
Application
Analog & Power
Lower on-resistance at the same breakdown and reliability, from low-voltage BCD switches to LDMOS.
How MST helps
Shorter, stronger power switches
Shrinking a power switch lowers its on-resistance, until spreading dopants cost breakdown or reliability. MST holds those dopants in place, in the same BCD or discrete flow.
| Device | Range | What MST does | Result |
|---|---|---|---|
| Low-voltage switch | 5 V · BCD | Blocks boron in the body, slows source/drain-extension spread, enables Lg scaling | Delivers best-in-class RspSilicon |
| LDMOS | 5–48 V · BCD | Holds a doped surface layer in the drift; blocks boron from diffusing up into the channel | 8–20% lower on-resistance at the same breakdown; breaks the 1-D silicon Rsp vs. BVdss limitMSTcad™ simulation · In R&D |
LV BCD · Source engineering · silicon
A shorter gate that still meets SOA
MST slows lateral dopant diffusion, so the effective channel is longer than the drawn gate: lower peak field and impact ionization. Same device doping as the silicon control, 180 nm foundry process.
−18%
specific on-resistance vs the silicon control, same device doping
Silicon0.25 µm
gate length that meets SOA, vs 0.27 µm for the silicon control, comparable HCI margin
Silicon+25–33 nm
effective channel length at the same drawn gate (SCM, NMOS and PMOS)
SiliconLDMOS · 5–48 V · MSTcad™ simulation
LDMOSIn R&D
MST carries the switch's source engineering into an LDMOS and holds a doped surface layer in the drift. Projected with MSTcad™ from MST silicon, it beats published BCD LDMOS at the same breakdown and breaks the 1-D silicon R_SP vs BV_DSS limit.
Below BCD
lower R_SP than leading 0.16–0.18 µm BCD platforms across 10–50 V
MSTcad™ projection>36 V
where the projected R_SP passes the classical 1-D silicon limit
MSTcad™ projection11 V
starting point: MST silicon; the model deck is validated on it
SiliconDrift engineering · MSTcad™ projection
Past the classical silicon limit
MST piles up phosphorus near the drift-layer surface; source engineering lowers the body resistance for a higher on-state breakdown. Same drift and RESURF implants as the silicon control.
−8 to −20%
R_SP across 10–50 V BV_DSS
MSTcad™ projectionBeyond 1-D
the silicon R_SP vs BV_DSS limit, for BV_DSS above 36 V
MSTcad™ projection+2–4 V
on-state breakdown, or >25% lower R_SP at the same on-state breakdown
MSTcad™ projectionBuried-channel LDMOS · MSTcad™ projection
A buried channel that extends the hot-carrier limit
A p⁺ poly gate and shallow n⁻ counter-doping move electrons off the interface. MST keeps the counter-doping shallow and the p-body in place, so only with MST does the buried channel keep its on-state breakdown. 16 V LDMOS: 12.5 nm oxide, 1.2 µm device, 0.68 µm gate, step oxide, field plate in the drift.
>18 V
on-state breakdown of a 16 V device (TLP), vs below 13 V for a silicon-control buried channel
MSTcad™ projection~20%
better R_ON than a conventional surface-channel LDMOS
MSTcad™ projection+2 V
BV_DSS vs surface channel: R_ON and on-state breakdown together only with MST
MSTcad™ projection
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Evaluate MST in your own process and devices with Atomera's engineering team.
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