Parameter Comparison and Analysis Report of N-channel (Enhancement Mode) GaN Power Transistors: IGLD65R140D2 vs VBQE165A20S
1. Product Overview
IGLD65R140D2: Infineon CoolGaN™ G5 series 650 V enhancement-mode GaN transistor, using 200 mm wafer technology, featuring ultra-fast switching speed, no reverse recovery charge, low gate and output charge, and excellent commutation robustness. Package: PG-LSON-8 (with Kelvin source). Suitable for industrial, telecom, data center SMPS, totem-pole PFC, high-frequency LLC, and charger adapters.
VBQE165A20S: VBsemi 650 V enhancement-mode GaN transistor with ultra-low gate charge, ultra-high switching frequency, no reverse recovery charge, and built-in ESD protection. Package: DFN8×8. Suitable for server and telecom power supplies, switching power supplies, PFC, and fast battery charging.
2. Comparison of Absolute Maximum Rated Values
Parameter |
IGLD65R140D2 |
VBQE165A20S |
unit |
VDS,max |
650 |
650 |
V |
VDS,trans |
900 |
800 |
V |
VDS,pulse |
750 (Tc=25°C) / 650 (Tc=125°C) |
750 |
V |
VGS |
-10 ~ Not provided |
-1.4 ~ +7 |
V |
VGS,pulse |
-25 ~ Not provided |
Not provided |
V |
ID (Tc=25°C) |
12 |
20 |
A |
ID (Tc=125°C) |
Not provided |
10 |
A |
IDM |
23 |
30 |
A |
PD (Tc=25°C) |
42 |
119 |
W |
TJ |
-55 ~ 150 |
-55 ~ 150 |
°C |
Tstg |
-55 ~ 150 |
-55 ~ 150 |
°C |
EAS |
Not provided |
Not provided |
mJ |
dv/dt |
200 |
200 |
V/ns |
Analysis: Both devices have a withstand voltage of 650 V. The VBQE165A20S offers higher continuous current (20 A vs 12 A) and power dissipation (119 W vs 42 W), making it suitable for higher power requirements. The IGLD65R140D2 has stronger transient voltage capability (900 V vs 800 V) and a wider gate voltage range (negative voltage down to -10 V).
3. Comparison of Electrical Characteristic Parameters
3.1 Conduction characteristics
Parameter |
IGLD65R140D2 |
VBQE165A20S |
unit |
V(BR)DSS |
650 (Min) |
650 (Min) |
V |
VGS(th) |
0.9 ~ 1.6 (Typ 1.2) |
Typ 1.2 (Scope not provided) |
V |
RDS(on)(VGS=6V / 10V) |
Typ 0.140 / Max 0.170 (VGS=10mA) |
Typ 0.110 / Max 0.140 (VGS=6V) |
Ω |
gfs |
Not provided |
Not provided |
S |
Analysis: The VBQE165A20S has a lower on-resistance (typically 0.110 Ω vs 0.140 Ω), which helps reduce conduction losses. The IGLD65R140D2 has a well-defined threshold voltage range, which is beneficial for driver design.
3.2 Dynamic characteristics
Parameter |
IGLD65R140D2 |
VBQE165A20S |
unit |
Ciss |
155 |
120 |
pF |
Coss |
22 |
37 |
pF |
Crss |
0.31 |
0.4 |
pF |
Qg |
1.8 |
3.3 |
nC |
Qgs |
Not provided |
0.3 |
nC |
Qgd |
Not provided |
3 |
nC |
Analysis: The IGLD65R140D2 has an extremely low total gate charge (1.8 nC), significantly reducing drive power consumption. The VBQE165A20S has a slightly smaller input capacitance (120 pF vs 155 pF), but a larger output capacitance (37 pF vs 22 pF). Both have extremely low Crss, making them suitable for high-frequency switching.
3.3 Switching time
Parameter |
IGLD65R140D2 |
VBQE165A20S |
unit |
td(on) |
7 |
4 |
ns |
tr |
7 |
3 |
ns |
td(off) |
10 |
5 |
ns |
tf |
23 |
1.2 |
ns |
Analysis: The VBQE165A20S has a significantly faster switching speed, especially with a fall time of only 1.2 ns, which is far superior to the IGLD65R140D2's 23 ns. This can greatly reduce switching losses in high-frequency applications.
4. Body Diode Reverse Conduction Characteristics
Parameter |
IGLD65R140D2 |
VBQE165A20S |
unit |
VSD |
Typ 2.0 / Max 2.4 |
Typ 2.4 |
V |
trr |
0(Zero reverse recovery time) |
0 |
ns |
Qrr |
0 |
0 |
μC |
IRRM |
Not provided |
Not provided |
A |
Analysis: Both devices are GaN, which have no reverse recovery charge (Qrr=0). In a bridge topology, they can eliminate diode reverse recovery losses and improve efficiency.
5. Thermal Characteristics
Parameter |
IGLD65R140D2 |
VBQE165A20S |
unit |
RθJC |
3.0 (Max) |
1.05(Typ) |
°C/W |
RθJA |
130 (Minimum package) / 67 (SMD 6cm²copper foil) |
62 (Max) |
°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
Advantage of IGLD65R140D2 |
Advantage of VBQE165A20S |
◆ Lower total gate charge(1.8 nC),Ultra-low power drive |
◆ Higher continuous current(20 A)and power dissipation(119 W) |
◆ lower output capacitance(22 pF),Lower light-load power loss |
◆ Faster switching speed(tf=1.2 ns,td(off)=5 ns) |
◆Higher transient withstand voltage(900 V),Good overvoltage robustness |
◆ lower on-resistance(Typ 0.110 Ω) |
◆ Junction-to-Case Thermal Resistance(3.0 °C/W) |
◆Lower thermal resistance RθJA(62 °C/W),More flexible heat dissipation design |
◆ Wide gate voltage range(-10 V),Negative voltage drive compatibility |
◆ Built-in ESD protection enhances reliability |
Selection Recommendations
Choosing the IGLD65R140D2: When applications are extremely sensitive to gate drive power consumption, require higher transient voltage margins, or need to use negative voltage shutdown schemes (such as high-speed half-bridge drives), this device is superior due to its extremely low Qg and 900 V transient capability.
Choosing the VBQE165A20S: When greater current handling capacity (>12 A), higher power density (PD=119 W), and ultra-fast switching speed (tf<2 ns) are required, the VBQE165A20S is a better choice due to its low RDS(on), high current rating, and excellent thermal performance, making it particularly suitable for high-frequency, high-power-density power supply applications.
Note: This report is based on the official datasheets for Infineon IGLD65R140D2 and VBsemi VBQE165A20S. All parameter values are from the original manufacturer's documentation, and some missing parameters have been marked. Please refer to the latest official datasheet for design selection.
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