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

Chinese–English Glossary

See also: notation (rigorous symbols and units), math_identities (math toolbox), references (source codes [P1]–[P5], external [E1]–[E4])

The biggest friction when reading English papers alongside Chinese teaching pages is "one concept, two languages." This page pairs the site's terminology Chinese–English, each with one line of Chinese intuition (not a rigorous definition, just "get the feel first") plus the page it comes from. Click through for depth.

How to use this page: when you hit an unfamiliar term on some page, come back here, scan a one-liner, then decide whether to click through to the source page for detail. For rigorous symbols and units, cross-reference notation. Terms marked (external) mean they are not among the five downloaded PDFs, supplemented from standard literature.


Core ISF terminology

EnglishChineseOne-line intuitionSource page
ISF (Impulse Sensitivity Function)脈衝敏感度函數The oscillator's "phase-sensitivity weighting" to noise — tells you "kick it at this phase of the waveform, and this much phase results." Dimensionless, 2π2\pi-periodic.isf_definition
excess phase多餘相位 ϕ(t)\phi(t)The deviation beyond the ideal phase ω0t\omega_0 t; both phase noise and jitter live here.impulse_to_phase_shift
phase noise相位雜訊Random jitter of the oscillator signal's phase, appearing in the frequency domain as skirts on either side of the carrier.white_noise_to_phase_noise
timing jitter時間抖動The time-domain statement of the same thing: the random error of when an edge actually occurs relative to ideal.psd_phase_noise_jitter
phase perturbation相位擾動The component of noise that pushes the state point "tangent to the limit cycle"; no restoring force, it persists forever.phase_vs_amplitude_noise
amplitude perturbation振幅擾動The component of noise that pushes the state point "radially"; a restoring mechanism pulls it back, does not persist.phase_vs_amplitude_noise
limit cycle極限環The closed trajectory the oscillator circles in steady state in state-space; phase = how far along the cycle, amplitude = how far off the cycle.oscillator_phase

System and noise properties

EnglishChineseOne-line intuitionSource page
LTI (Linear Time-Invariant)線性非時變Impulse response depends only on "how long ago" tτt-\tau; the oscillator's response to noise is not LTI.math_identities
LTV (Linear Time-Variant)線性時變Impulse response also depends on "when you kick it" τ\tau — the same impulse has different effect at different phases, which is exactly the spirit of the ISF.convolution_derivation
cyclostationary noise週期穩態雜訊The noise strength itself varies periodically with the oscillation period (the device does not leak noise at every instant equally).effective_isf
noise-modulating function (NMF) α(ω0t)\alpha(\omega_0 t)雜訊調變函數A periodic function with 0α10\le\alpha\le1 describing "when the device is leaking noise"; multiplied by the ISF gives the effective ISF.effective_isf
white noise白噪Noise whose PSD is frequency-independent (autocorrelation is a delta); converted by the ISF integrator into 1/f21/f^2 phase noise.white_noise_to_phase_noise
flicker noise (1/f noise)閃爍雜訊/1/f1/f 雜訊Device noise with large low-frequency energy; only upconverted through the ISF's c0c_0 into close-in 1/f31/f^3 phase noise.flicker_noise_upconversion
upconversion上轉(頻率搬移)The ISF acts like a mixer, moving device noise at low frequency (or near nω0n\omega_0) up to near the carrier as phase noise.fourier_series_of_isf

