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Semiconductors                                                                               Semiconductors


 in catastrophic failure.



 Besides overstress on the enabled gate, disa-
 bled gates can be affected too. If the V  >V , ID
 GS
 th
 starts flowing in the disabled device. The shoot-
 through current will lead to further excitation of
 the resonant tank and a self-sustained oscilla-
 tion with shoot-through currents can occur. This
 is show in Figure 2.


          Figure 3: schematic for simulation.
 Often, designers try to mitigate these oscilla-
 Figure 1: Reverse Recovery current SiC MOSFET.
 tion effects by adding an external C  capacitor   real gate. The external C  builds an additional   best possible switching. Enabling transients in
                                 GS
 GS
 Why do you need to pay attention to the SiC   (impact seen in Figure 2). This capacitor conven-  resonance tank and worsens the effects of the   excess of 120 V/ns and 6 A/ns (with best in class
 MOSFET gate? Despite having a conventional SiO    iently dampens away oscillations and seems to   fast I  transients (snap back) on the gate. Using   MOSFETs), provided the rest of the loop parasitic
               RR
 2
 gate oxide, this oxide has worse properties than   fix the problem, or so it seems. What is overseen   physical, scalable SPICE models one can study   inductance is taken care of.
 the classical Si-SiO  interface found in conven-  is the fact that the dampening and the resulting   these difficult to probe effects and will quickly
 2
 tional Si based semiconductors. This is due to   clean oscilloscope pictures are resembling the   notice that the C  capacitor. Figure 3 shows the
                          GS
 intrinsic defects at the interface of SiO  grown   events outside the real gate, what the designer   schematic for the simulations and Figure 4 the
 2
 on the Si terminated face of SiC. This makes the   is doing in reality is worsening the effects on the   resulting outcome, showing a 7 V overstress on
 oxide more susceptible to over voltage, and other   the V  caused by the interplay of the fast I  and
               GS
                                                    RR
 electric stress limiting the V GSMax  considerably   the added dampening capacitor.
 relative to Si based devices.
          The key to successful high speed switching using
 Figure 1 shows the snappy body diode of a SiC   SiC MOSFETs is a proper adjustment of the gate
 MOSFE, the small Q  and the short trr can be   circuit and the drive conditions to the used de-
 RR
 tricky to measure and are often convoluted with   vice, a careful read of the data sheets will quick-

 the test systems parasitic capacitances. How-  ly reveal the fast range of internal RGs current
 ever di/dt of >40 A/ns in the I  return leg can   devices have. Furthermore, removing external
 RR
 occur. This ultra-fast I  event can pull the V  on   C  capacitors, setting the right external gate
           GS
 GS
 RR
 the device itself up in excess of Volts and cause   resistor R , and utilizing packages with a source
                   G
 severe overstress during each turn on cycle.   sense (TO-247-4L, D2PAK-7L or similar), paired
 The resulting overshoot is proportional to the I    Figure 2: Switching transient of SiC MOSFET at:   with the correct gate loop design will yield in the   Figure 4: analysis of simulation.
 RR
 speed; eventually this continues stress will result   V =720V, I =20A, T =175°C, R =10Ω, C =10nF.
 DD  D  C  G  GS
          For More Information




                 ▶ ON Semiconductor



                 ▶ (S15) How to kill a SiC MOSFET – Errors in Gate Circuit Design, ON Semiconductor

                – Wide bandgap Conference 2020




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