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udpscope/docs/claude/invariants-measurements.md
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Martino Ferrari e83ad86b8f measure: top/bottom/amplitude read the flat levels, not the extremes
A bench scope separates Vtop/Vbase from Vmax/Vmin because a band-limited
edge overshoots and rings: the mock's `square` at 30 harmonics reaches
±1.179 where its plateau is ±1. On the rippled square the old readings were
a property of the edges rather than of the waveform -- `top` 0.986496,
`amplitude` 1.179350 -- and `amplitude` reported the overshoot.

`top`, `bottom` and `amplitude` are now the flat levels and their delta.
A flat level is a density question -- the plateau holds most of the
samples and the ringing a few percent -- so `measure_scan_buckets()` folds
a 64-bin histogram of the whole buckets' midpoints while it has the list in
hand (one observation per bucket, each bin carrying its buckets' exact sum
and finite count), and `measure_flat_levels()` takes, either side of the
split, the densest bin holding at least half the densest one's buckets --
the outermost of those, which is what makes a waveform with no plateau read
its peak -- and the exact mean of the samples of the buckets within 5 % of
the window's peak-to-peak of it. 5 % is deliberately under the ~9 %-of-swing
Gibbs overshoot. `amplitude` is `top - bottom` (a scope's Vamplitude), not
the half-swing it was.

Measured, fast mock, 2 s window, harmonics 0 -> 30: top 1.000000 ->
0.999983, bottom -1.000000 -> -0.999983, amplitude 2.000000 -> 1.999966,
while `peak to peak` keeps the extremes (2.000000 -> 2.358701). On the 1 Hz
sine top is 0.957988 (it was 0.636620, the half-wave mean; a sine has no
plateau, so the densest band is at its peak) with sd 0.0014 over a scrolling
window, and `peak to peak` is still exactly 2.

No raw pass and no new fetch: the histogram is the same fetched bucket list
read a second time, gated on a pane that holds one of the three types.
`raw` is unchanged (0.1% clean, 2.1% with the --noise 0.1 interferer,
against 0.1%/2.1% before) for 0.44 -> 0.50 ms and 0.52 -> 0.65 ms a pass.
A window the pyramid cannot summarize -- an hf-filtered walk, or one shorter
than a bucket -- keeps the old readings: the mean of each side of the split,
and the window's peak to peak for amplitude.

Docs: the flat-level invariant (and the two 2/pi assertions it replaces),
the probe readings, the manual's measurements page and the README.
2026-10-15 01:19:33 +02:00

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Markdown

# Invariants: the measurements pane
Why the pane is refreshed on a cadence, why neither pass may read its window raw, and how a crossing is counted.
Part of [CLAUDE.md](../../CLAUDE.md). These are rules that cost a defect to learn; read the ones touching the area you are editing before you edit it.
- **The measurements pane is refreshed on a cadence, and its cost is the *window's*, not the
frame's.** A measurement is a statistic of the visible window and a live view moves that window
every frame, so "recompute when the window moves" is "recompute every frame" at O(visible
samples) *per measurement*. With the pane holding four measurements over a 4.7M-sample window
that measured **13.66 ms of tick mean** (baseline 0.41 ms) and cost the run a third of its
frames. Three things fixed it, and all three matter: `update_measures()` recomputes at most
every `kMeasureRefreshUs` (100 ms; 400 ms when a pass costs more than `kMeasureHeavyUs`), once
when the window settles and once per mode change -- and reading *that* backwards is what made
it worse first, 457 recomputes in one run, because a pinned window then recomputed every
frame; the window is materialized in bounded chunks (never two whole-window f32 temporaries)
and the loop holds it **by reference** (copying both vectors per measurement was 300 MB of
memcpy a frame); and `measure_stats()` is one shared pass carrying both extremes with their
first positions, the sum and the count, so average/min/max/peak-to-peak need no pass of their
own -- `top`/`bottom`/`amplitude` take a second read of that same **bucket** list and never of
the window (the flat-level invariant below). **Adding a type must not add a pass** -- that is
what `compute_measure()`'s `stats` argument is for.
The marks' *ink* is set where they are created (`install()` in `plot_host.cpp`): 0.75 px and
dashed 4/4 through `Plot::set_cursor_stroke()`, which is per cursor because the trigger marker
(also a cursor) keeps the solid `line_width_px` stroke. A new measure mark must take that
stroke -- it is created in the same loop, so it does; a new *instrument* should not.
