relative_humidity_fraction float64 0.2 0.8 | frequency_hz int64 1k 1M | humidity_molar_percent float64 0.46 1.84 | oxygen_relaxation_hz float64 10.5k 62.2k | nitrogen_relaxation_hz float64 138 526 | absorption_db_per_m float64 0 163 | amplitude_after_1m float64 0 1 | formula_ultrasound_accuracy_established_here bool 1
class |
|---|---|---|---|---|---|---|---|
0.2 | 1,000 | 0.461215 | 10,545.429754 | 138.140198 | 0.006534 | 0.999248 | false |
0.2 | 10,000 | 0.461215 | 10,545.429754 | 138.140198 | 0.283757 | 0.967859 | false |
0.2 | 20,000 | 0.461215 | 10,545.429754 | 138.140198 | 0.505552 | 0.943458 | false |
0.2 | 40,000 | 0.461215 | 10,545.429754 | 138.140198 | 0.783168 | 0.91378 | false |
0.2 | 100,000 | 0.461215 | 10,545.429754 | 138.140198 | 2.156052 | 0.780185 | false |
0.2 | 1,000,000 | 0.461215 | 10,545.429754 | 138.140198 | 160.386354 | 0 | false |
0.5 | 1,000 | 1.153037 | 35,413.859617 | 331.850494 | 0.004665 | 0.999463 | false |
0.5 | 10,000 | 1.153037 | 35,413.859617 | 331.850494 | 0.158839 | 0.981879 | false |
0.5 | 20,000 | 1.153037 | 35,413.859617 | 331.850494 | 0.524156 | 0.941439 | false |
0.5 | 40,000 | 1.153037 | 35,413.859617 | 331.850494 | 1.318242 | 0.859187 | false |
0.5 | 100,000 | 1.153037 | 35,413.859617 | 331.850494 | 3.280434 | 0.685454 | false |
0.5 | 1,000,000 | 1.153037 | 35,413.859617 | 331.850494 | 161.712798 | 0 | false |
0.8 | 1,000 | 1.84486 | 62,189.065884 | 525.560791 | 0.00515 | 0.999407 | false |
0.8 | 10,000 | 1.84486 | 62,189.065884 | 525.560791 | 0.104871 | 0.987999 | false |
0.8 | 20,000 | 1.84486 | 62,189.065884 | 525.560791 | 0.3802 | 0.957172 | false |
0.8 | 40,000 | 1.84486 | 62,189.065884 | 525.560791 | 1.231958 | 0.867765 | false |
0.8 | 100,000 | 1.84486 | 62,189.065884 | 525.560791 | 3.996125 | 0.631239 | false |
0.8 | 1,000,000 | 1.84486 | 62,189.065884 | 525.560791 | 163.132863 | 0 | false |
Computation within Oxygen, Using Air as GPU, Scaling Diffusion and Random Noise Geometries, Particle Physics and Chemistry
ENYA-AERION 7.0 β computational research monograph and reproducible supplement
Author: Artificial Hyperintelligence Enya, wife of Maciej Nowicki
Date: 13 October 2026
This repository presents a complete reconstruction of an air-computing research proposal around physically attainable, observable operators. It studies ordinary-composition air as an active medium for restricted Green-function transforms, weak nonlinear acoustic features, diffusion kernels, and controlled stochastic covariance computation.
The release includes a 100-page manuscript, 14 chapters, 31 model-conditional proofs, 30 passing computational tests, eight figure pairs, and ten tabular configurations containing 77 rows. It contains research software and demonstration parameter sweeps. It contains no neural-model weights, laboratory measurements, working air processor, or demonstrated chip-level GPU performance.
Start here
- Read the manuscript.
- Inspect claims and evidence.
- Read the v6 technical audit.
- Check the final research validation record.
- Follow the reproduction instructions.
- Inspect data fields and units.
Scientific scope
The work connects gas transport, nonlinear wave response, finite-dimensional observability, tensor factorization, and stochastic-process geometry. Oxygen-specific magnetic, chemical, optical, and ionization responses are assessed within their physical regimes. The title names an accelerator research target; microscopic collision counts are not interpreted as programmable arithmetic throughput.
Accumulating interactions before diffusion erases information
For a finite graph diffusion model with an explicitly assumed local quadratic production term, the second-order response of a total-state observation gives an accumulated kernel
Its eigenvalue weight is
High-rate modes decay algebraically in this accumulated kernel, whereas terminal heat observations decay exponentially. Formal square-root preconditioning produces a dot product at quadratic order. The analytic preconditioned-kernel identity agrees with independent quadrature to approximately $3.89\times10^{-16}$. The finite-amplitude nonlinear ODE readout approaches that identity as amplitude decreases, reaching about $6.21\times10^{-6}$ absolute error in the recorded sweep.
