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Status of SiC high voltage device technology Mikael stling, KTH - PowerPoint PPT Presentation

Status of SiC high voltage device technology Mikael stling, KTH Royal Institute of Technology, Sweden Outline 1. Introduction 2. Device Review (JFET, MOSFET, BJT) 3. 6 kV-Class BJTs 4. 15 kV-Class BJTs 5. HT & harsh environments 6.


  1. Status of SiC high voltage device technology Mikael Östling, KTH Royal Institute of Technology, Sweden

  2. Outline 1. Introduction 2. Device Review (JFET, MOSFET, BJT) 3. 6 kV-Class BJTs 4. 15 kV-Class BJTs 5. HT & harsh environments 6. Summary NEREID WORKSHOP BERTINORO OCT 2016 2

  3. Outline 1. Introduction 2. Device Review (JFET, MOSFET, BJT) 3. 6 kV-Class BJTs 4. 15 kV-Class BJTs 5. HT & harsh environments 6. Summary NEREID WORKSHOP BERTINORO OCT 2016 3

  4. Global Warming Energy Renewable Conservation Energy Improving the Electrical Efficiency Conversion Power Devices At least 50 % of the electricity used in the world is controlled by Power Devices. B.J. Baliga, Advanced High Voltage Power Device Concepts, Springer NEREID WORKSHOP BERTINORO OCT 2016 4

  5. Application for Power Devices 10 4 HVDC TRANSMISSION 10 3 ELECTRIC TRAINS Current rating (A) MOTOR 10 2 AUTOMOTIVE ELECTRONICS DRIVES POWER SUPLIES ROBOTICS 10 1 LAMP BALLAST 10 0 TELECOM. 10 -1 DISPLAY DRIVES 10 -2 10 1 10 2 10 3 10 4 Voltage rating (V) NEREID WORKSHOP BERTINORO OCT 2016 5

  6. SiC Device Roadmap Source: Dr. Muhammad Nawaz, ABB, ESCDERC 2016 but modified NEREID WORKSHOP BERTINORO OCT 2016 6

  7. Price Scenario SiC Source: Dr Anant Agarwal, US Department of Energy, ESCDERC 2016 NEREID WORKSHOP BERTINORO OCT 2016 7

  8. Price Scenario SiC The price for a 1.2 kV, is significantly below the PowerAmerica’s target of 10 cents/A. If the industry can approach these numbers in 3-5 years then the device 6.1 cents/A demand will grow exponentially across multiple applications. 4.6 cents/A 200mm SiC substrates, expected by 2020, will further reduce the cost of SiC MOSFETs. NEREID WORKSHOP BERTINORO OCT 2016 8

  9. Outline 1. Introduction 2. Device Review (JFET, MOSFET, BJT) 3. 6 kV-Class BJTs 4. 15 kV-Class BJTs 5. HT & harsh environments 6. Summary NEREID WORKSHOP BERTINORO OCT 2016 9

  10. MOSFETs Application: Solar inverters, switch mode power supplies, high voltage DC/DC converters, battery chargers, motor drive, pulsed power applications, renewable energy, lighting, telecom power supplies, induction heating, auxiliary power supplies, HVAC, LED lighting power supplies NEREID WORKSHOP BERTINORO OCT 2016 10

  11. 1700 MOSFETs NEREID WORKSHOP BERTINORO OCT 2016 11

  12. JFETs Applications: Solar inverters, high voltage DC/DC or AC/DC conversion, bidirectional inverter. NEREID WORKSHOP BERTINORO OCT 2016 12

  13. CoolSiC™ 1700 V JFETs Recently, Infineon presented their 1200V CoolSiC™ with record low Ron of 45 mΩ·cm 2 NEREID WORKSHOP BERTINORO OCT 2016 13

  14. BJTs Application: Down hole oil drilling, geothermal instrumentation, hybrid electric vehicles (HEV), solar inverters, switched, mode power supply (SMPS), power factor correction (PFC), induction heating, uninterruptible power supply (UPS), motor drives. NEREID WORKSHOP BERTINORO OCT 2016 14

