license: cc-by-4.0
task_categories:
- tabular-classification
- tabular-regression
tags:
- physics
- electromagnetics
- verification
- interval-arithmetic
- formal-methods
- counterexamples
- eda
- parasitic-extraction
pretty_name: Screening Ceiling — Certified Regions and Counterexamples
size_categories:
- n<1K
configs:
- config_name: regions
data_files: data/certified_regions.jsonl
- config_name: counterexamples
data_files: data/counterexamples.jsonl
screening-ceiling
📖 Documentation site — the portfolio narrative, the concepts, a full walkthrough, and what all of this proves (and does not).
A machine-certified impossibility result about coupling extraction, plus the concrete layouts where a plausible extractor predicts impossible physics.
Most ML-for-physics datasets are samples: here are some inputs, here are the answers, fit something. This one is different in a way worth being precise about. It carries a universal claim — a statement about every layout in a continuous four-parameter family, established by interval branch-and-bound rather than by sampling — together with existential counterexamples that refute a specific competing method.
Why this exists
When conductors are packed together, every other conductor screens the field between any two. So a pair's mutual capacitance inside an array is at most its isolated-pair value:
k = |C_full| / |C_iso| ≤ 1
Pairwise-superposition extraction — used throughout fast parasitic extraction —
assumes k ≡ 1. The certified claim here is that on a particular manufacturable
family it is provably never right, and quantifies by how much:
For every layout in the family box,
k ≤ 0.909090909091. A pairwise extractor therefore over-predicts the worst coupling by at least 10.000002% on every member of the family — not on average, not usually, always.
And the other direction: a second-order Born correction, the obvious cheap fix
when a full solve is too slow, does not merely stay inaccurate — on 27 layouts
here it predicts k > 1, which is anti-screening, a physical impossibility.
30-second quickstart
No install, no dependencies, nothing from the repository that produced it:
python3 verify.py
screening-ceiling independent re-derivation (stdlib only)
claim k <= 0.909090909091 for every layout in the family
forced error pairwise over-predicts by >= 10.0000%
regions 256 x 25 samples = 6400 layouts
worst sampled k 0.903974725909 (bound 0.909090909091)
margin to bound 0.005116183182
violations 0
worst at region 3.0.3.3 d0_um=55.7830 jog_mult=0.3838 pt_mult=1.0009 sep_mult=4.4492
counterexamples 27/27 re-derived and confirmed above the ceiling
consistent: no sampled layout exceeds the bound, and every counterexample re-derives
scope: A complete interval theorem about the frozen MONOPOLE-CLOSURE model only. The closure-vs-BEM/PDE model gap remains additive and unresolved. This witness does not establish Maxwell, BEM, driven-S, fabrication, or measured-silicon truth.
verify.py rebuilds the electrostatics from the published geometry using the
standard library alone — its own Gauss-Jordan inverse, its own potential matrix.
It does not import this dataset's producer, numpy, or anything else.
Sampling cannot prove the universal claim. That is what the interval branch-and-bound in the source proof is for. What sampling can do is refute it, and that is the useful thing to hand a skeptical reader: a cheap, dependency-free way to try to catch us being wrong.
Loading
from loader import load_regions, load_counterexamples, load_theorem
theorem = load_theorem()
print(theorem["statement"])
print(theorem["honest_scope"]) # read this one
for c in load_counterexamples():
print(c["case_id"], c["k_predicted"], c["n_pairs_violating"], "/", c["n_pairs_total"])
Optional conveniences: to_pandas("regions") and to_hf_dataset().
Contents
data/certified_regions.jsonl — 256 rows, the universal claim
The branch-and-bound partition. Each row is one region of the family box that
the prover certified, having subdivided it into leaves until the interval
enclosure of k fell below the bound everywhere inside.
| Field | Type | Meaning |
|---|---|---|
region_id |
string | position in the 4×4×4×4 root partition, e.g. 3.0.3.3 |
bounds |
object | {d0_um, pt_mult, sep_mult, jog_mult} → {lo, hi} |
status |
string | CERTIFIED for every row in this release |
certified_leaves |
int | leaves the region was subdivided into |
processed_leaves |
int | leaves examined, including interior splits |
sup_certified_k_hi |
float | largest k the enclosure admits anywhere in the region |
volume_fraction_of_region |
float | fraction certified (1.0 throughout) |
unresolved_leaves |
int | leaves left undecided (0 throughout) |
Totals: 237,490 certified leaves, 474,724 processed, 0 failure regions, 0 unresolved, certified volume fraction 1.0.
