fracpll

fracpll is a Python package for designing and checking a fractional-N frequency synthesizer: the circuit that turns one clean reference frequency into a precise, adjustable output frequency (for example 50 MHz in, 2.005 GHz out, a ratio of 40.1). It works from the numbers you have measured or designed -- your oscillator's tuning curve, your noise measurements, your pump current, your filter parts -- and answers the questions every design has to answer:

• Is the loop stable, and with how much safety margin?
• How much noise does the output have, and how much timing jitter does that give?
• Will the loop lock from a cold start, how fast, and how large a steady timing offset does leakage leave once it is locked?
• What unwanted tones (spurs) does the fractional divider create?
• How long must the measurement instrument average before the jitter number is trustworthy?

It also reads your measured noise traces and tuning curves straight from text files (CSV and similar).

The main results are checked by automated tests against independent calculations (see How the results are checked). One exception is stated there: the lock settling time is an estimate. When a question falls outside what a model can answer reliably, the package stops with an error message that says why and what to use instead, rather than returning a number that looks fine but is not.

Contents

• A short guide to the words used here
• Install
• Three ways to model the loop
• Examples (each with the output it prints)
• What is in the package
• When it refuses, and why
• How the results are checked
• Corrections in earlier versions
• Limits
• Where it comes from
• Citing, support and license

A short guide to the words used here

A synthesizer of this kind is a feedback loop. Going around the loop:

• Reference -- a clean, fixed input frequency (f_ref), for example from a crystal oscillator.
• Oscillator (VCO) -- makes the output. Its frequency is set by a control voltage v_c. Kvco is how many hertz the frequency moves per volt. It can be negative (frequency falls as voltage rises). A loop built around such an oscillator also reverses the direction of its pump current, and the two sign flips cancel. So: fit_tuning accepts a falling curve; sampled_loop_map, sampled_stability, simulate_sampled and simulate_pll take the negative Kvco together with pump_polarity=-1; and the averaged-model functions (open_loop, stability, continuous_closed_loop_poles, lock_transient) need Kvco as a positive number and refuse a negative one.
• Tuning curve -- the measured relation between control voltage and oscillator frequency.
• Divider -- divides the output frequency by N so it can be compared with the reference. In a fractional-N synthesizer the divider switches among a few nearby whole numbers (from N-3 to N+4 for a third-order MASH) so that N is a fraction on average (for example 40.1). The switching pattern comes from a delta-sigma modulator; the kind used here is called MASH, and its order (1, 2 or 3) says how strongly it pushes its switching noise to high frequencies.
• Phase detector and charge pump (PFD/CP) -- each reference cycle they compare the timing of the reference edge with the divider edge, and push a short burst of current (the pump current, Icp) into or out of the loop filter. The burst lasts as long as the timing gap (plus a short reset delay, if the circuit has one, during which both the UP and DN currents flow). The timing gap is called the pulse width here.
• Loop filter -- a few resistors and capacitors that turn those current bursts into a smooth control voltage.
• Loop bandwidth -- roughly, how fast the loop reacts. Below it the loop follows the reference; above it the oscillator runs on its own. Phase margin, in degrees, measures how far the loop is from oscillating: more is safer, and zero or less means it is unstable. Gain margin, in dB, says how much the loop gain (for example the pump current) could grow before the loop becomes unstable.
• Phase noise -- small random wobbles in the output timing, given as a spectrum over offset frequency. It is quoted in dBc/Hz (decibels relative to the output, per hertz of bandwidth). Inside the package the same noise is held as S_phi: the noise power per hertz, counted over positive offsets only ("one-sided"), in rad^2/Hz. The two are related by the standard rule dBc/Hz = 10 log10(S_phi/2) (IEEE Std 1139), and dbc_to_psd / psd_to_dbc convert. Jitter is the same wobble expressed as a time spread in seconds.
• Spur -- an unwanted pure tone next to the output, quoted in dBc.
• Leakage -- a small current that drains the loop filter. The loop cancels it by holding a small permanent timing offset.

Install

pip install fracpll

It needs Python 3.9 or newer, NumPy 1.22 or newer and SciPy 1.8 or newer, and nothing else. Units are SI: hertz, volts, amperes, ohms, farads, seconds. Phases come on three scales:

• Reference radians, where 2 pi is one reference period: phase errors at the phase detector (lock_transient's phi_e and phi_static, pfd_static_offset's phase_ref_rad).
• Oscillator radians, where 2 pi is one oscillator period (N times more radians for the same time shift): the noise spectra, spur tones and SimResult.phase_rad().
• Oscillator cycles: names containing cycles or psi.