  15. SiC power bipolar junction transistors by TranSiC Emitter contact SiO 2 surface passivation Base contact N D+ JTE implant P Base implant N N + substrate Collector contact Emitter Base • Vertical epitaxial NPN structure • Dry etching to form base-emitter and base-collector junctions • Al implantation for low-resistive base contact and junction termination (JTE) • Surface passivation by SiO 2 , reduced surface recombination • Large area BJT has many narrow emitter fingers • Deposited isolation oxide, via holes and Al metal pads • Active areas between 4.3mm 2 and 15 mm 2 NEREID WORKSHOP BERTINORO OCT 2016 15

  16. Recent Performance of SiC BJTs 40 T=25 C I B =400 mA I B =300 mA 35 30 Collector current (A) 4.3 mm 2 I B =200 mA 25 BJT 20 h FE =117 15 I B =100 mA 10 5 0 0 1 2 3 4 5 Collector emitter voltage V CE (v) Current gain at T=25 C : h FE =117 at I C =22 A • V CESAT =0.95 V at I C =15 A (J C =350 A/cm 2 ), ρ ON =2.7 mΩcm 2 • Low leakage current at V CEO =1200 V, Open-base breakdown ~ 1800 V • NEREID WORKSHOP BERTINORO OCT 2016 16

  17. 1200 V 4H-SiC Unipolar and Bipolar Devices NEREID WORKSHOP BERTINORO OCT 2016 18

  18. 1700 V 4H-SiC Unipolar and Bipolar Devices NEREID WORKSHOP BERTINORO OCT 2016 19

  19. Ultra High Voltage Devices The on-resistance for a 4H-SiC unipolar device above 15 kV, increases to the point where it is impractical from a yield standpoint and cost. Bipolar devices are likely to be the first choice. Source: Dr. John W. Palmour, CREE, IEDM 2014 NEREID WORKSHOP BERTINORO OCT 2016 20

  20. 21 kV BJT (T. Kimoto Kyoto University) MIYAKE et al. IEEE ELECTRON DEVICE LETTERS, VOL. 33, NO. 11, NOVEMBER, 2012, p.1598 NEREID WORKSHOP BERTINORO OCT 2016 21

  21. Active area small – 0.0035 mm 2 MIYAKE et al. IEEE ELECTRON DEVICE LETTERS, VOL. 33, NO. 11, NOVEMBER, 2012, p.1598 NEREID WORKSHOP BERTINORO OCT 2016 22

  22. Outline 1. Introduction 2. Device Review (JFET, MOSFET, BJT) 3. 6 kV-Class BJTs 4. 15 kV-Class BJTs 5. HT & harsh environments 6. Summary NEREID WORKSHOP BERTINORO OCT 2016 23

  23. 6 kV-Class 4H-SiC BJTs in Proc. 27th ISPSD , May 2015, pp. 249-252 NEREID WORKSHOP BERTINORO OCT 2016 24

  24. Trench JTE Design IEEE ELECTRON DEVICE LETTERS, VOL. 36, NO. 2, Feb. 2015 NEREID WORKSHOP BERTINORO OCT 2016 25

  25. I-V Characteristics Termination efficiency 92 % Termination efficiency 93 % in Proc. 27th ISPSD , May 2015, pp. 249-252 IEEE ELECTRON DEVICE LETTERS, VOL. 36, NO. 2, Feb. 2015 NEREID WORKSHOP BERTINORO OCT 2016 26

  26. Outline 1. Introduction 2. Device Review (JFET, MOSFET, BJT) 3. 6 kV-Class BJTs 4. 15 kV-Class BJTs 5. HT & harsh environments 6. Summary NEREID WORKSHOP BERTINORO OCT 2016 27

  27. 15 kV-Class BJTs and PiN Diodes 15 kV-class PiN diodes will be presenteded in Tu1.04 NEREID WORKSHOP BERTINORO OCT 2016 28

  28. I-V Characteristics of the BJTs A current gain record of 139 for 15 kV-class BJTs NEREID WORKSHOP BERTINORO OCT 2016 29

