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Decoupling strategy — beyond “0.1 µF everywhere.”

TL;DR

  • A capacitor only decouples below its self-resonant frequency; above it, it’s an inductor. So you tile values to keep the PDN below target impedance across the band.
  • The real enemy is anti-resonance — the impedance peak between two cap values where one’s inductance rings with the next one’s capacitance. That peak, not the average, blows your budget.
  • Placement and mounting inductance often matter more than the cap value. The smallest, closest cap wins at high frequency.

Why a capacitor stops being a capacitor

Every real cap is a series R-L-C: capacitance C, equivalent series resistance ESR, and equivalent series inductance ESL (package + mounting). Its impedance is minimum at the self-resonant frequency:

fSRF = 1 / (2π·√(L·C)) — above fSRF the ESL dominates and |Z| rises. A 0.1 µF 0402 self-resonates near ~30–50 MHz; past that it does nothing for you.

This is why “0.1 µF everywhere” fails on fast loads — it leaves the rail undecoupled above ~50 MHz, exactly where modern logic draws its fastest current.

Choosing values against the impedance profile

Work the target-impedance method backwards: pick a set of values whose self-resonant frequencies tile the band you must cover, with enough of each to push |Z| under the target. In practice:

  • Bulk (10–100 µF) near the VRM for low-frequency droop.
  • Mid (0.1–1 µF) for the MHz region.
  • High-frequency (1–22 nF, smallest body) at the power balls.

Don’t space the values too far apart — wide gaps create deep anti-resonance peaks. Values within ~a decade, with the plane pair providing high-frequency capacitance, keep the profile flat.

|Z(f)| under target across band · anti-resonance at 18 MHz damped with controlled-ESR cap
Figure 1 — A healthy decoupling network: flat under target, anti-resonance peaks damped.

Placement & mounting inductance

At high frequency, the loop inductance from the cap to the IC power/ground pins dominates — and that’s set by layout, not the cap. Rules that hold up:

  1. Smallest, highest-frequency caps closest to the power pins/balls.
  2. Minimize the via-to-pad loop: vias at the pad ends, or via-in-pad for BGAs.
  3. Tight power/ground plane spacing gives you “free” high-frequency plane capacitance with near-zero ESL.
  4. Don’t share a long fanout trace between a cap and the pin it’s decoupling — that trace’s inductance defeats the cap.
The cap value sets where it helps. The mounting inductance sets how much. Layout is half the PDN.

Decoupling checklist

  • ☐ Derive the target impedance first (V·ripple% / ΔI)
  • ☐ Tile cap SRFs across the band the board can influence
  • ☐ Keep values within ~a decade to avoid deep anti-resonance
  • ☐ Smallest/HF caps at the power balls; via-in-pad for BGAs
  • ☐ Tight plane pair for HF plane capacitance
  • ☐ AC PDN sim to catch anti-resonance peaks; damp as needed

Want it verified?

Decoupling against a real impedance profile is core PDN design — DC + AC, coupled with thermal in TRM. Scope a project.

References

  1. Smith & Bogatin, Principles of Power Integrity for PDN Design.
  2. Istvan Novak, decoupling and anti-resonance papers (DesignCon).
  3. Murata/TDK capacitor SRF and ESL datasheets.