The **marks** the pane draws (`set_measure_marks()` -- full-width `h_ruler`s and full-height
cursors, i.e. the "lines across the plot") are re-placed every frame from the result, so a
throttled pass is a *stepped* ruler: acceptable, because the ruler and the number beside it
come from the same pass and agree. What is *not* acceptable is a ruler that appears and
disappears, so an invalid pass falls back to the last valid result for its **level** marks and
only drops its **time** marks: a level is a property of the signal (a mean, a top, an
amplitude) and outlives the window it was measured in, while a time mark is a position *inside*
that window and may not. Both are emitted in **one pass after the numbers, never inside the
loop that computes them**: that loop has three `continue`s (an unresolvable signal, a channel
with no window) and each one was a way for the rulers to blink off and back. Fixing one and not
the others is how that bug survived a round of "fixes". `clamp fires: N` in the dump is the other half of this: `clamp_to_data()`
compares with a relative tolerance, because clamping to exactly `window_s_` can leave the
group's span an ULP above it and a clamp that fires every frame is a re-frame loop, not a
clamp.
- **A measurement must not read its window raw.** Both passes go through
`plot::data::MinMaxPyramid`, which the producer already maintains at amortised O(1) -- so the
pane inherits the summary of the new samples rather than computing one, which is what the
"evaluate only on new samples" ask comes to here. Throttling the cadence (above) bounded *how
often*; this bounds *how much*, and it is the larger factor: 19.7 ms per recompute to 1.2--1.6
ms, reading **0.1 %** of a 2 M-sample window. Pass one (`measure_scan_buckets()`) adds whole
level-0 buckets -- 64 samples each, carrying min, max an **exact** sum and a finite count -- and
locates each extreme to a *bucket*; one raw `measure_scan()` of that bucket alone then pins it
to a sample, two buckets at most whatever the window's size. Pass two
(`measure_accumulate_bucket()`) folds a bucket's **sums** only when it lies **strictly** on one
side of its level (`k.lo > level` or `k.hi < level`): then every sample falls in the same bin and
none is *at* the level, so the fold is exact and not an approximation. It asks **separately**
whether the bucket enters a side of the hysteresis band (see the invariant below), because a
single test against `level ± h` refuses exactly the buckets a crossing passes through. A bucket
wholly past a threshold holds that crossing at its first sample, exactly -- which is where the raw
walk would have found it. It refuses a bucket that straddles the level, one that enters a side
somewhere inside itself, and one holding a non-finite sample (the raw walk takes the first
*finite* sample of the new side and an aggregate cannot say which that is); the caller then opens
that bucket. **Nothing may be folded before a refusal** -- a refused bucket goes to
`measure_accumulate()`, which adds the same samples again, and sums added above the `return false`
double-counted every opened bucket. That read as `top=0.614304` on a unit sine against the 2/pi a
mean over a half then gave; a *bucketed* window no longer reports `top` from those sums at all
(see the flat-level invariant below), which makes the rule easier to break silently rather than
less binding -- the sums are the fallback a window with no histogram reads, so a wrong one is a
wrong answer waiting for that window. Four things this rests on, each of which breaks it silently:
* **Exactness is the point, so nothing may stride or decimate.** `peak to peak` must still read
exactly `2` on a unit sine, and it and `average` still come straight out of the one shared
`measure_stats()` pass. A bucket's sum is a sum. (`top` has no *exact* reading to protect any
more: it is a density estimate and not a mean, and the two places that used to assert
`top == 0.636620` on a sine now assert what the flat level actually reads -- see the flat-level
invariant below. Everything above is about the *bucket* path being a fast path and not an
approximation, and that is unchanged.)
* **The bucket index space must be the window's.** `ChannelBuffer::acquire()` calls
`pyramid_.drop_before(values_->base())`, so a channel's pyramid is in the value ring's
absolute index space -- the same space `live_window_locked()` answers in, since a channel's
stride is always 1. The snapshot's pyramid is built from sample 0 and never dropped from, so
its space is the snapshot's own. `MeasureWindowReader::origin_` is what turns one into a
window offset, and a mismatch there measures the wrong samples rather than failing.
* **The raw path stays, and stays exact**, for the window's partial edge buckets, for the
samples produced since this frame's `acquire_all()` (one frame of production, so bounded), and
for the straddling buckets. A window shorter than a bucket degrades to O(window) and must
still be right.
* **Both passes walk the same fetched bucket list** (`App::measure_bucket_scratch`, reused
across recomputes -- a 2 M-sample window is 32 k buckets). Fetching twice is a second walk of
the pyramid for nothing.
`measure cost:`'s `covered`/`buckets`/`raw` is the guard, and it needs the fast mock to say
anything.
