650V Enhanced GaN Power Transistor Parameter Comparison Analysis Report: IGL65R140D2 vs VBQE165A20S
1. Product Overview
IGL65R140D2: Infineon CoolGaN™ G5 series 650V enhancement-mode GaN transistor, utilizing 200mm wafer technology, featuring ultra-fast switching speed, zero reverse recovery charge, and low gate and output charge. Package: PG-TSON-8. Suitable for industrial, telecom, and data center SMPS (half-bridge hard/soft switching topologies, such as totem-pole PFC and high-frequency LLC), as well as chargers and adapters.
VBQE165A20S: VBsemi 650V enhancement-mode GaN transistor with ultra-low gate charge (Qg typically 3.3nC), ultra-high switching frequency, zero reverse recovery charge, and built-in ESD protection. Package: DFN8*8. Suitable for server and telecom power supplies, switching power supplies (SMPS), power factor correction (PFC), fast battery charging, and other applications.
2. Comparison of Absolute Maximum Rated Values
Parameter |
IGL65R140D2 |
VBQE165A20S |
unit |
VDS |
650 |
650 |
V |
VDS,trans |
900 ( <1% duty cycle,<1μs ) |
800 (pulse,TPulse<200μs ) |
V |
VGS |
-10 ~ - (continuous) ; -25 ~ - (pulse) |
-1.4 ~ +7 |
V |
ID (Tc=25°C) |
13 |
20 |
A |
ID (Tc=125°C) |
- |
10 |
A |
IDM |
23 |
30 |
A |
PD (Tc=25°C) |
47 |
119 |
W |
TJ |
-55 ~ +150 |
-55 ~ +150 |
°C |
Tstg |
-55 ~ +150 |
-55 ~ +150 |
°C |
dv/dt |
200 |
150 |
V/ns |
Analysis: Both devices have a continuous withstand voltage of 650V. The IGL65R140D2 supports a higher transient voltage (900V) and a higher voltage slope (200V/ns). The VBQE165A20S has a higher continuous current capability (20A vs 13A) and higher power dissipation (119W vs 47W), as well as a higher pulse current (30A vs 23A). The IGL65R140D2 has a gate voltage range of negative turn-off, while the VBQE165A20S is -1.4V to +7V.
3. Comparison of Electrical Characteristic Parameters
3.1 Conduction characteristics
Parameter |
IGL65R140D2 |
VBQE165A20S |
unit |
V(BR)DSS |
650 (Min) |
650 (Min) |
V |
VGS(th) |
0.9 ~ 1.6 |
1.2 (Typ) |
V |
RDS(on) (VGS=6V) |
0.140 Typ/ 0.170 Max |
0.110 Typ (VGS=6V, ID=3.5A) |
Ω |
Analysis: The VBQE165A20S has a lower typical on-resistance (0.110Ω vs 0.140Ω), which helps reduce conduction losses. The IGL65R140D2 has a wider threshold voltage range (0.9~1.6V), while the VBQE165A20S has a typical threshold voltage of 1.2V.
3.2 Dynamic characteristics
Parameter |
IGL65R140D2 |
VBQE165A20S |
unit |
Ciss |
130 (Typ) |
120 (Typ) |
pF |
Coss |
22 (Typ) |
37 (Typ) |
pF |
Crss |
0.31 (Typ) |
0.4 (Typ) |
pF |
Qg (VGS=6V) |
1.8 |
3.3 |
nC |
Qgs |
Not provided |
0.3 (Typ) |
nC |
Qgd |
Not provided |
3 (Typ) |
nC |
Analysis: Both devices exhibit extremely low capacitance and gate charge, a key advantage of GaN technology. The IGL65R140D2 has a lower total gate charge (1.8nC vs 3.3nC) and smaller output capacitance (22pF vs 37pF), which is beneficial for ultra-high frequency switching. The VBQE165A20S provides more detailed gate charge distribution parameters.
3.3 Switching time
Parameter |
IGL65R140D2 |
VBQE165A20S |
unit |
td(on) |
7 |
4 (Typ) |
ns |
tr |
7 |
4 (Typ) |
ns |
td(off) |
10 |
5 (Typ) |
ns |
tf |
23 |
7 (Typ) |
ns |
Analysis: The VBQE165A20S has superior switching time parameters, especially the fall time (7ns vs 23ns), indicating a faster switching speed and suitability for higher frequency applications. The IGL65R140D2 also has an extremely fast switching time, but the testing conditions (Rg=12Ω) differ from the VBQE165A20S (Rg=3Ω), so direct comparison requires caution.
4. Body Diode Reverse Conduction Characteristics
Parameter |
IGL65R140D2 |
VBQE165A20S | unit |
VSD |
2.0 Typ (ISD=3.1A, VGS=0V) |
2.4 Typ (IS=3A, VGS=0V) |
V |
IS |
Not provided |
10 |
A |
ISM |
23 |
30 |
A |
Qrr |
0 |
0 |
nC |
Analysis: Both GaN devices have no body diode (and thus have reverse conduction capability), so their reverse recovery charge is 0nC. This is a significant advantage of GaN over Si devices, completely eliminating reverse recovery losses.
5. Thermal Characteristics
Parameter |
IGL65R140D2 |
VBQE165A20S |
unit |
RθJC |
2.7 (Max) |
1.05 (Typ) |
°C/W |
RθJA (SMD version) |
67 (Typ , Specific PCB conditions) |
62 (Typ) |
°C/W |
Analysis: The VBQE165A20S features a lower junction-to-ambient thermal resistance (62 °C/W) and higher power dissipation (119 W), enabling greater output power with excellent heat dissipation. This is key to its ability to handle higher power dissipation (119W vs 51W). With a well-designed thermal interface, the VBQE165A20S can achieve higher power density.
6. Summary and Selection Recommendations
Advantages of IGL65R140D2 |
Advantages of VBQE165A20S |
◆ Lower gate charge (Qg = 1.8 nC)
◆ Lower output capacitance (Coss = 22 pF)
◆ Higher transient withstand voltage (900 V)
◆ Higher voltage slope (dv/dt = 200 V/ns)
◆ Explicit thermal resistance parameters. (RθJC = 2.7°C/W) | ◆ Lower on-resistance (RDS(on) = 0.110Ω)
◆ Higher continuous current capability (20A)
◆ Higher pulse current (30A)
◆ Higher power dissipation (119W)
◆ Faster switching speed (tf = 7ns)
◆ Built-in ESD protection |
Selection Recommendations
Choose the IGL65R140D2: When applications are extremely sensitive to gate drive power, require very low switching drive losses, or need to handle higher transient voltages and higher dv/dt (such as high-frequency LLCs and high-density power supplies). Its well-defined junction-to-case thermal resistance is beneficial for thermal design.
Choose the VBQE165A20S: When applications require higher current output capability, lower on-resistance for high efficiency, higher power density (higher PD), and faster switching speeds. Its zero reverse recovery charge and built-in ESD protection are also suitable for high-frequency, high-efficiency scenarios, and its overall performance is well-balanced with a significant cost-performance advantage.
Note: This report is automatically generated based on the official datasheets for the IGL65R140D2 (Infineon) and VBQE165A20S (VBsemi). All parameter values are from the original manufacturer's datasheets; please refer to the latest official documentation for design selection.
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