0 48.8 48.6 48.4time [µs]
50
0
50
100
150
200
250
Vout [
V]
0.2 0.0 0.2time [µs]
310°C
Previous results show that SiC JFETs are attractive for> 200 °C operation:
I rated at 1200 V (or more), several AmpsI Voltage-controlled devicesI No reliability issue related to gate oxide degradation
31 / 32
Properties of some semiconductors
“Classical” wide-bandgap
Si GaAs 3C-SiC
6H-SiC
4H-SiC
GaN Diamond
Bandgap EnergyEg (eV) 1,12 1,4 2,3 2,9 3,2 3,39 5,6
Elec. mobilityµn (cm2.V−1.s−1) 1450 8500 1000 415 950 2000 4000
Hole mobilityµp (cm2.V−1.s−1) 450 400 45 90 115 350 3800
Critical elec. fieldEC (V.cm−1) 3.105 4.105 2.106 2,5.106 3.106 5.106 107
Saturation velocityvsat (cm.s−1) 107 2.107 2,5.107 2.107 2.107 2.107 3.107
Termal cond.λ (W.cm−1.K−1) 1,3 0,54 5 5 5 1,3 20
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