  29. Current Gain Wafer map β ≥ 100 (91 % of the dies) NEREID WORKSHOP BERTINORO OCT 2016 30

  30. Outline 1. Introduction 2. Device Review (JFET, MOSFET, BJT) 3. 6 kV-Class BJTs 4. 15 kV-Class BJTs 5. HT & harsh environments 6. Summary NEREID WORKSHOP BERTINORO OCT 2016 31

  31. Applications for HT & harsh environments Application Type Temperature Radiation Oil and gas drilling P, S 600 °C No Industrial motor drives P 300 °C No Automotive P, S 300-600 °C No Aviation P, S 300-600 °C (Yes) Space exploration S 600 °C Yes Nuclear energy (P) S 300-600 °C Yes P = Power switching applications S = Sensor signal processing NEREID WORKSHOP BERTINORO OCT 2016 32

  32. A new high temperature SiC electronics project WOV – Working on Venus $ 3,3M Project funding 2014 – 2018 NEREID WORKSHOP BERTINORO OCT 2016 33

  33. Radiation stability of SiC BJT vs. MOSFET Commercially available 24 A (CMF10120D) SiC Forward current gain degradation up to power MOSFETs fabricated by CREE, shows a 38 Mrad was found negligible, but for large negative threshold voltage shift and the dose of 332 Mrad, a degradation of becomes inoperative after a dose of only 300 52% is seen. krad. A. Akturk, et.al, IEEE Trans. Nucl. Sci., 59 (2012). To be published in IEEE TED NEREID WORKSHOP BERTINORO OCT 2016 34

  34. Comparison of various bipolar technology Gamma irradiation Protons irradiation 4H-SiC KTH-Low Power BJT [7] Si- BJT [8] • 4H-SiC technology show more tolerance to gamma radiation in comparison to other technologies. • 4H-SiC devices irradiated with 3 MeV protons show about one order of magnitude higher tolerance in comparison to the Si technology NEREID WORKSHOP BERTINORO OCT 2016 35

  35. Outline 1. Introduction 2. Device Review (JFET, MOSFET, BJT) 3. 6 kV-Class BJTs 4. 15 kV-Class BJTs 5. HT & harsh environments 6. Summary NEREID WORKSHOP BERTINORO OCT 2016 36

  36. Summary • Replacing Si with SiC switch devices gives great savings with respect to energy density, efficiency, and physical systems volume • At 1200-1700V SiC MOSFETs, JFETs and BJT performs about equally good • In a few years the cost issues with SiC looks very competitive < 5 cents/Amp • Above 15 kV, BJTs/IGBTs are likely to be the first choice • For high temperature and radhard environments BJTs have a clear advantage NEREID WORKSHOP BERTINORO OCT 2016 37

  37. Acknowledgments The KTH research team The Swedish Energy Agency The Swedish Research Council VINNOVA – research and innovation for sustainable growth Swedish Foundation for Strategic Research KAW Foundation STandUP for Energy NEREID WORKSHOP BERTINORO OCT 2016 38

  38. Commercial SiC-MOSFET (Si-IGBT) Power Module 10/21/16 NEREID WORKSHOP BERTINORO OCT 2016 39

  39. Emitter Size Effect NEREID WORKSHOP BERTINORO OCT 2016 40

  40. Base Size Effect 10/21/16 NEREID WORKSHOP BERTINORO OCT 2016 MIKAEL ÖSTLING 41

  41. Current Gain vs Geometry W E = 40 µm W B = 30 µm 10/21/16 NEREID WORKSHOP BERTINORO OCT 2016 MIKAEL ÖSTLING 42

  42. Compactness: Si Vs SiC Source: Dr. Muhammad Nawaz, ABB 10/21/16 NEREID WORKSHOP BERTINORO OCT 2016 MIKAEL ÖSTLING 43

  43. Current Gain vs Applied Voltage Decreasing effective base Base width modulation (Early effect) 10/21/16 NEREID WORKSHOP BERTINORO OCT 2016 MIKAEL ÖSTLING 44

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