Title: Microwave Solid State Power Devices Yonglai Tian
1Microwave 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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4Various types of microwave power devices
Magnetron
Traveling wave tube
Gyrotrons
Klystron
5Disadvantages
- 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
6Multiple DoD platform will benefit from microwave
solid state devices and WBG semiconductors
7Electrodeless HID lamps driven by microwaves
200w aperture HID lamps (7mm) driven by solid
state microwave devices
1400w magnetron driven HID lamps,
8Various 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)
9Various 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
11Performance 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
12Performance 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
13Widely 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
14GaAs 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
15HEMT 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
16State of the art power output performance
17State of the art power density performance
18State of the art PAE performance
19Evolution 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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25Advantages 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
26Advantages
- 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
27Advantages
- 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
28Physical characteristics of Si, GaAs and main
wide bandgap semiconductors
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31WBG 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
33Growth 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
34Physical 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
35Defects in SiC wafer
- Micropipes breakdown at low voltage
- Dislocations
- Low angle grain boundaries
- Stacking faults
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37GMU 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.
38N-implanted SiC (50 KeV to 4MeV at 700oC)
39B-implanted SiC (50 KeV to 4MeV at 700oC)
40Multiple energy P-implanted SiC
41Rapid 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.
42RSB spectra on N-implanted SiC
43Sheet 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.
45Best 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
47SiC 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
48High 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..
50High 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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52Cross 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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54- 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
55GaN 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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