Three ways to model the loop

The package offers three models of the same loop. They trade speed for detail, and each one is checked against the others where they overlap.

Rule of thumb: start with the averaged model. If it refuses because the loop is too fast, use the per-cycle model. If you need behaviour far from lock or circuit non-idealities, use the edge-by-edge simulator.

Examples

Each example below runs as written, and the output shown is what it printed with fracpll 0.4.0. The circuit values are illustrative design values, not a recommended design.

1. Is the loop stable?

from fracpll import loop_filter_impedance, stability

# Loop filter: 100 pF to ground, in parallel with 4.7 kOhm in series with 1.5 nF.
zf = lambda w: loop_filter_impedance(w, c_shunt=100e-12,
                                     branches=[(4.7e3, 1.5e-9)])

rep = stability(icp=100e-6,           # charge-pump current: 100 uA
                kvco_hz_per_v=20e6,   # oscillator gain: 20 MHz per volt
                n_div=40.0,           # divide ratio
                zfilter=zf,
                f_ref_hz=50e6)        # reference: 50 MHz
print(f"loop bandwidth {rep['f_crossover_hz']:.0f} Hz, "
      f"phase margin {rep['phase_margin_deg']:.1f} degrees")

loop bandwidth 40014 Hz, phase margin 54.2 degrees

A loop filter is described by one capacitor to ground (c_shunt) and any number of resistor-capacitor pairs in parallel with it (branches, each (R, C) in series).

2. Output noise and jitter from your measured parts

import numpy as np
from fracpll import (loop_filter_impedance, open_loop, NoiseSpec,
                     white_floor, dsm_phase_psd, synthesizer_psd,
                     rms_jitter, averages_for_jitter)

zf = lambda w: loop_filter_impedance(w, c_shunt=100e-12,
                                     branches=[(4.7e3, 1.5e-9)])
f = np.geomspace(1e4, 1e7, 800)                  # offsets 10 kHz .. 10 MHz
lg = open_loop(2 * np.pi * f, 100e-6, 20e6, 40.0, zf)

# Your measured free-running oscillator noise (dBc/Hz at each offset).
# The numbers here are placeholders: put yours in, and say in
# `reference` where they came from (instrument and date, or a citation).
vco = NoiseSpec((1e4, 1e5, 1e6, 1e7), (-65.0, -92.0, -115.0, -135.0),
                reference="illustrative VCO noise points, not a measurement")
pfd = white_floor(-102.0, "illustrative PFD+CP floor, not a measurement")

out = synthesizer_psd(f, lg, 40.0,
                      s_vco=vco.psd(f),
                      s_inband=pfd.psd(f),
                      s_dsm=dsm_phase_psd(f, 50e6, 3))   # 3rd-order delta-sigma
jit = rms_jitter(f, out["s_out"], 2.0e9)                  # 2 GHz output
print(f"RMS jitter (10 kHz to 10 MHz): {jit * 1e12:.2f} ps")

n_avg, achieved = averages_for_jitter(0.01, f, out["s_out"])
print(f"averages for a 1 % error bar: {n_avg} (gives {achieved * 100:.3f} %)")

RMS jitter (10 kHz to 10 MHz): 10.82 ps
averages for a 1 % error bar: 9 (gives 0.993 %)

The output noise is built from three sources: the oscillator's own noise (the loop suppresses it at low offsets), the noise floor of the phase detector and charge pump (the loop passes it at low offsets, multiplied by N squared), and the delta-sigma divider's switching noise (the loop passes it at low offsets and filters it at high ones). out also holds each of the three separately.

NoiseSpec joins your measured points with straight lines on a log-log plot and refuses offsets outside the measured range. The measurement plan in the last two lines treats each point of the offset grid f as one analyzer reading averaged n times, with independent readings.

3. Will it lock, and how fast?

from fracpll import fit_tuning, lock_transient

# Your measured tuning curve: control voltage (V) -> frequency (Hz).
curve = fit_tuning(vc=[0.0, 1.0, 2.0, 3.0],
                   f_hz=[4.8e9, 5.2e9, 5.6e9, 6.0e9],
                   reference="illustrative tuning points, not a measurement")

res = lock_transient(curve, n_div=100.0, f_ref_hz=50e6, icp=200e-6,
                     c_shunt=50e-12, branches=[(4.7e3, 1.5e-9)],
                     i_leak=2e-6)                  # 2 uA leakage
print("locked:", res["locked"])
print(f"settles in {res['t_settle'] * 1e6:.1f} us")
print(f"phase error left by the leakage: {res['phi_static']:.4f} rad")

locked: True
settles in 29.0 us
phase error left by the leakage: 0.0628 rad

The phase error is at the phase detector, in reference radians (2 pi is one reference period), so 0.0628 rad is 1 % of a 20 ns reference period, or 0.2 ns.