The published rows are the 256-region partition, not all 237,490 leaves — the source proof records per-region certification and aggregate counts. That is a real limitation of what is published and it is stated rather than glossed: you can re-derive any region yourself, but you are not being handed every leaf.
data/counterexamples.jsonl — 27 rows, the existential refutation
Layouts where born_second_order predicts k > 1.
| Field | Type | Meaning |
|---|---|---|
case_id |
string | e.g. born2_n6_p100_s1 |
model |
string | born_second_order |
n_conductors |
int | 6, 8 or 12 |
nominal_pitch_um |
float | 60, 80 or 100 |
seed |
int | generator seed |
worst_pair |
[int, int] | indices of the worst-violating pair |
k_predicted |
float | predicted screening factor (> 1 for every row) |
n_pairs_violating |
int | pairs above the ceiling in this layout |
n_pairs_total |
int | ordered pairs in this layout |
xy_um |
[[float, float]] | conductor centres, micrometres |
radius_um |
[float] | conductor radii, micrometres |
eps_r |
float | relative permittivity (4.6) |
2,060 violating pairs across the 27 layouts, worst k = 3.5141. Full
coordinates are included deliberately: a counterexample you cannot rebuild is an
anecdote, not evidence.
data/theorem.json — the claim, its scope, its provenance
The statement, the family box, the certified totals, the exact geometry definition, and the SHA-256 of the source proof witness.
Geometry
Four parallel circular conductors forming two tight pairs:
pitch = 1.6 · d0 · pt_mult
separation = pitch · sep_mult
jog = jog_mult · separation
centres: (0,0) (pitch,0) (separation,jog) (separation+pitch,jog)
every conductor has diameter d0
Family box: d0 ∈ [25,60] µm, pt_mult ∈ [1.0,1.2], sep_mult ∈ [2.5,4.5],
jog_mult ∈ [−0.4,0.4]. Self-term radius scale 1.0.
loader.family_layout(...) builds it for you.
Scope, honestly
This is a theorem about the monopole-closure model, not about Maxwell. The closure is a zero-parameter analytic multiple-scattering model that matches a boundary-element reference to 0.081% in the exact two-cylinder limit, but the closure-versus-solver gap is an additive, disclosed, unresolved term. It is never absorbed into the bound.
That 0.081% comes from the boundary-element solver used to develop the closure, which is not part of this release — so unlike every other figure on this page, you cannot re-derive it from what is published here. It is quoted because it bounds how much trust the closure has earned, and a reader is entitled to know which numbers are checkable and which are taken on our word.
The scope line travels with the data, in theorem.json:
A complete interval theorem about the frozen MONOPOLE-CLOSURE model only. The closure-vs-BEM/PDE model gap remains additive and unresolved. This witness does not establish Maxwell, BEM, driven-S, fabrication, or measured-silicon truth.
Three further limits worth stating plainly:
- One family, not all layouts. Four conductors in a specific arrangement. Nothing here says anything about a different topology.
- The bound is not tight. The certified supremum is 0.90909089; the worst
layout found by adversarial search is ≈0.9053. The gap is the price of a
first-order interval relaxation, not a claim about physics. That 0.9053 is
the second figure on this page you cannot re-derive from the release — it
came from a differential-evolution search in the source prover. What you
can check here is weaker but points the same way:
verify.pyreports a worst sampledkof 0.903974725909 at its defaults, and sampling harder climbs toward that 0.9053 without ever reaching the bound — at--seed 7, 25 / 100 / 400 samples per region give 0.902144353337, 0.903775408593, 0.904308125283, with zero violations at each. - No measured data. Every number is computational.
