Allan Deviation
Reading the Slope: What Each Line Tells You
σy²(τ) = (1/2) · 〈(ȳn+1 − ȳn)²〉
where ȳn is the average fractional frequency over the n-th interval of duration τ
Allan deviation: σy(τ) = √(σy²(τ))
| ADEV Slope (log-log) | Noise Type | σy(τ) ∝ | Physical Origin |
|---|---|---|---|
| −1 | White phase noise | τ−1 | Broadband noise in buffer amplifiers |
| −1/2 | White frequency noise | τ−1/2 | Thermal noise in oscillator loop |
| 0 (flat) | Flicker frequency noise | τ0 | 1/f noise in active devices |
| +1/2 | Random walk frequency | τ+1/2 | Environmental perturbations |
| +1 | Frequency drift | τ+1 | Crystal aging, temperature ramp |
Oscillator Technology Comparison
| Oscillator Type | ADEV at τ=1s | ADEV at τ=100s | ADEV Floor | Typical Cost |
|---|---|---|---|---|
| TCXO | 1×10−9 | 5×10−10 | 1×10−10 | $5 to $30 |
| OCXO | 1×10−12 | 3×10−13 | 1×10−13 | $200 to $2,000 |
| Rubidium | 3×10−11 | 5×10−12 | 1×10−12 | $1,000 to $5,000 |
| Cesium beam | 5×10−11 | 5×10−12 | 2×10−14 | $30,000+ |
| GPSDO | 2×10−12 (OCXO) | 5×10−13 | 1×10−13 | $500 to $3,000 |
Frequently Asked Questions
Why use Allan deviation instead of standard deviation?
Standard deviation diverges for flicker and random-walk FM noise, the dominant oscillator noise types beyond 1 second. Allan deviation uses two-sample differences that converge for all five noise types and reveals the dominant mechanism through its slope on a log-log plot (−1/2 for white FM, 0 for flicker FM, +1/2 for random walk).
What ADEV does a GPS-disciplined oscillator achieve?
Short-term (τ=1s) is set by the internal OCXO: ~2×10−12. Long-term (τ=10,000s) is governed by GPS: ~1 to 5×10−13. The crossover point is at τ=100 to 1,000s depending on the PLL bandwidth.
How does ADEV relate to phase noise?
Both measure oscillator instability in different domains. ADEV at averaging time τ corresponds approximately to phase noise at offset frequency 1/(2πτ). Close-in phase noise (1 to 100 Hz offset) maps to long averaging times; far-out noise (kHz+) maps to short averaging times.