The run starts from the bottom of the measured voltage range and uses the averaged model, which is written for a positive Kvco (for a falling tuning curve it refuses and points to simulate_pll). It replaces the phase detector's exact behaviour with a smooth curve (a tanh), so the settling time is an estimate; simulate_pll gives the edge-accurate transient. The settling time is the last moment the phase error is more than settle_tol_rad (default 0.05 rad) away from its final value. Since 0.4.0 it is found on the solver's continuous solution; before, it was rounded up to the next of 2000 output samples, and this example printed 31.8 us.

The leftover phase error is a closed-form value, 2 pi atanh(I_leak / Icp) here (it also includes pump mismatch when you give one), and the test suite checks that the simulated transient settles onto it.

4. Edge by edge: leakage, reset delay and pump mismatch

from fracpll import LinearVCO, simulate_pll, pfd_static_offset

vco = LinearVCO(f0_hz=4.8e9, kvco_hz_per_v=400e6,
                reference="illustrative design values, not a datasheet")

# 2 uA leakage, 100 ps reset delay, DN current 5 % weaker than UP.
run = simulate_pll(vco, n_int=100, f_ref_hz=50e6, icp=200e-6,
                   c_shunt=50e-12, branches=[(4.7e3, 1.5e-9)],
                   n_cycles=6000, i_leak=2e-6, i_dn=190e-6,
                   t_reset=100e-12)
print(f"simulated timing offset at lock: {run.time_error()[-1] * 1e12:.6f} ps")

exact = pfd_static_offset(50e6, 200e-6, i_dn=190e-6, i_leak=2e-6,
                          t_reset=100e-12)
print(f"exact charge-balance answer:     {exact['dt_s'] * 1e12:.6f} ps")
print("cycle slips:", run.slips)

simulated timing offset at lock: 195.000000 ps
exact charge-balance answer:     195.000000 ps
cycle slips: 0

The timing offset is the divider edge minus the reference edge. Once locked, the charge the pump adds each cycle must exactly replace what leakage and mismatch remove; pfd_static_offset solves that balance directly, and the simulator reaches the same value on its own.

5. A fast loop the averaged model cannot judge

from fracpll import loop_filter_impedance, stability, sampled_stability

loop = dict(icp=0.5e-3, kvco_hz_per_v=400e6, n_div=10, f_ref_hz=50e6)
zf = lambda w: loop_filter_impedance(w, 2e-12, [(20e3, 200e-12)])

try:
    stability(zfilter=zf, **loop)
except ValueError as err:
    print("averaged model:", err)

st = sampled_stability(c_shunt=2e-12, branches=[(20e3, 200e-12)], **loop)
print("per-cycle model: stable =", st["stable"],
      f"(growth factor per cycle {st['spectral_radius']:.5f}; below 1 means stable)")

averaged model: crossover 1.566e+07 Hz exceeds f_ref/10 = 5e+06 Hz: the averaged continuous-time model is no longer trustworthy this close to the reference (Gardner, IEEE Trans. Commun. 28, 1849 (1980)); this averaged model refuses here. Use fracpll.sampled_stability for the exact sampled-data answer at any bandwidth, or fracpll.simulate_pll for the edge-level loop
per-cycle model: stable = True (growth factor per cycle 0.99501; below 1 means stable)

The averaged model treats the current bursts as a smooth current. That is only accurate when the loop is much slower than the reference, so it refuses here. The per-cycle model steps the loop once per reference cycle exactly and answers at any speed. "Stable" is not the same as "well designed": example 8 shows that this loop has almost no margin.

6. Spurs from a first-order divider

import numpy as np
from fracpll import (mash_line_spectrum, closed_loop_lines,
                     loop_filter_impedance, open_loop)

# A first-order divider with fraction 3/64 repeats every 64 cycles, so its
# error is a set of pure tones (spurs) at multiples of 50 MHz / 64.
lines = mash_line_spectrum(num=3, den=64, m=1, f_ref_hz=50e6)

zf = lambda w: loop_filter_impedance(w, 100e-12, [(4.7e3, 1.5e-9)])
lg = open_loop(2 * np.pi * lines["f_hz"], 100e-6, 20e6, 40.0, zf)
spurs = closed_loop_lines(lines["f_hz"], lines["line_rad2"], lg)

for f, dbc in zip(lines["f_hz"][:3], spurs["sideband_dbc"][:3]):
    print(f"spur at {f / 1e6:.5f} MHz: {dbc:.2f} dBc")

spur at 0.78125 MHz: -59.19 dBc
spur at 1.56250 MHz: -70.97 dBc
spur at 2.34375 MHz: -52.82 dBc

