SiC Transistor Basics: FAQs

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SiC Transistor Basics: FAQs
Silicon Carbide (SiC) MOSFETs exhibit higher blocking voltage, lower on state resistance
and higher thermal conductivity than their silicon counterparts.
Oct. 9, 2013 Sam Davis | Power Electronics
Source URL: http://powerelectronics.com/discrete-power-semis/sic-transistor-basics-faqs
As an alternative to traditional silicon MOSFETs, silicon carbide MOSFETs offer the advantages of
higher blocking voltage, lower on-state resistance, and higher thermal conductivity. The devices
can replace silicon MOSFETs and IGBTs in many applications.
Why SiC Devices?
Silicon Carbide (SiC) MOSFETs exhibit higher blocking voltage, lower on state resistance and higher
thermal conductivity than their silicon counterparts. SiC MOSFETs are designed and essentially
processed the same way as silicon MOSFETs. The enhanced performance is derived from the material
advantages inherent in the silicon carbide physics. Due to its simple structure, ease of a design-in, and
low drive losses, the N-channel enhancement mode SiC MOSFET offers good compatibility as a
replacement for silicon MOSFETs and IGBTs.
What nomenclature do SiC devices employ? SiC transistors borrowed the same nomenclature as their silicon brethren: gate, drain and source, as
shown in Fig. 1. In addition, on-resistance and breakdown voltage of a SiC device have a similar
meaning as their silicon counterparts. On-resistance (RDS(ON)) vs. gate-source voltage curves are
similar to silicon MOSFETs. The temperature coefficient of SiC
MOSFET on-resistance is similar to the silicon MOSFET as it is
positive, but the magnitude of RDSon change is less over the
device operating range.
Fig. 1 - The schematic diagram of an enhancement
mode SiC MOSFET is similar to that of a silicon
MOSFET, having a gate, drain, and source.
How has the SiC transistor evolved? Adoption of SiC semiconductors has been limited by substrate costs, the material’s physical
idiosyncrasies and defect density. These issues have limited SiC devices to diodes in the last five
years. However, the wafer processing challenges have been largely resolved with development of
low-defect SiC wafers that make it possible to produce SiC MOSFETs. Cree introduced the first SiC
MOSFET in January 2011. This CMF20120D transistor was rated at 1200V, had 80 mΩ onresistance, and was housed in TO-247 package. Although its cost was higher than the Si IGBT it was
supposed to replace, the SiC MOSFETs have faster switching, better efficiency and better thermal
performance. The second generation SiC MOSFET, C2M0080120D, was released in March 2013
and has improved performance characteristics. Table 1 compares the key device parameters of the
first and second generation parts. Note, in particular, the reduction in die size and associated
capacitance values. This contributes to the better switching efficiency of the Gen2 device and the
sizable cost reduction as well.
Power Modules
Are there any SiC MOSFET Power Modules?
Cree introduced the industry's first commercially available all-silicon carbide (SiC) six-pack power
module in an industry standard 45 mm package (Fig. 2). When replacing a silicon module with
equivalent ratings, Cree's six-pack module reduces power losses by 75 percent, which leads to an
immediate 70 percent reduction in the size of the heat sink, or a 50 percent increase in power
density. The six-pack SiC module unlocks the traditional design constraints associated with power
density, efficiency and cost, thereby enabling the designer to create high performance, reliable
and low cost power conversion systems. When compared to state-of-the-art silicon modules, the
SiC 1.2 kV, 50 A modules deliver performance equivalent to silicon IGBT modules rated up to 150 A
depending upon efficiency requirement and switching frequency.
Fig. 2 - The SiC six-pack power module is housed in a standard 45 mm package. This module can
reduce power losses by 75 percent, compared with a functionally similar silicon MOSFET
module.
What gate drivers can be used with a SiC MOSFET?
Gate driver ICs suitable for SiC MOSFETs are available from IXYS, Texas Instruments and most
recently from Avago. Texas Instruments’ UCC2753x IC family are single-channel, high-speed, gate
drivers capable of driving SiC MOSFET power switches by up to 2.5 A source and 5 A sink
(asymmetrical drive) peak current (Fig. 3). Strong sink capability in asymmetrical drive boosts
immunity against parasitic Miller turn-on effect. The UCC2753x can also feature a split-output
configuration that allows the designer to apply independent turn-on and turn-off resistors to the
OUTH and OUTL pins, respectively, and easily control the switching slew rates.
Fig. 3 - Texas Instruments’ UCC2753x IC family of high-speed, gate drivers can handle SiC
MOSFET power switches by up to 2.5 A source and 5 A sink peak current. For the UCC27531 the
EN pull-up resistance to VREF = 500 kΩ, VREF = 5.8 V, in pull-down resistance to GND = 230 kΩ.
