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Unified Notation Table

β: This English translation is in beta — the Traditional-Chinese original is the authoritative version.

Different papers write the same thing with different symbols. This page unifies them; every later chapter follows this table. If you encounter a different convention in one of the papers, come back here to cross-reference.

How to use this page: skim it once to get acquainted; when actually reading the derivations, come back and look up any symbol you do not recognize. Every quantity is labeled with its unit — doing a dimension check is the fastest way to catch mistakes.

Main symbols

SymbolMeaning (intuition)UnitUsed inNotes
tttimesall
τ\tauinjection instant of the noise/impulses[P1]the ISF's argument is the injection phase ω0τ\omega_0\tau
TToscillation period T=1/f0T=1/f_0sall
ω0\omega_0oscillation angular frequency =2πf0=2\pi f_0rad/sall
f0f_0oscillation (carrier) frequencyHzalle.g. 5 GHz
ϕ(t)\phi(t)excess phase (the deviation beyond the ideal phase)rad[P1][P2]phase noise / jitter lives here
Δϕ\Delta\phiphase step / phase errorradallthe jump caused by one impulse
A(t)A(t)instantaneous amplitudeV or normalized[P1][P4]perturbations get pulled back (see [P4] APF)
Γ(ω0τ)\Gamma(\omega_0\tau)ISF, the oscillator's "phase sensitivity" to noise; dimensionless, 2π2\pi-periodic[P1]not the noise itself, but a weighting function
qmaxq_{max}maximum node charge swing =CVmax=C\cdot V_{max}C[P1]used for normalization; the larger it is, the lower the phase noise
Δq\Delta qinjected charge =idt=\int i\,dtC[P1]e.g. 1 fC
in(t)i_n(t)noise currentA[P1][P2]the noise source injected into the node
in2/Δf\overline{i_n^2}/\Delta fcurrent-noise power spectral density (single-sided)A²/Hz[P1]white: independent of frequency
Si(f)S_i(f)current-noise PSDA²/Hzallanother way of writing the same thing
Sϕ(f)S_\phi(f)phase PSD (single-sided)rad²/Hzallintegrating over ff gives σϕ2\sigma_\phi^2
L(Δf)\mathcal{L}(\Delta f)SSB phase noise (single-sideband phase noise)dBc/Hzall12Sϕ\approx\frac12 S_\phi
Δf, Δω\Delta f,\ \Delta\omegaoffset frequency (how far from the carrier)Hz, rad/sallΔω=2πΔf\Delta\omega=2\pi\Delta f
c0c_0DC Fourier coefficient of the ISF (DC value =c0/2=c_0/2)[P1]the key to 1/f upconversion
cn, θnc_n,\ \theta_namplitude / phase of the ISF's nn-th harmonic[P1]moves noise near nω0n\omega_0 onto the carrier
Γrms\Gamma_{rms}rms value of the ISF[P1][P2]sets the magnitude of the 1/f² phase noise
Γeff\Gamma_{eff}effective ISF (including cyclostationarity)[P1]Γeff=Γα\Gamma_{eff}=\Gamma\cdot\alpha
α(ω0t)\alpha(\omega_0 t)noise-modulating function (NMF): when the device is "leaking noise"[P1]0α10\le\alpha\le1, periodic
σt\sigma_trms timing jitters[P2]what SerDes cares about most
σϕ\sigma_\phirms phaseradallσt=σϕ/(2πf0)\sigma_t=\sigma_\phi/(2\pi f_0)
κ\kappaproportionality constant of ring accumulated jitters\sqrt{\mathrm{s}}[P2]σΔt=κΔt\sigma_{\Delta t}=\kappa\sqrt{\Delta t}
ω1/f\omega_{1/f}the device's 1/f-noise cornerrad/s[P1]note: ≠ the phase-noise 1/f³ corner
NNnumber of ring-oscillator stages[P2]ΓrmsN3/2\Gamma_{rms}\propto N^{-3/2}
QQtank quality factor[P1]appears in the Leeson comparison
η\etaproportionality constant in the ring frequency / FOM[P2]f0=1/(2NτD)f_0=1/(2N\tau_D)

The four "dialects" of jitter

Many people lump all jitter together, when in fact the measured quantities differ:

NameDefinitionIntuition
period jitterTkTT_k-T (a single period vs. nominal)how long/short this beat is
cycle-to-cycle jitterTk+1TkT_{k+1}-T_k (difference between two adjacent beats)how fast the beat changes from one to the next
accumulated / long-term jittertiming error between two edges separated by Δt\Delta t, σΔt=κΔt\sigma_{\Delta t}=\kappa\sqrt{\Delta t}an open-loop oscillator drifts further the longer it runs
random jitter (RJ)Gaussian, unbounded; described by σ\sigmawhat SerDes BER uses to estimate eye closure

See psd_phase_noise_jitter and serdes_clocking_connection for details.

Symbol correspondence across the papers (where unification is needed)

ConceptThis site's symbolPapers' notation / remarks
ISFΓ(ω0τ)\Gamma(\omega_0\tau)[P1][P2] use Γ\Gamma; some later literature uses hh or "ISF"
maximum chargeqmaxq_{max}[P1] qmax=CnodeVmaxq_{max}=C_{node}V_{max}; in rings it corresponds to the per-stage node charge
offset frequencyΔω\Delta\omega or Δf\Delta f[P1] mostly uses Δω\Delta\omega; datasheets use Δf\Delta f (Hz)
amplitude counterpart of phase sensitivity(see [P4]) APF Λ~\tilde\Lambda[P4] amplitude perturbation function; ideal LC fundamental Λ~1=τ0qmax0°\tilde\Lambda_1=\frac{\tau_0}{q_{max}}\angle0°, in quadrature with the ISF; τ0=2Q/ω0\tau_0=2Q/\omega_0
dimensioned ISFΓ~=Γ/qmax\tilde\Gamma=\Gamma/q_{max}[P3] Eq.(26): Hong uses the dimensioned version (rad/C); this site's core uses the dimensionless Γ\Gamma
phase equation (injection)generalized Adler[P3] Eq.(30),(33): dθdt=(ω0ωinj)+Ω(θ)\frac{d\theta}{dt}=(\omega_0-\omega_{inj})+\Omega(\theta), Ω=Γ~iinj\Omega=\langle\tilde\Gamma\,i_{inj}\rangle
PPV / adjoint / Floquetnot in these 5 PDFs; external literature (Demir et al.), see effective_isf

Notation trap: c0c_0 is the Fourier coefficient, while the DC value of the ISF is c0/2c_0/2 (see Eq.(12)). This factor is an easy source of error when computing the 1/f³ corner (Eq.(24)); later chapters will keep reminding you.