A divider pattern of any MASH order repeats exactly after a fixed number of cycles, so its error is a set of exact tones. mash_line_spectrum finds that repeat length and every tone (for repeat lengths up to 2^22 cycles by default; longer ones are refused). closed_loop_lines then passes them through the loop to the output. A dBc value is only meaningful for a small tone, so it is given only where the tone's phase swing is 0.2 rad or less and is NaN elsewhere.

7. Why the noise near the loop bandwidth is higher than a linear model says

import numpy as np
from scipy import signal
from fracpll import simulate_sampled, simulate_pll, LinearVCO

design = dict(icp=100e-6, f_ref_hz=50e6, c_shunt=100e-12,
              branches=[(4.7e3, 1.5e-9)])
frac = dict(n_int=40, num=104857, den=2**20, mash_order=3,
            n_cycles=(1 << 16) + 2048)
n_mean = 40 + 104857 / 2**20          # the average divide ratio

# Fast per-cycle model, first order (linear) and second order.
lin = simulate_sampled(kvco_hz_per_v=20e6, n_div=n_mean, order=1, **design, **frac)
full = simulate_sampled(kvco_hz_per_v=20e6, n_div=n_mean, order=2, **design, **frac)

# The same loop, edge by edge.
vco = LinearVCO(f0_hz=1.995e9, kvco_hz_per_v=20e6,
                reference="design value for this example")
edge = simulate_pll(vco, **design, **frac)

def level_db(psi_cycles, lo=2e4, hi=5e4):
    """Average phase noise between lo and hi (dB rad^2/Hz)."""
    f, p = signal.welch(2 * np.pi * psi_cycles, fs=50e6,
                        nperseg=1 << 14, detrend="linear")
    return 10 * np.log10(p[(f >= lo) & (f < hi)].mean())

keep = slice(8192, None)              # drop the start-up
for name, psi in [("edge by edge", edge.psi_ref),
                  ("per cycle, order 1", lin["psi"]),
                  ("per cycle, order 2", full["psi"])]:
    print(f"{name:20s} {level_db(psi[keep]):7.1f} dB  (20-50 kHz)")

edge by edge          -145.3 dB  (20-50 kHz)
per cycle, order 1    -160.3 dB  (20-50 kHz)
per cycle, order 2    -145.3 dB  (20-50 kHz)

With a delta-sigma divider, the edge-by-edge simulator shows more noise near the loop bandwidth than a linear model predicts (15 dB more in this example), even with perfectly matched pumps. The cause is the width of the current bursts. A burst of width tau delivers its charge centred tau/2 after the reference edge, not at the edge. The resulting error grows with tau squared, and because the delta-sigma divider makes tau jump around from cycle to cycle, squaring it moves some of the divider's high-frequency noise down to low frequencies, where the loop does not filter it. simulate_sampled(order=2) includes this effect with no fitted numbers and matches the edge-by-edge result; order=1 is the linear model. (Welch and signal above come from SciPy and are used only to measure the spectra.)

8. Phase and gain margin of a fast loop

from fracpll import sampled_margins

loop = dict(icp=0.5e-3, kvco_hz_per_v=400e6, n_div=10, f_ref_hz=50e6)
m = sampled_margins(c_shunt=2e-12, branches=[(20e3, 200e-12)], **loop)
print(f"loop bandwidth {m['f_crossover_hz'] / 1e6:.2f} MHz, "
      f"phase margin {m['phase_margin_deg']:.2f} degrees")
print(f"gain margin {m['gain_margin_db']:.2f} dB "
      f"(at {m['f_phase_crossover_hz'] / 1e6:.1f} MHz), stable = {m['stable']}")

slow = sampled_margins(icp=100e-6, kvco_hz_per_v=20e6, n_div=40.0,
                       f_ref_hz=50e6, c_shunt=100e-12,
                       branches=[(4.7e3, 1.5e-9)])
print(f"example 1 loop: {slow['f_crossover_hz']:.0f} Hz, "
      f"{slow['phase_margin_deg']:.1f} degrees, "
      f"gain margin {slow['gain_margin_db']:.1f} dB")

loop bandwidth 22.68 MHz, phase margin 2.06 degrees
gain margin 0.18 dB (at 25.0 MHz), stable = True
example 1 loop: 40015 Hz, 54.2 degrees, gain margin 86.0 dB

sampled_margins works from the exact per-cycle loop gain (sampled_open_loop), so it answers at any loop speed. The fast loop of example 5 is stable, but only just: 2 degrees of phase margin, and a pump current only 2 % (0.18 dB) higher would make it oscillate at half the reference frequency. For the slow loop of example 1 it agrees with the averaged model (40014 Hz and 54.2 degrees in example 1). A sampled loop also has a finite gain margin, which the averaged model cannot give: its phase always returns to -180 degrees at half the reference frequency.