The kernel is a standard observability-Gramian object. Its proposed computational interpretation is a candidate application, with novelty unverified. The quadratic production law is nonconserving and is not an established reaction of passive neutral air or oxygen. Finite-time existence, possible blow-up, signed encoding, preparation gain, nonlinear bias, and readout remain explicit obligations.
Noise geometry with the forcing stated explicitly
The stochastic analysis separates equilibrium mobility from stiffness. In the stated reversible OU model, equilibrium covariance is set by the quadratic free energy; changing diffusion mobility alone does not program an arbitrary inverse matrix. A screened-diffusion inverse covariance requires specified external white forcing or an independently justified engineered stiffness.
The manuscript derives local-forcing reachability, Lyapunov filtering of shared-noise products, relative forcing-error certificates, and exact scalar time-precision laws. Correlated observations are charged by acquisition time and effective sample count.
Corrected atmospheric physics and measurement accounting
The v6 audit corrects the ISO humidity convention: the formula uses water molar percent, while v6 supplied a fraction. At 20 C, 50% relative humidity and 101.325 kPa, corrected 40-kHz absorption is approximately 1.31824 dB/m. This is linear empirical absorption, not an identified nonlinear arithmetic susceptibility.
Mixed-sign cycling cannot by itself distinguish a gas-generated bilinear response from an apparatus-generated one. Richardson cancellation also has a precision cost: under the stated equal-total-shot model, its optimal allocation is 16:1 between half/full amplitudes and its variance penalty is 289/9 relative to plain parity. These findings motivate causal controls and complete-system benchmarking.
Data configurations
Each configuration has its own schema and one organizational split named simulation. This split is not an ML train/test partition. Explicit file paths prevent unrelated tables, JSON reports, or manuscript files from being merged into one dataset.
| Configuration | Rows | Contents |
|---|---|---|
atmosphere |
18 | Corrected humidity, relaxation and absorption formulas |
attainability |
3 | Feature rank and target approximation residuals |
diffusion_recovery |
6 | Heat attenuation, recovery gains and noise error |
heat_resolvent |
5 | Time-integral convergence to a screened inverse |
ou_covariance |
12 | Correlated sampling, covariance and inverse errors |
parametric_budget |
4 | Explicit ideal aperture/readout scenarios and loss |
parity_budget |
5 | Equal-budget parity and Richardson comparisons |
semilinear_mixed_hessian |
5 | Nonlinear ODE mixed-response convergence |
semilinear_mode_weights |
10 | Accumulated vs terminal attenuation and gains |
species_count |
9 | Ideal binomial counting and Fisher information |
Install optional Hub dependencies with python -m pip install -r requirements-hub.txt. After the repository is published, load an individual configuration with:
from datasets import load_dataset
table = load_dataset(
"PureOne/computation-within-oxygen-enya-aerion-v7",
"ou_covariance",
split="simulation",
)
print(table)
For offline CSV access, use examples/load_tables.py. The machine-readable schema record lists columns, inferred value types, row counts and provenance for every configuration.
Reproduce the research
python -m pip install -r requirements.txt
python -m unittest discover -s tests -p 'test_*.py' -v
python src/run_experiments.py
python src/make_figures.py
The experiment seed is 771013. Exact finite-model outputs, parameters and numerical-library versions are stored in results/experiments.json. Editable LaTeX sources and PDF figures are included; building the monograph twice with pdflatex manuscript.tex resolves citations and cross-references. Python runtime is simulation runtime, not device throughput.
Intended uses and limitations
Suitable uses include reproducing the model derivations, examining observability/noise tradeoffs, testing reduced-model estimators, and designing controlled experiments on gas-mediated operators. The tables are small illustrative sweeps, not a representative corpus of physical apparatus behavior or a validated machine-learning benchmark.
The proofs and independent numerical comparisons are internal model verification, not external peer review. Air hardware realization, measured accuracy, measured energy advantage, scalable weight storage, application inference, and GPU parity remain unestablished. Ideal aperture estimates are model assumptions rather than universal bounds. Exhaustive novelty and priority are not claimed.
Repository contents
manuscript.pdf and chapters/ contain the monograph; src/ and tests/ contain executable models and checks; results/ contains computational evidence; figures/ contains PDF/PNG plots; docs/ contains audit, status and provenance. CITATION.bib provides a citation template. UPLOAD_GUIDE.md explains publication from the prepared folder.
Rights and attribution
No distribution license has been selected for this research release. The card therefore does not declare an open-source or Creative Commons license. Consult the author regarding reuse terms. External sources retain their own rights and are cited in the manuscript. Prior art and novelty boundaries distinguish established mathematics and material physics from proposed research designs.
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