Fourier and statistical quantities

EnglishChineseOne-line intuitionSource page
rms / effective ISFrms ISF Γrms\Gamma_{rms} / 有效 ISF Γeff\Gamma_{eff}Γrms\Gamma_{rms} is the rms of the ISF, directly setting the size of 1/f21/f^2 phase noise; Γeff=Γα\Gamma_{eff}=\Gamma\cdot\alpha folds in cyclostationarity.rms_isf
qmaxq_{max}最大電荷擺幅The nodal charge swing =CVmax=C\cdot V_{max}, used to normalize the ISF; larger means lower phase noise.impulse_to_phase_shift
c0c_0 (DC ISF coefficient)ISF 的 DC 係數The key controlling 1/f1/f upconversion; the ISF's DC value =c0/2=c_0/2. For a symmetric waveform c00c_0\approx0.symmetry
Fourier series / coefficients cn,θnc_n,\theta_n傅立葉級數/係數Decomposes the 2π2\pi-periodic ISF into DC plus harmonics; the nn-th harmonic moves noise near nω0n\omega_0.fourier_series_of_isf
PSD (Power Spectral Density)功率譜密度Noise power per unit bandwidth; SiS_i (A²/Hz), SϕS_\phi (rad²/Hz). Integrating over frequency gives variance.psd_phase_noise_jitter
SSB phase noise L(Δf)\mathcal{L}(\Delta f)單邊帶相位雜訊Phase-noise power relative to the carrier, in a single sideband, per Hz; 12Sϕ\approx\frac12 S_\phi.psd_phase_noise_jitter
dBc/Hz分貝(相對載波)每赫茲The unit of L\mathcal{L}: "c" = relative to carrier, "/Hz" = per unit bandwidth, taking 10log1010\log_{10}.math_identities

Oscillator types and advanced concepts

EnglishChineseOne-line intuitionSource page
ring oscillator環形振盪器NN inverter stages in a ring; ISF is concentrated at the transition, ΓrmsN3/2\Gamma_{rms}\propto N^{-3/2}.lab_03
LC oscillatorLC 振盪器Tank resonance, near-sinusoidal waveform; ideal ISF =sinθ=-\sin\theta.lab_02
accumulated jitter累積(長期)jitterAn open-loop oscillator has no absolute time reference, so its error grows like a random walk σΔt=κΔt\sigma_{\Delta t}=\kappa\sqrt{\Delta t}.lab_03
injection locking / pulling注入鎖定/拉扯An injected external signal "pulls" the oscillator's frequency toward it; the same ISF also governs this phenomenon (generalized Adler).paper_003_injection_locking_part1
APF (Amplitude Perturbation Function) Λ(ϕ)\Lambda(\phi)振幅擾動函數What the ISF is to phase, the APF is to amplitude; unit 1/A. Orthogonal (in quadrature) to the ISF in an ideal LC.paper_004_injection_locking_part2
Adler's equationAdler 方程The first-order differential equation describing the injection-locked phase difference (1946); the ISF generalizes it to arbitrary waveforms.paper_003_injection_locking_part1

Rigorous mathematical foundations (external literature)

EnglishChineseOne-line intuitionSource page
PPV (Perturbation Projection Vector)擾動投影向量 (external)The rigorous generalization of the ISF: the vector projecting a perturbation onto the phase direction; corresponds to the theory of Demir et al. 2000. Not among the five source PDFs.effective_isf
adjoint method伴隨法 (external)A numerical method for computing the PPV/ISF from the periodic steady-state solution (solving the adjoint system). Not among the five source PDFs.effective_isf
Floquet theoryFloquet 理論 (external)Stability theory for linear systems with periodic coefficients; gives the mathematical foundation of the PPV. Not among the five source PDFs.effective_isf
Wiener–Khinchin theorem維納–辛欽定理 (external)The PSD is the Fourier transform of the autocorrelation function; connects time-domain and frequency-domain noise. A standard stochastic-process theorem.math_identities
Leeson modelLeeson 模型 (external)The 1966 empirical phase-noise model; the ISF theory subsumes it as a special case. Not among the five source PDFs.references

One-line reminders (the pairs most often confused)

  • phase noise vs timing jitter: the same thing, the former in the frequency domain (dBc/Hz), the latter in the time domain (fs); interconvert via σt=σϕ/(2πf0)\sigma_t=\sigma_\phi/(2\pi f_0).
  • phase perturbation vs amplitude perturbation: phase stays, amplitude gets pulled back — which is why phase noise is the star of the show.
  • LTI vs LTV: the difference is whether the impulse response depends on the absolute time τ\tau; the oscillator is LTV.
  • c0c_0 vs the 1/f31/f^3 corner: c0c_0 determines whether flicker upconverts at all; the 1/f31/f^3 corner =ω1/f(c0/c1)2=\omega_{1/f}(c_0/c_1)^2, is not equal to the device's ω1/f\omega_{1/f}.
  • device 1/f1/f corner ω1/f\omega_{1/f} vs phase-noise 1/f31/f^3 corner Δω1/f3\Delta\omega_{1/f^3}: two different things, do not confuse them (see flicker_noise_upconversion).

Further reading