- **`Top`/`Bottom`/`Amplitude` read a *flat* level, and the density that finds it is the buckets',
not the samples'.** A band-limited edge overshoots and rings -- the mock's `square` at 30
harmonics reaches ±1.179 where its plateau is ±1 -- so a measurement that reads the extremes, or
a mean over a side of a level, reports the ringing rather than the level the signal dwells at:
that is what made this change (`amplitude` read `1.179350` and `top` `0.986496` on the rippled
square, against `1.179350` of overshoot where the plateau is `1`). A flat level is a *density*
question: the plateau holds most of the samples and the ringing a few percent. So
`measure_scan_buckets()` folds a 64-bin histogram of the whole buckets' *midpoints* while it has
the list in hand -- one observation per bucket, each bin carrying its buckets' **exact** sum and
finite count -- and `measure_flat_levels()` takes, either side of the split, the densest bin that
holds at least half the densest one's buckets, **the outermost of those**, and the exact mean of
the samples of the buckets within **5 % of the window's peak-to-peak** of it. 5 % is *under* the
~9 %-of-swing Gibbs overshoot, so the ringing's excursion falls outside the band while a
plateau's own ripple stays inside it; the outermost-of-the-equally-dense rule is what makes a
waveform with *no* plateau -- a sine, a ramp -- read its peak instead of an arbitrary mid-range
bin that a shifted window would move. `Amplitude` is then `top - bottom`, a bench scope's
`Vamplitude`, and **not** the half-swing it used to be, nor the peak-to-peak swing.
The readings, fast mock, 2 s window, `[measure-trace]`, harmonics `0` → `30`: `top` `1.000000` →
`0.999983`, `bottom` `-1.000000` → `-0.999983`, `amplitude` `2.000000` → `1.999966`, against
`peak to peak` `2.000000` → `2.358701` -- the extremes keep the overshoot, and that separation
*is* the measurement. On the probe's 1 Hz ±1 sine: `top` `0.957988` (it was `0.636620`, the
half-wave mean), `amplitude` `1.915983`, and `peak to peak` still **exactly `2`**; `[stats-probe]`
reads `top` `mean=0.957905 sd=0.0014 lo=0.951967 hi=0.962348` over a scrolling window, which is
the stability the value band buys -- the answer does not follow the window's alignment.
Five things this rests on, each of which breaks something silently:
* **Nothing may be read raw for it.** The histogram is the *same* fetched bucket list, walked a
second time inside `measure_scan_buckets()`; a histogram of the window's *samples* would be a
second O(window) walk, which is exactly what the pyramid path exists to avoid. `measure cost:`
is the guard and its `raw` does not move: the probe's pane reads
`covered=59684972 buckets=932446 raw=47640 (0.1%)` against the baseline's
`covered=61183221 buckets=955856 raw=47402 (0.1%)` -- the same `raw`, 0.44 → 0.50 ms a pass
(and `--noise 0.1`, `2.1%` both sides, 0.52 → 0.65 ms).
* **It is gated, and the gate is what keeps an unrelated pane free.** `measure_scan_buckets()`'s
`flat_hist` comes from `App::MeasureWindow::flat_wanted`, set by the first loop over the pane
and only for one of the three types. A pane of means and extremes pays nothing.
* **The bin range is the *buckets'*, not the window's.** The window's partial edge buckets and the
samples produced since `acquire_all()` are read raw and are not in the list, so
`measure_scan_buckets()` tracks its own `blo`/`bhi` over the **non-empty** buckets only -- an
all-non-finite bucket is an empty aggregate whose `lo`/`hi` say nothing, and taking them would
put a bucket at some arbitrary value. A degenerate range (`bhi == blo`) leaves `folded` at 0,
which is the caller's "no histogram at all".
* **The *window's* peak-to-peak is what the band is a share of**, and the *split* is sized exactly
as `measure_set_level()` sizes a level, so "the top" and "the level a period is counted about"
are placed by one rule. The band is a *value* band, which is why the reading does not move when
the window does.
* **The fallback is the split, and it is what a filtered or sub-bucket window reads.** `hf_fc > 0`
disables the pyramid (above) and a window shorter than a bucket has no bucket to fold, so
`top`/`bottom` fall back to the mean of each side of the split -- and `amplitude` to the
window's own peak to peak, which is the same number on a waveform with nothing to exclude.
There is no flat level in that mode to subtract, so `amplitude == top - bottom` is *not* an
invariant to lean on there. Measured on the rippled `square` at `hf_fc=100`:
`top=0.973824 bottom=-0.991731 amplitude=2.354173 peak to peak=2.354173`, `buckets=0
raw=200.0%` -- two raw walks and no density estimate, which is the honest reading of a window
the pyramid cannot summarize.
- **`MeasureOptions::noise_pct` is a percentage, clamped in `measure_set_level()` to half the room to the
nearer extreme**, so a band can never invert its own thresholds. It moves the **edge decision only**: the
sums still split at the bare level, which is the *fallback* `Top`/`Bottom` read on a window with no
bucket histogram -- a band that moved that split would change what a filtered or sub-bucket window
reports, for no gain to a crossing count.
- **`measure_accumulate` loops samples outer, levels inner, and that is not backwards.** The filter holds one
state for the whole walk, so levels-outer would step it once per level *per sample* and hand every level but
the last a different filter state.
