Wilson Bandgap Reference: Adding a Third Transistor to Fix the Widlar's Weaknesses

2026-08-24

The classic Widlar bandgap reference uses two transistors with different current densities to generate a PTAT (Proportional To Absolute Temperature) voltage that cancels the CTAT (Complementary To Absolute Temperature) drift of a VBE. It works, but it has a subtle flaw: the collector currents of the two transistors are set by a resistor ratio, and any mismatch in the base currents of Q1 and Q2 corrupts the ratio. The Wilson bandgap adds a third transistor to force equal collector currents through negative feedback, dramatically improving accuracy.

How it works: Two matched PNPs form a current mirror at the top of the circuit, forcing IC1 = IC2. Q1 runs at high current density (small emitter area, or single unit), Q2 runs at low current density (N parallel units, typically 8). The difference in VBE across the two transistors appears across a resistor R1 in Q2's emitter:

The third transistor Q3 senses the output and feeds back to close the loop. The output voltage is VBE3 + (R2/R1) · VT · ln(N). Choose R2/R1 so the PTAT term contributes about +2 mV/°C at the output, exactly canceling the -2 mV/°C of VBE3. You land at approximately 1.25 V — the silicon bandgap voltage extrapolated to 0 K.

Worked example: Target output 1.25 V at 300 K with N = 8. VBE3 ≈ 0.65 V, so the PTAT term must add 0.60 V. With ΔVBE = 54 mV, you need R2/R1 = 0.60/0.054 ≈ 11.1. If R1 = 10 kΩ, then R2 ≈ 111 kΩ. Tail current will be 54 mV / 10 kΩ = 5.4 µA.

Real-world example: The venerable REF200 and countless CMOS voltage references (LM4040, MAX6100 series) use Wilson-style bandgap topologies internally. The Wilson variant is preferred over the plain Widlar in modern IC processes because the added feedback loop makes the reference far less sensitive to β mismatch and Early voltage — you can hit 0.5% initial accuracy without laser trimming, and 50 ppm/°C over -40 to +85 °C with basic curvature correction.

Rule of thumb: If your bandgap output drifts more than you'd expect from VBE curvature alone, suspect the current-mirror mismatch first. The Wilson topology's feedback fixes this at the cost of one transistor and a slightly higher minimum supply voltage (roughly 2·VBE + VCE(sat) ≈ 1.5 V).

Key Takeaway: The Wilson bandgap adds a feedback transistor to enforce equal collector currents in the ΔVBE pair, eliminating the current-mirror mismatch error that limits the accuracy of the simpler Widlar bandgap.

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