9. Measured noise from a file, integrated exactly

import numpy as np
from fracpll import read_noise_csv, rms_jitter, dbc_to_psd

# A small file of the kind an analyzer or a bench script saves:
# a header line, then one "offset, dBc/Hz" row per point.
with open("vco_noise.csv", "w") as fh:
    fh.write("Offset (Hz),Phase noise (dBc/Hz)\n"
             "1e4,-65\n1e5,-92\n1e6,-115\n1e7,-135\n")

vco = read_noise_csv("vco_noise.csv",
                     reference="illustrative decade points, not a measurement")
var = vco.phase_variance(1e4, 1e7)          # rad^2, exact between points
print(f"jitter of these points at 2 GHz: "
      f"{np.sqrt(var) / (2 * np.pi * 2e9) * 1e12:.3f} ps")

f = np.array(vco.f_offset_hz)
s = dbc_to_psd(np.array(vco.dbc_per_hz))
print(f"same four points, log-log rule: "
      f"{rms_jitter(f, s, 2e9, method='loglog') * 1e12:.3f} ps")
print(f"same four points, trapezoid:    {rms_jitter(f, s, 2e9) * 1e12:.3f} ps")

jitter of these points at 2 GHz: 4.869 ps
same four points, log-log rule: 4.869 ps
same four points, trapezoid:    13.579 ps

read_noise_csv skips the header line, reads the rows and builds a NoiseSpec (the reference is still required). phase_variance integrates the noise exactly as the spec draws it: straight lines between the points on a log-log plot. Given only a few points far apart, the ordinary trapezoid rule (straight lines on linear axes, the default of rms_jitter) overstates the jitter badly, here by a factor of 2.8; method="loglog" avoids that. On a dense grid the two rules agree: on the 800 points of example 2 they differ by about 1 part in 10^5. read_tuning_csv does the same for a (control voltage, frequency) file and returns a fitted tuning curve.

What is in the package

Loop and stability (averaged model)

• loop_filter_impedance(w, c_shunt, branches) -- the impedance of a passive loop filter: one capacitor to ground plus any number of series resistor-capacitor branches. second_order_impedance is the textbook two-capacitor, one-resistor formula, kept as an independent check.
• open_loop(w, icp, kvco_hz_per_v, n_div, zfilter) -- the loop gain L = Icp * Kvco * Z / (j w N); error_transfer and lowpass_transfer give 1/(1+L) and L/(1+L).
• stability(...) -- loop bandwidth and phase margin.

Delta-sigma divider

• mash_sequence(num, den, m, n_steps) -- the exact divider pattern of an order-m MASH, computed with whole-number arithmetic, so the average fraction is exactly num/den.
• dsm_phase_psd(f_hz, f_ref_hz, m) -- the smooth noise spectrum of that pattern (orders 2 and 3; order 1 makes tones, not smooth noise, and is refused with a pointer to the next item).
• mash_period, mash_line_spectrum -- the exact repeat length and exact tones of any order-1, 2 or 3 pattern.
• MASH_RANGE -- the smallest and largest divider step each order can produce.

Noise and jitter

• NoiseSpec, white_floor -- your measured noise, each with a required reference saying where it came from.
• synthesizer_psd -- the output noise from the three sources.
• closed_loop_lines -- divider tones as output spurs.
• rms_jitter -- jitter in seconds from a noise spectrum; method="loglog" integrates exactly between points joined by straight lines on a log-log plot (use it for a few measured points).
• NoiseSpec.phase_variance(f_lo, f_hi) -- the exact integrated phase noise (rad^2) of a measured spec, with no grid.
• dbc_to_psd, psd_to_dbc -- conversions between dBc/Hz and rad^2/Hz, using dBc/Hz = 10 log10(S_phi/2).

Tuning curves and lock

• fit_tuning, TuningCurve, TuningFamily -- a smooth, never-folding curve through your measured (voltage, frequency) points, its slope (Kvco), and straight-line blending between curves measured at different temperatures. Negative Kvco is supported.
• lock_transient, static_offset -- lock-in from a cold start on the measured curve, and the phase error that leakage and mismatch leave behind.

