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4HSIC JUNCTION BARRIERSCHOTTKY JBS DIODES

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PIN part limited by fabrication tolerances. PIN part ideally doesn't turn on at low currents ... Fabrication and DC testing were done. SiC material quality bottleneck ... – PowerPoint PPT presentation

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Title: 4HSIC JUNCTION BARRIERSCHOTTKY JBS DIODES


1
4H-SIC JUNCTION BARRIER/SCHOTTKY (JBS) DIODES
  • Rahul Radhakrishnan
  • Masters Technical Paper

2
Introduction
  • Modern power system trends
  • Size reduction
  • Higher efficiency
  • Fast switching devices
  • Rectifier
  • Low leakage current
  • Low on-resistance
  • Fast switching

3
Why JBS diode
  • Unipolar devices inherently faster
  • PIN junction reverse leakage current is lower
  • Schottky junction forward resistance is lower
  • Junction Barrier Schottky (JBS) diode combines
    both
  • Low barrier schottky
  • Predominant schottky action at low forward
    currents reduces minority carrier storage
  • Reverse depletion region of PIN junction expands
    laterally to pinch-off schottky junction

4
Silicon Carbide
  • High band-gap (3.2eV for 4-H SiC)
  • Low intrinsic concentration of charge carriers
  • Lower leakage current
  • 10-8/cm3 compared to 1010/cm3 for Si
  • Large saturated electron drift velocity
  • Faster switching
  • Small dielectric constant (9.7)
  • High thermal conductivity
  • High electron mobility
  • So, attractive candidate for power
    semiconductor!

5
SiC v/s Si JBS diode
  • Higher doped drift region
  • Minority carrier injection by PIN part is not
    essential in SiC JBS diodes.
  • So, reverse recovery is even better.
  • Smaller drift region thickness
  • About 10 times higher critical electric field
  • Series resistance is thus reduced
  • High voltage and current operation

6
JBS technology
  • Geometrical arrangement of PIN and Schottky parts
    critical
  • Schottky part carries forward current decides
    on-resistance
  • PIN part limited by fabrication tolerances
  • PIN part ideally doesnt turn on at low currents
  • Doping and thickness of semiconductor
  • Schottky metal
  • Overlay metal layers
  • Edge termination
  • Guard rings
  • Junction termination extension

7
JBS theory
  • On the left, schottky interface carries forward
    current
  • On the right, the PN junction depletion region
    widens to pinch off the schottky channels
  • Depletion region pinch off only under reverse
    bias
  • Schottky barrier is shielded from applied reverse
    voltage by pinch-off

8
Reverse Breakdown
  • Critical E-field Avalanche breakdown
  • Punch-through breakdown
  • 3-D field crowding at real junctions
  • Breakdown votage depends on
  • Critical field
  • Epitaxial layer doping
  • Epitaxial layer thickness
  • Edge-termination
  • Upto 80 of ideal breakdown by Guard rings
  • Upto 95 by Junction termination Extension

9
SiC JBS diodes
  • First used on Si by Williamovski and Baliga in
    1983-84
  • High voltage Si JBS later demonstrated.
  • Held and Dalquist realised SiC JBS diodes in 1998
  • No advanced edge termination
  • Later, very good JBS results achieved
  • In 2004, J.Wu, L.Fursin, P.Alexandrov and J.Zhao
  • 4308V blocking and 20.9m?.cm2 forward resistance
  • 30µm drift layer and active area 1.4mm2

10
Device Structure
  • n-/n 4H-SiC epitaxial wafer
  • 3 types of Devices- 3mm3mm, 4mm4mm 0.6mm0.6mm

11
Fabrication Steps-1
  • Wafer cutting, cleaning and alignment mark
    formation
  • Device mesa is about 3000-4000A

12
Fabrication steps-2
  • P implantation
  • Guard rings as well as PIN regions of MPS
  • Post implantation annealing at 1550ºC for 30
    minutes

13
Guard Ring Termination
  • Many p implanted guard rings separated by
    schottky regions
  • Designed to drop high voltage uniformly till edge
  • Electric field minimised
  • Right design of guard ring thickness and
    separation
  • Photograph of guard rings under backlight

14
Fabrication Steps-3
  • Surface passivation by thermal oxidation and
    PECVD
  • Window opening
  • Backside metal ohmic contact (AlTi/Ni)

15
Fabrication steps-4
  • Substrate-side ohmic contact with
    Ti(800A)/TiW(2500A)
  • Low schottky barrier height
  • Overlay metals

16
Photo- Masks
17
Testing after Schottky contact
18
Schottky metal Annealing
  • Various annealing temperatures from 500ºC to
    600ºC for upto 1 hour tried.
  • Annealing improves the Ti/SiC interface contact.
  • Best improvement in reverse characteristics
  • 550ºC for 20 in presence of inert gas Ar.
  • Au (2.5um) is used as the overlay metal, which
    decreases the forward resistance by providing a
    larger area for the spreading current

19
Testing after Schottky annealing
20
After Au overlay
21
Results
  • 7 probes used after final overlay.
  • 55A/cm2 at 1.5V and 170A/cm2 at 4V forward
  • More than 1.2kV breakdown voltage.
  • Yield is lower for bigger devices

22
Summary
  • Fabrication and DC testing were done
  • SiC material quality bottleneck
  • Switching test, high temperature test should be
    done
  • Packaging would further improve forward
    performance

23
Thank you!
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