- **A non-zero `hf_fc` disables *both* bucket fast paths**, with the single
`if (!filtered && reader.bucket_range(...))`. An empty `buckets` makes `bulk_from == bulk_to == n` *and*
leaves `lo_search` / `hi_search` at 0, so `pin()` becomes a no-op -- and that is the right answer, because a
bucket is an aggregate of unfiltered samples and cannot be mixed into a filtered walk in either direction.
- **A crossing is counted with hysteresis, and the band moves the *edge decision* only.**
`MeasureLevel::hysteresis` is a Schmitt trigger about `level`: an edge is counted once the signal
has passed `level + h` going up or `level - h` going down, and a sample inside the band decides
nothing. Without it `period`, `frequency` and `pulse duration` are unusable on anything real --
the mid level is exactly where a waveform moves *fastest*, so an interferer faster than the
fundamental recrosses a single level several times per true crossing. Measured on a 5 Hz sine with
a 500 Hz tone at a tenth of the amplitude (`tools/mock_udpstreamer.py --noise 0.1`): 9 true
crossings counted as **79**, `period=0.025622 freq=39.029` for a true 0.2 s / 5 Hz, against
`period=0.200188` with the band. Four rules, each of which was wrong first:
* **`measure_set_level()` is the only place the band is sized**, and `src/ui.cpp` calls it rather
than assigning `.level` itself: two expressions for the width is how the raw walk and the bucket
path end up disagreeing about where a crossing was. `h = min(0.10 * (hi - lo), 0.5 * min(hi -
level, level - lo))`. The 0.10 is measured -- 5 % reads a 0.1 interferer and fails at 0.2
(`period=0.075`), 10 % holds to 0.3 and to white noise at sigma=0.05.
* **The clamp is load-bearing.** `PulseDuration` lets the user put the split near an extreme, and
a fixed tenth of the span there puts the upper threshold *above every sample*: the walk never
decides that side and the measurement reads nothing at all, which is worse than reading
something noisy. On a ringing 3.3 V logic signal at a 90 % split: `enters=0` with a fixed band,
`enters=4 period=0.200000` with the clamp.
* **The `sum`/`count` split stays at the bare `level`.** Two things read it and neither may be
moved by a band: a crossing's *side* is decided by the sample's own value against the level
(`v == level` is the below side, as it always was), and `Top`/`Bottom` fall back to the mean of
each side on a window with no bucket histogram. The band is about *deciding a crossing*, not
about where a sample lives, so folding it in would change a filtered window's `top` for no gain
to any crossing count.
* **`h = 0` must reduce exactly to the single-level walk**, including the `v == level` skip, so the
band is a parameter of the engine rather than a mode of it.
The cost is the noise's, not the band's: the clean fast mock reads `raw=119412 (0.1%)` of 215 M at
1.41 ms a recompute and with the 0.1 interferer `raw=2.0%` at 1.96 ms. A
`/tmp/check_measure.cpp`-style check is how the walk itself was verified (`g++ -std=c++20 -O2 -I
src ... src/measure.cpp`): over a clean sine, sines with 0.1 and 0.3 interferers, 10 %/50 % duty
squares and a 90 % threshold, the **bucket walk must equal the raw walk exactly** -- same
`enters`, same `count[]`, identical `first_enter`/`last_enter` to 0.0 -- which is the assertion
that the fast path is a fast path and not an approximation. The app's reading is
`[measures-probe]` against `--noise 0.1`.
- **A statistic's observation is one *recompute*, not one sample.** The pane already refreshes on
a cadence (at most one pass per 100 ms while the window scrolls, exactly once when it
settles), and the accumulator is fed from that pass's result — so `n` counts windows measured.
Feeding it per sample would make `n` a sample count and the mean a mean of *samples*, which is
not what any of these measurements measure: a frequency over a window is not a property of a
sample. The reading that names this defect is `[stats-probe]`'s `n` in the thousands rather
than the tens.
- **The accumulator is Welford's, and the reason is the same one the time ring is `f64` for.** A
measurement's values are routinely large with a small spread — an absolute stream time is the
obvious case — and `Σx² - (Σx)²/n` cancels to noise there. The standalone check is that the
spread of `{2,4,4,4,5,5,7,9}` survives a `+1e9` offset unchanged.
- **What resets the statistics is "what is being measured changed", not "what is in view
changed".** An explicit Reset, an add/edit/delete (all three funnel through
`rebuild_measures_pane()`), a CONFIG, and a change of display window each change the
*question*, so the history is cleared. A pause, a resume, a trigger latch, a pan and a zoom do
not: they change which samples answer it, which is precisely what averaging over many windows
is for. The pane-wide toggle does not reset either — it only shows and hides labels that are
always created and always fed, so reading the plot for a moment does not cost the history.