Reading measured data

• read_noise_csv, read_tuning_csv -- a NoiseSpec or a fitted tuning curve from a text file (comma, semicolon, tab or space separated; header lines skipped; choose the columns and the frequency unit). Text inside the data, repeated or unsorted points and missing values are refused with the line number.

Measurement planning

• jitter_relative_sigma, averages_for_jitter -- how uncertain a measured jitter value is after n averages, and how many averages a target uncertainty needs.

Per-cycle model (any loop bandwidth)

• sampled_loop_map, sampled_stability -- the exact one-cycle step of the loop for small deviations from lock, and stability from it.
• sampled_open_loop, sampled_margins -- the exact per-cycle loop gain, and the phase margin and gain margin read from it, at any loop bandwidth.
• continuous_closed_loop_poles -- the averaged model's poles, for comparison.
• simulate_sampled(..., order=1 or 2) -- a fast cycle-by-cycle noise run; order=2 adds the pulse-width effect of example 7.
• pulse_doublet_vector -- the building block of that effect.

Edge-by-edge simulator

• simulate_pll(vco, ...) with LinearVCO or a measured TuningCurve -- supports a phase detector reset delay, a dead zone, unequal UP and DN currents, leakage, negative Kvco, fractional division, optional reference timing noise, and counts skipped cycles (cycle slips).
• SimResult -- the recorded edge times, control voltage and phase; time_error(), nearest_edge_error() and phase_rad() read them.
• pfd_static_offset -- the exact locked timing offset from charge balance.

Each function's docstring (help(fracpll.stability), for example) gives its inputs, units and conventions.

When it refuses, and why

fracpll raises an error instead of guessing when:

• the averaged model's loop bandwidth passes f_ref/10, where that model stops being accurate (Gardner, IEEE Trans. Commun. 28, 1849 (1980)); the message points to the per-cycle model;
• the loop gain does not fall through 1 within the scanned band (by default f_ref/10^6 to f_ref/2), or the phase margin is zero or negative (stability); for sampled_margins, when the loop gain is still 1 or more at f_ref/2 (such a loop is always unstable);
• a negative Kvco is given to an averaged-model function (pass its size; the sign belongs in pump_polarity for the other models);
• smooth noise is asked of a first-order divider (it makes tones; use mash_line_spectrum);
• a noise value or tuning-curve value is asked outside the measured range;
• a measured tuning curve folds back (the error names the voltage where it happens);
• the lock target frequency, or the starting control voltage of lock_transient, is outside the oscillator's measured range;
• leakage or mismatch is too large for the pump to cancel;
• the phase detector has no locked state (for example inside a dead zone with nothing to push it out);
• a measured value is given without saying where it came from;
• a data file has text inside its data, repeated or unsorted points, or missing values (the message gives the line number).

How the results are checked

90 automated tests run on every change, on Python 3.9 to 3.14, and once more on Python 3.9 with the oldest NumPy (1.22.0) and SciPy (1.8.0) the package allows. Each numerical check compares the package with something independent of it: an exact formula, a second calculation done a different way, or a published result; none compares against a number stored from an earlier run. The rest check that the refusals fire, plus one check of the version number and the list of exported names. The lock settling time is checked against an exact solution only in the small-signal limit (below); for a large start-up transient such as example 3 it remains the tanh model's estimate. The main checks:

Averaged model

• The general filter formula equals the textbook second-order formula to 1 part in 10^12.
• The reported bandwidth and phase margin agree with a direct search over 400 000 frequencies.
• The divider pattern's average fraction is checked with exact fractions.
• The smooth delta-sigma noise formula agrees within 15 % with the measured spectrum of the actual divider pattern.
• The jitter calculation matches exact results for flat and falling-slope noise. The log-log rule matches the exact integral of a power law, for slopes from -3 to +1.5 including -1 (a logarithm), to 1 part in 10^12, and a dense-grid integration of a measured spec to 1 part in 10^8.
• The measurement-planning formula agrees within 6 % with 4000 simulated measurements.
• The lock transient settles onto its closed-form phase error to 10^-6 rad, with the oscillator on N * f_ref to 1 part in 10^9.
• For a small phase step from lock on a straight-line tuning curve, where the averaged model is linear, the transient matches the matrix-exponential solution of that linear system to 10^-5 of the step, and the settling time to 3 parts in 10^5. The settling time no longer changes with the number of output samples (to 1 part in 10^9).
• The dBc/Hz conversion reproduces the printed form of the delta-sigma noise formula (eq. 3.7 of W. Rhee's thesis, University of Illinois, 2001), and spur dBc values use the same rule.

