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Title: Microwave Solid State Power Devices Yonglai Tian


1
Microwave Solid State Power DevicesYonglai Tian
2
  • Introduction of microwave power devices
  • Performance of Si and GaAs microwave devices
  • Wide bandgap semiconductors for microwave
    applications
  • Processing of WBG silicon carbide wafers
  • SiC microwave power devices
  • GaN microwave power device

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Various types of microwave power devices
Magnetron
Traveling wave tube
Gyrotrons
Klystron
5
Disadvantages
  • Large size
  • Heavy
  • Fixed frequency
  • Complicated power supply (HV)
  • Poor quality of waveform spectrum
  • Slow tuning and coupling
  • Cost

Single mode cavity for Microwave sintering of
advanced ceramics
6
Multiple DoD platform will benefit from microwave
solid state devices and WBG semiconductors
7
Electrodeless HID lamps driven by microwaves
200w aperture HID lamps (7mm) driven by solid
state microwave devices
1400w magnetron driven HID lamps,
8
Various types of microwave solid state devices
  • Bipolar Junction Transistors (BJT)
  • Si BJT
  • HBT (hetero junction bipolar transistor)
  • AlGaAs-GaAs HBT
  • SiGe-Si HBT
  • Field Effect Transistors
  • GaAs MESFET (metal-semiconductor field effect
    transistors)
  • HEMT (high electron mobility transistors)

9
Various types of microwave solid state devices
  • Wide Bandgap Transistors
  • SiC
  • SIT (static induction transistors)
  • MESFET (metal-semiconductor field effect
    transistors)
  • HBT (hetero junction bipolar transistor)
  • GaN
  • HEMT (high electron mobility transistors)

10
  • Introduction of microwave power devices
  • Performance of Si and GaAs microwave devices
  • Wide bandgap semiconductors for microwave
    applications
  • Processing of WBG silicon carbide wafers
  • SiC microwave power devices
  • GaN microwave power device

11
Performance characterization
  • Out put power Pmax
  • Pmax a Vmax x Imax
  • Vmax Voltage breakdown
  • Imax Heat removed, gate width and length
  • Power Density PD
  • PD Vmax x Current density
  • Vmax Voltage breakdown
  • Current density limited by bandgap and thermal
    conductivity

12
Performance characterization
  • Frequency
  • f max a (Vs/L)
  • Vs. saturated carrier velocity
  • Gate length
  • Pma a 1/f2
  • Efficiency PAE
  • Depends on wave shape, impedance, leakage
    current and power gain

13
Widely used Si microwave devices
  • A typical Si BJT characteristics
  • Frequency 2.7-2.9 GHz
  • Output power 105 W
  • Pulse width 50 mm
  • Duty cycle 10
  • Gain 6.5 db (min)
  • Efficiency 40 (min)
  • Supply voltage 40V
  • Si BJT
  • lt 5 GHz
  • 100-600W at 1 GHz
  • gt 40 Efficiency
  • Low cost
  • Limitation
  • Pmax voltage breakdown and current (limited by
    emitter periphery and resistivity of epitaxial
    layer)
  • f limited by carrier mobility,
  • capacitance C bc

14
GaAs MESFET (Metal semiconductor field effect
transistors)
  • GaAs MSFET
  • 3-30 GHz
  • Power density 0.5-0.8 w/mm
  • Power level and cost
  • Frequency band Power (W) cost ()
  • C and S 10 300
    20 600 30 900
  • Ku 10 1000 15
    1500
  • Limitation
  • f and Pmax gate length, thermal conductivity

15
HEMT and HBT
  • HEMT (High electronic mobility transistor)
  • AlGaAs-GaAs heterojunction
  • 5-100 GHz
  • High frequency
  • High Pmax
  • High efficiency
  • Low noise
  • HBT (heterojunction bipolar junction transistor)
  • Similar to BJT, but much higher power and
    frequency performance

16
State of the art power output performance
17
State of the art power density performance
18
State of the art PAE performance
19
Evolution of microwave device noise figures
20
  • Introduction of microwave power devices
  • Performance of Si and GaAs microwave devices
  • Wide bandgap semiconductors for microwave
    applications
  • Processing of WBG silicon carbide wafers
  • SiC microwave power devices
  • GaN microwave power device

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Advantages of wide bandgap semiconductors(SiC,
GaN and diamond)
  • Wide bandgap
  • SiC 3.2 eV
  • GaN 3.4 eV
  • Si 1.1 eV
  • GaAs 1.4 eV
  • 3 times higher than that of Si and GaAs
  • High service temperature of 650 oC due to the
    high intrinsic temperature
  • Low noise

26
Advantages
  • High breakdown voltage
  • SiC 10 times higher than that of Si and GaAs
  • High output power due to high V
  • High operating frequency
  • Short-channel MESFETs in SiC
  • Fmax 50 GHz

27
Advantages
  • 3. High thermal conductivity
  • SiC 4.9 w/(C-cm)
  • 10 times higher than that of Si and GaAs
  • Si 1.6 w/(C-cm)
  • GaN 0.5 w/(C-cm)
  • High Saturated velocity
  • SiC 2.2 x107 m/s
  • 2 times higher than that of Si and GaAs
  • Si and GaAs 1 x107 m/s