Reproduction
python3 verify.py --samples 100 --seed 7 # sample harder, different seed
python3 verify.py --self-test # prove the checker still discriminates
python3 export.py --check # confirm data matches a fresh export
The self-test is the part that makes a clean report worth anything. It fabricates
an impossible bound, tampers with a published value, and requires the checker to
reject both — then confirms an isolated pair reproduces k = 1.000000000000
exactly, since a lone pair has nothing to screen it.
Troubleshooting
verify.py reports violations — that is the interesting outcome, and we
want to hear about it. Sampling cannot prove the bound but it can refute it, so
a genuine violation means the theorem is wrong. Before reporting, re-run with
--self-test to confirm the checker still discriminates: a checker that has
stopped working can produce either verdict.
ModuleNotFoundError: numpy from verify.py — it should never import
numpy. If it does, the file has been edited; the shipped version runs under
env -i /usr/bin/python3 with nothing installed, and a test asserts it imports
no third-party module.
loader.to_pandas or to_hf_dataset raises ImportError — those two are
conveniences and do need pandas / datasets. Everything else, including
verify.py, is standard library only.
The Hub viewer shows two configs and you wanted one table — regions and
counterexamples have different schemas and are deliberately separate. Pick the
config in the viewer's dropdown, or use load_regions() / load_counterexamples().
export.py --check says the data does not match — it re-derives the files
from the committed proof witness and compares. A mismatch means either the data
or the witness was edited. Counterexample regeneration also needs maxwell-lint
installed, since they are produced by running its reference models.
You want every certified leaf, not the 256 regions — they are not published. The source proof records per-region certification plus aggregate counts, so the 237,490 leaves are attested but not enumerated here. That is a real limit of this release and is stated rather than glossed.
Provenance
Exported by export.py from a committed proof witness produced by an
outward-rounded interval branch-and-bound prover (256 parallel roots, 243.5 s
wall clock, centered/mean-value enclosure forms). The witness digest is recorded
in theorem.json; export.py --check re-derives the files and compares.
Counterexamples are generated by running the open-source
maxwell-lint reference models, so they are reproducible
from published code alone.
Citation
@misc{screening_ceiling_2026,
title = {Screening Ceiling: Certified Regions and Counterexamples for
Many-Body Coupling Extraction},
author = {ChipletOS / Genesis contributors},
year = {2026},
note = {CC-BY-4.0}
}
The rest of the toolkit
Eight artifacts that answer one question in different places: is this model physically possible? Each is a grader — it can tell you a model is wrong; none can tell you one is right.
sparam-lint |
Is an S-parameter model physically possible? Five laws + a negative control. |
maxwell-lint |
Does a coupling extractor predict impossible physics? Screening ceiling k ≤ 1. |
abstain-bench |
Does a model know when to shut up? Abstention recall, never pooled with accuracy. |
sparam-conformance |
11 labelled networks with verified ground truth. Grades the graders. |
screening-ceiling ← you are here |
A certified impossibility result + 27 counterexamples. Zero-dependency verifier. |
physics-lint-action |
The same checks, in your CI. |
physics-lint-mcp |
A physics oracle your AI agent can call. |
| Try it in your browser | All three checks, no install, runs client-side. |
These tools grade a model. Producing one that is passive by construction — so it cannot fail these laws whatever its parameters — and accurate at speed in the many-body regime, with calibrated abstention and a fail-closed signoff certificate, is the commercial core: ChipletOS.
Licence
CC-BY-4.0. Synthetic and computational throughout; no proprietary or measured data. Attribution: ChipletOS / Genesis contributors.
Related
maxwell-lint— run the ceiling test on your extractorsparam-conformance— the S-parameter analogue- ChipletOS — the closed core: a learned many-body coupling operator that stays inside this ceiling and is accurate at speed, with calibrated abstention and a fail-closed signoff certificate
Contributing
One non-negotiable rule here: the verifier must import nothing from this project, so a skeptic can read it in one sitting and run it with nothing installed. CONTRIBUTING.md has the detail. Each sibling repository states its own, and they differ — that is deliberate, and it is why each is trustworthy on its own terms.