Reading data files

• Numbers written to a file with 17 significant digits read back bit for bit, with any of the four separators, a header, a byte-order mark, a chosen column or a unit scale; a file of an exact power law integrates to the closed form to 1 part in 10^12; each refusal is checked to name the right line.

Divider tones

• For a first-order divider, the exact tones match a known closed form to 1 part in 10^12, and they add up to the total variance.
• For long patterns, the exact tones agree with the smooth formula within 10 % in every band.

Edge-by-edge simulator

• The locked timing offset matches the exact charge balance to 1 part in 10^6, in five cases covering leakage, mismatch, reset delay and dead zone.
• After a small nudge, it follows the exact per-cycle model cycle by cycle, to 1 part in 10^5.
• With the pump current 10 % below the stability limit that the per-cycle model predicts, the simulated loop settles; 10 % above, it oscillates with growing size. The averaged model refuses this case.
• The measured-curve path matches the exact straight-line path to 10^-18 s.
• A fractional lock keeps the average ratio N + num/den, drifting by less than 10^-6 cycles per reference cycle.
• It locks after skipping cycles, and it works with negative Kvco.
• Its delta-sigma noise at high offsets matches the averaged formula (ratio between 0.85 and 1.2), and would be off by N squared (1600) with the error that version 0.1.0 had (the test asserts more than 1000; see below).
• Its first-order spurs match the exact tones through the loop within 0.5 dB.
• Unequal UP and DN currents raise the low-offset noise by more than 20 dB, and a small deliberate offset current lowers it by more than 6 dB. This known effect is checked here qualitatively (T.-H. Lin, C.-L. Ti and Y.-H. Liu, IEEE Trans. Circuits Syst. I 56, 877 (2009)).

Per-cycle model and pulse-width effect

• The per-cycle loop gain equals the averaged loop gain summed over all its aliases (shifts by multiples of f_ref, an exact identity) to 1 part in 10^10, for the slow loop of example 1 and the fast loop of example 5, and, for a filter that is a single capacitor, a closed form to 1 part in 10^9; for that filter the phase margin and the gain margin are both 0 whatever the scan grid.

• The margins are checked by eigenvalues: shifting the phase of the loop gain by the phase margin, or scaling it by the gain margin, puts a pole of the per-cycle map on the unit circle at the matching frequency (to 10^-8). In the fast loop, the pump current times the gain margin equals the current at which the loop becomes unstable (found separately from the poles) to 1 part in 10^9. For the slow loop the margins agree with the averaged model (bandwidth to 10^-4, phase margin to 0.01 degrees).

• Driven by a sine wave, or by the exact tones of a first-order divider in a fast loop the averaged model refuses, the per-cycle simulation gives the output that the per-cycle loop gain predicts (to 1 part in 10^9 and 10^6 respectively).

• For a slow loop, the per-cycle and averaged models predict the same settling behaviour: their poles match after the conversion z = exp(s T) with T = 1/f_ref, to 0.1 % of each pole's distance from 1.

• simulate_sampled(order=2) matches the edge-by-edge simulator, cycle by cycle, more than 1000 times more closely than the linear model. For two values of the capacitor to ground, c_shunt (100 pF and 400 pF), its pulse widths also agree to 10^-15 s and its low-offset noise within 0.5 dB. With negative Kvco, the 1000-times match is checked.

• order=1 equals the linear per-cycle model to 1 part in 10^12.

• Making the pulses half as wide in the same loop lowers the effect by about 6 dB (the test allows 4.5 to 7.5 dB), in both the simulator and order=2.

Corrections in earlier versions

0.2.0 fixed a noise error in 0.1.0. Version 0.1.0 multiplied the delta-sigma divider noise by N squared in synthesizer_psd. That was wrong. The divider noise formula already describes the error at the oscillator, so it reaches the output through the loop alone, with no factor of N squared. This agrees with eq. (3.7) of W. Rhee's thesis (University of Illinois, 2001) and with the edge-by-edge simulator. The error overstated delta-sigma noise by N squared (32 dB at N = 40). The phase detector and charge pump floor does keep its N squared. If you used 0.1.0 with a delta-sigma term, please re-run that analysis.

0.3.0 explained an effect that 0.2.0 only reported. 0.2.0 noted extra low-offset noise in the edge-by-edge simulator without a cause. 0.3.0 identifies the cause (example 7).

0.3.1 fixed three problems found in a review of 0.3.0.