28
Physical characteristics of Si, GaAs and main
wide bandgap semiconductors
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WBG semiconductor material challenges
32
  • Introduction of microwave power devices
  • Performance of Si and GaAs microwave devices
  • Wide bandgap semiconductors for microwave
    applications
  • Processing of WBG silicon carbide wafers
  • SiC microwave power devices
  • GaN microwave power device

33
Growth of SiC single crystal
  • J. A. Lely , Philips Labs 1955 sublimation
    process for growing a-SiC crystals
  • Davis at North Carolina State University (NCSU),
    1987 seeded-growth sublimation process
  • Cree Res, started in 1987 by students from the
    NCSU.
  • Cree, 1990, Introduction of 25 mm single crystal
    wafers of 6H-SiC 1990

34
Physical vapor transport (PVT) growth of SiC
single crystal wafers
  • PVT growth process
  • Evaporation of SiC charge materials
  • Transport of vapor spices to the growth surface
  • Adsorption surface diffusion and incorporation of
    atoms into crystal.
  • Temperature 2000-2300oC
  • DT of 10-30C controlled by moving RF coil
  • Growth rate controlled by DT and pressure in
    reactor

35
Defects in SiC wafer
  • Micropipes breakdown at low voltage
  • Dislocations
  • Low angle grain boundaries
  • Stacking faults

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GMU WBGS research projectsIon implantation of
SiC wafers
  • Ion implantation is the only viable selective
    area doping techniques for SiC device production
  • N and P were implanted in p-type and Al and B
    were implanted in n-type 6H-SiC using single and
    multiple ion energy schedules ranged from 50 KeV
    to 4 MeV
  • Second ion mass spectrometry measurements (SIMS)
    were conducted to obtain the implant depth
    profiles
  • Doping layer theickness.

38
N-implanted SiC (50 KeV to 4MeV at 700oC)
39
B-implanted SiC (50 KeV to 4MeV at 700oC)
40
Multiple energy P-implanted SiC
41
Rapid annealing of ion implanted SiC
  • The crystal lattice is damaged by the penetration
    of ion energetic ions
  • Post annealing is necessary to recover the
    lattice damage
  • Microwave and conventional annealing at 1500C
  • Microwave Heating rate 200oC/min, total time
    20 min.
  • Conventional heating rate 10oC/min, total time
    3 hr.
  • Rutherford backscattering (RBS) measurements are
    conducted before and after ion-implantation to
    study the recovery of the crystal lattice.

42
RSB spectra on N-implanted SiC
43
Sheet resistivity of annealed SiC wafersGMU data
44
  • Sheet resistivity of nitrogen-implanted 4H-SiC
    as a function of time and temperature.

Sheet resistivity of phosphorus -implanted 4H-SiC
as a function of time and temperature.
45
Best Reported Sheet Resistivity of Ion Implanted
SiC
. Figure 2. Sheet resistivity of Al implants
into 6H silicon carbide at room tmperature
Figure 1. Sheet resistivity of nitrogen implants
into 6H silicon carbide at room tmperature
46
  • Introduction of microwave power devices
  • Performance of Si and GaAs microwave devices
  • Wide bandgap semiconductors for microwave
    applications
  • Processing of WBG silicon carbide wafers
  • SiC microwave power devices
  • GaN microwave power device

47
SiC microwave power devices
  • High power 4H-SiC static induction transistors
    (SITs)
  • Vertical short channel FET structure
  • Current flow vertically by modulating the
    internal potential of the channel using
    surrounding gate structure
  • Characteristics similar to a vacuum-tube tiode
  • 470W (1.36 /mm) at 600 MHz
  • 38 W (1.2 w/mm) at 3 GHz
  • PAE 47

48
High power 4H-SiC static induction transistors
(SITs)
Cross section of a SiC SIT
SEM photo of a SIT device. The mesa fingers are 1
µm wide and 100 µm long. The total mesa length is
1 cm (100 fingers).
Measured static I-V characteristics of a SIT
49
  • The best performance
  • High output power 900 W (at 1.3 GHz, drain
    efficiency 65, gain 11 dB)
    Northrop-Grumman/ Cree Inc
  • High frequency performance with a cut-off
    frequency of 7 GHz Purdue

A comparison of SIT with other relevant SiC
microwave devices..
50
High power SiC MESFET
  • Three epitaxial layers
  • P buffer layer
  • Channel layer doped Nd3x1017cm-3
  • Heavily doped n cap layer
  • Performance
  • Pmax 15W
  • Frequency 2.1 Ghz
  • Power density 1w/mm
  • PAE 54

a
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Cross section of SiC MESFET. The epitaxial layers
were grown on a semi-insulating SiC substrate,
including p-buffer layer and a n-doped channel
layer
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  • Introduction of microwave power devices
  • Performance of Si and GaAs microwave devices
  • Wide bandgap semiconductors for microwave
    applications
  • Processing of WBG silicon carbide wafers
  • SiC microwave power devices
  • GaN microwave power device

55
GaN Power High electronic mobility transistors
  • two dimensional electron gas with a high mobility
    is formed at the AlGaN-GaN heterojunction
    interface, the mobility can be in excess of 1000
    cm2/Vs
  • High frequency 100GHz
  • High power density 10w/mm
  • Base station microwave power amplifier
  • highly linear mixers
  • high power switches

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