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Phase Noise to Jitter Converter

Convert oscillator phase noise (dBc/Hz) to RMS jitter in ps and ADC SNR limit. Integrate over offset frequency range for clock design. Free, instant results.

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Formula

Jrms=(210(Lint/10))/(2πf0)J_rms = √(2·10^(L_int/10)) / (2π·f₀)
J_rmsRMS jitter (s)
L_intIntegrated phase noise power (dBc)
L(f)Phase noise spectral density (dBc/Hz)
f₀Carrier frequency (Hz)
BWIntegration bandwidth (Hz)
SNR_jADC SNR limit from clock jitter (dB)

How It Works

The Phase Noise to Jitter Calculator converts oscillator phase noise (dBc/Hz) to time-domain jitter (ps RMS) — essential for clock source selection, high-speed serial link design, and radar system development. Clock IC designers, SERDES engineers, and RF system architects use this to verify timing margins and select oscillators. Per IEEE 1139-2008, phase noise L(f) at offset f from carrier relates to jitter via integration: sigma_rms = (1/(2*pi*fc)) sqrt(2 integral[L(f)df]) from f1 to f2. A -100 dBc/Hz oscillator at 100 MHz with integration from 12 kHz to 20 MHz yields approximately 0.5 ps RMS jitter. Per Egan "Phase-Lock Basics" (2nd ed.), jitter directly impacts bit error rate: 0.1 UI jitter at 10 Gbps (10 ps) causes BER floor of 1e-12. Modern XO/TCXO oscillators achieve -110 to -150 dBc/Hz at 10 kHz offset, translating to sub-picosecond jitter.

Worked Example

Select oscillator for 10 Gbps SERDES requiring < 1 ps RMS jitter integrated 12 kHz to 20 MHz. Step 1: UI = 100 ps at 10 Gbps. Per IEEE 802.3, jitter budget = 0.15 UI = 15 ps total. Step 2: Clock source allocation = 30% = 4.5 ps. Step 3: Convert to phase noise requirement. For 100 MHz clock: -100 dBc/Hz flat yields ~0.8 ps. -110 dBc/Hz yields ~0.25 ps. Step 4: Select oscillator with L(10kHz) < -105 dBc/Hz. Step 5: Verify: SiTime SiT9121 specifies -115 dBc/Hz at 10 kHz, yielding 0.15 ps RMS — 30x margin. Per Maxim AN-3359, this approach ensures robust 10G link operation.

Practical Tips

  • Per IEEE 1139-2008, always specify integration bandwidth when reporting jitter — 12 kHz to 20 MHz is industry standard for SERDES
  • Close-in phase noise (< 1 kHz offset) dominates jitter for narrowband PLLs; far-from-carrier dominates for wideband systems
  • Use spectrum analyzer with cross-correlation for < -140 dBc/Hz measurements per Keysight AN 1316
  • Budget 3 dB margin below phase noise spec to account for temperature variation per SiTime application notes

Common Mistakes

  • Assuming linear phase noise to jitter relationship — integration is required; flat -100 dBc/Hz across decade yields different jitter than -100 at center
  • Neglecting integration bandwidth — 1 kHz to 100 MHz integration yields 10x higher jitter than 12 kHz to 20 MHz
  • Using single-point phase noise — must integrate across full PLL bandwidth or SERDES CDR bandwidth per IEEE 802.3

Frequently Asked Questions

L(f) in dBc/Hz at specified offset frequency from carrier per IEEE 1139-2008. Example: -110 dBc/Hz at 10 kHz offset means phase noise power in 1 Hz bandwidth at 10 kHz from carrier is 110 dB below carrier. Convert to jitter: integrate L(f) from f_low to f_high, take sqrt, divide by 2*pi*f_carrier.
Per Egan: Phase noise (1) sets radar Doppler resolution — -100 dBc/Hz at 1 kHz limits velocity resolution to 0.1 m/s. (2) Degrades EVM in digital modulation — -30 dBc phase noise floor limits 64-QAM EVM to 3%. (3) Causes reciprocal mixing — -90 dBc/Hz LO adds 10 dB to receiver noise at 1 MHz offset. Critical for 5G mmWave where < 1 degree RMS phase error required.
Per SiTime: Crystal oscillators degrade 3-10 dB from -40C to +85C. MEMS oscillators maintain < 1 dB variation. Oven-controlled (OCXO) maintain < 0.5 dB but consume 1-5W. For temperature-sensitive applications, specify phase noise at worst-case temperature, not 25C typical.

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