The driver has rail-to-rail drive capability and extremely small propagation delay, typically 17 ns.
The input threshold of UCC2753xDBV is based on TTL and CMOS compatible low-voltage logic,
which is fixed and independent of VDD supply voltage. Its 1V typical hysteresis offers excellent
noise immunity.
IXYS’ IXD_609SI is an automotive grade, high-speed gate driver. Its output can source and sink 9 A
of peak current, while producing rise and fall times of less than 45 ns. Both the output and input
are rated to 35 V. The input is virtually immune to latch-up, and proprietary circuitry eliminates
cross conduction and "shoot-through." The IXD_609SI has a Grade 1, -40 °C to +125 °C ambient
operating temperature range. It is AEC Q100 qualified and available in an 8-pin Power SOIC
package with an exposed metal back.
Avago’s ACPL-P346 is a high-speed 2.5 A gate drive optocoupler that contains an AlGaAs LED,
which is optically coupled to an integrated circuit with a power output stage. This optocoupler is
ideally suited for driving power and SiC MOSFETs used in inverter or AC-DC/DC-DC converter
applications. The high operating voltage range of the output stage provides the drive voltages
required by gate controlled devices. The voltage and high peak output current supplied by this
optocoupler make it ideally suited for direct driving MOSFETs at high frequency for high efficiency
conversion. The ACPL-P346 has the highest insulation voltage of VIORM= 891 V peak in the IEC/
EN/DIN EN 60747-5-5 and is UL1577 recognized with 3750 VRMS for 1 minute.
Optimizing Layout
How do you optimize layout to ensure proper gate drive?
To achieve fast switching time, the gate drive interconnections must have minimum parasitics,
especially inductance. This requires the gate driver to be located as close as possible to the
C2M0080120DD. Exercise care in selecting an appropriate external gate resistor to manage
voltage overshoot and ringing. As with any majority carrier device, the C2M0080120D has no tail,
so the amount of drain voltage overshoot and parasitic ringing is noticeably higher. The higher
ringing can be a concern, because the lower transconductance and low threshold voltage of the
C2M0080120D di/dt can couple back to the gate circuit through any common gate/source
inductance. Ferrite beads help minimize ringing while maintaining fast switching time. A high value
resistor (10 kΩ) between gate and source should be used in order to prevent excessive floating of
the gate during system power up propagation delays.
Does the SiC MOSFET have a body diode? Like conventional silicon MOSFETs, the SiC MOSFET has a body diode – a PN type with 3.1 V to 3.3
V threshold voltage. The higher turn-on voltage reduces efficiency slightly versus an external SiC
Schottky diode, but the body diode has a much lower reverse recovery charge than a silicon
MOSFET’s body diode.
How does the efficiency of the two generations of SiC MOSFETs compare with silicon IGBTs?
Fig. 4 shows efficiency testing data with the SiC MOSFETs at 100KHz (first generation SiC MOSFET
CMF20120D and second generation SiC MOSFET C2M0080120D) and Si IGBT (IGW40N120H3) at
20 KHz. Output diodes used for both switch devices were Cree 1200 V SiC Schottky diode
C4D10120D, thus assuring a fair comparison. All data are based on an external gate resistor of 2 Ω.
Even with five times the switching frequency, the SiC solution was able to achieve a maximum
efficiency of 99.3% at 100 KHz, reducing losses by 18% from the best efficiency of the IGBT
solution at 20 KHz. At light loads, where the two designs exhibit the poorest efficiency, the 100
KHz SiC solution still matched the 20KHz performance of the silicon system. This comparison
shows that the SiC MOSFET exhibits both an efficiency and a frequency advantage over a silicon
IGBT. Highly efficient systems can thus be designed with SiC MOSFETs at switching frequencies
that allow lower magnetic element values, reducing overall system size, weight and cost.
Fig. 4 - SiC
MOSFET
efficiency at
100 KHz for
the
CMF20120D
and
C2M0080120D
outperfrom a
silicon IGBT
(IGW40N120H
3) at 20 kHz.
Minimizing EMI
What should be done to minimize EMI in SiC MOSFET circuits? EMI design should be given attention with high frequency SiC power devices. There are some
practical approaches that can be employed to limit the influence of noise with high switching
frequency.
With high switching frequency and fast switching times of SiC MOSFETs, drain voltage
ringing is potentially much higher due to parasitic oscillation, especially due to parasitic
capacitance of the inductor. When the circuit switches are turn-on and turn-off, there is high
frequency resonance between the parasitic capacitance of inductor and stray inductance in the
switching power loop, which will lead to excessive ringing. To reduce the ringing at high frequency,
use a single layer winding inductor. A single layer winding can dramatically reduce the parasitic
capacitance of the inductor with good flux coupling. The will result in reduced ringing within the
VDS switching node.
This article was prepared with the help of Cree Inc., Durham, NC.
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