• dbc_to_psd turned dBc/Hz into rad^2/Hz without the standard factor of 2, while the delta-sigma formula and the spur dBc values used it. Measured oscillator noise and noise floors were therefore counted 3 dB too low next to the delta-sigma noise, and jitter computed from them came out too small by a factor of about 1.41 (example 2 printed 7.65 ps before the fix and 10.82 ps after). If you converted measured dBc/Hz values with 0.3.0 or earlier, please re-run those results.
• The averaged-model functions accepted a negative Kvco and returned results for a loop with positive feedback (for example a phase margin above 180 degrees), and lock_transient returned an unlocked run for a falling tuning curve. Both are now refused with a pointer to the right tool.
• rms_jitter used a NumPy function that only exists from NumPy 2.0, although the package allows NumPy 1.22. It now works on both, and NumPy 1.22.0 with SciPy 1.8.0 is tested.

0.4.0 fixed the lock settling time and tightened input checks.

• lock_transient rounded its settling time up to the next output sample (by default 2000 samples over about 32 ms, so 15.9 us steps). Example 3 printed 31.8 us, exactly two samples; the settling time is 29.0 us. It is now found on the solver's continuous solution, whatever n_eval is. The transient itself (t, phi_e, vc, locked) is unchanged, bit for bit.
• lock_transient accepted a starting control voltage outside the measured tuning curve (holding the oscillator at the curve's edge while the filter voltage came back into range) and a negative capacitor (returning a meaningless run); pfd_static_offset returned NaN for a NaN input and raised a division-by-zero error for f_ref_hz = 0; stability scanned a reversed band and gave a misleading message. All are now refused with a clear message.

The full history is in CHANGELOG.md.

Limits

• The averaged model is valid only for loops much slower than the reference. It says so and refuses beyond f_ref/10; use sampled_margins for stability margins of faster loops.
• lock_transient replaces the phase detector with a smooth tanh curve, so for a large start-up transient its settling time is only an estimate of the real loop's; the tests check it against an exact solution only in the small-signal limit. Use simulate_pll for an edge-accurate transient.
• The per-cycle model covers small deviations from lock, with equal UP and DN currents, no leakage, no dead zone and a constant Kvco. order=2 keeps effects up to the square of the pulse width and drops smaller ones (cube and higher); in the tested designs these are 60 dB or more below the second-order effect. sampled_open_loop and sampled_margins use the linear (first-order) per-cycle model; the pulse-width effect of order=2 is not part of the margins.
• In the edge-by-edge simulator, the pump switches instantly apart from the stated delays. The dead zone is modelled as a turn-on delay, not as transistor physics. The only noise the simulator itself injects is the delta-sigma divider's and any reference timing noise you supply; other noise sources are added in the frequency domain with synthesizer_psd.
• The smooth delta-sigma noise formula is an approximation: it ignores that the divider pattern repeats exactly. The tests confirm it within 10 % for long repeat lengths; for short ones, use mash_line_spectrum for the exact tones.
• rms_jitter keeps the trapezoid rule as its default, so existing results do not change; on a few widely spaced points it overstates a falling spectrum, and method="loglog" is the right choice there. The measurement plan (jitter_relative_sigma, averages_for_jitter) uses the trapezoid weights, which suits a dense analyzer trace.
• The file readers do not know any instrument's file format; you choose the columns and the frequency unit. A decimal comma (1,5) is not supported.
• No transistor models, device physics or foundry data ship with the package. Your measured tuning curves and noise carry the technology, each with a required reference field.

Where it comes from

The methods were first written for a study of a single-chip GaN-on-SOI transistor-varactor PLL, where the oscillator has negative Kvco and its tuning curve comes from measurements rather than a formula. The parts that apply to any technology that uses a charge-pump loop (CMOS, SiGe, GaN, or board level) are here. The study's machine-learning and optimisation parts stay with the study, and its foundry design-kit files are licensed material that is not included.

Citing, support and license

If fracpll helps your work, please cite it with the concept DOI 10.5281/zenodo.22829473, which always points to the latest release; each release also has its own DOI on Zenodo. CITATION.cff has the details.

Written and maintained by Tanvir Mahmud Mahim (Department of Electrical and Electronic Engineering, BRAC University), who reviews every change and decides on scope and releases. Questions and bug reports are welcome in the issue tracker. A docstring that leaves a unit or convention unclear counts as a documentation bug. Changes that touch the physics come with a test, and claims come with a source; see CONTRIBUTING.md. Until version 1.0 the programming interface may still change between minor versions; any such change is listed in the release notes.

Licensed under Apache-2.0.