Plasmata
Every module so far asks what a rule — written, trained, or selected — can produce on a lattice. Plasmata is a sibling project asking the same question of a different substrate: continuous, physically modeled solar plasma rather than any rule chosen in advance. This page hosts prose about that project alongside this project’s own from-scratch toy physics engine, tested to the same standard as everything else in this atlas.
part of The Automata Atlas →
Plasmata — the sibling question, asked of matter
Plasmata is a solar-plasma laboratory searching, in the site's own words, for "life-like dynamics in a solar plasma." Its physics is 2.5D isothermal resistive MHD — the coronal-loop geometry the sun's own magnetic loops sit in — evolved forward in Elsässer carriers W⁺ and W⁻ plus a current J, all starting from zero: no seed structure, no hand-placed pattern, just the field equations and time.
This atlas has spent nine phases asking what a rule — written, trained, or selected for — can produce on a lattice: gliders, replicators, structured equilibria, a rule that learns its own numbers. Plasmata asks the same question of a different substrate: not a rule anyone chose, but continuous, physically grounded matter, to see what it organizes into on its own.
Plasmata runs six "emergence starters," arenas built to test for a specific kind of self-organization rather than to reproduce a known result: a homogeneous coronal loop (wave-supported magnetic organization), a fluctuation bath (spontaneous individuation), a fissioner alpha (repeated body splitting), a metastable propagule (compositional inheritance), a loop challenge (boundary maintenance), and a field filament (transport-guided organization). Four further "positive controls" — an Alfvén packet glider, a zero-net dipole glider, a flux-rope breather, and a counter-packet collision — are deliberately excluded from any emergence claim: they exist to prove the instrument can detect known, designed structure at all, not to demonstrate anything novel.
All of this runs in a persistent experiment rack rather than as one-off trials: matched A/B arms share a starting state, with arm B given an independent forcing seed, run alongside footpoint-drive-off, phase-scrambled-drive, and high-damping control variants. A candidate is watched continuously against its own controls, not examined once and called a result.
The next two sections cover how Plasmata judges what it's watching (heredity, the falsification standard); the last two are this project's own contribution — a from-scratch physics engine and a toy demonstration of that same falsification logic.

Plasmata's own interactive plasma field, mid-run: both footpoints driven and glowing at the boundary edges, the interior dark with no persistent structure of its own — the site's own HUD (8 coherent regions, threshold 0.379, coherence Hc 0.000, lock 0.000) is the site's own reading, not this project's.
Captured from the live Plasmata site, 2026-08-19.
Heredity — a destination, not yet a result
Plasmata's long-term target is what its site calls hereditary plasma attractors: self-organized structures the physics produces and then, in principle, propagates — a parent structure ablated, a descendant surviving that ablation as genuine transmission rather than coincidence. The site's own promotion ladder runs upward from Tier 0, and no candidate has been promoted past it: the site states the reason directly, "Tier is capped below reproduction until parent-ablation and multi-generation transmission tests exist." A "lineage trace" panel exists for exactly this purpose — labeled for provisional descent state-change candidates — but as of this writing it is still waiting for its first entry, showing a candidate score of 0.000 and zero coherent regions. Heredity is Plasmata's stated destination, not a demonstrated result.
Whether any candidate is even a coherent structure worth tracking is decided by named metrics, not by eye: an Alfvén crossing time (τ_A) serves as the site's own natural time unit; a segmentation threshold separates a coherent region from background noise; a coherent-region count tracks how many such regions exist at once; translation-shape R² checks whether a moving structure keeps its own shape; spectral entropy tracks how concentrated or diffuse its Fourier content is; and a post-cut energy ratio is exactly the falsification move the next section describes, applied to a real candidate instead of a toy.
This atlas already has its own replicators — Langton's loop, which copies a fixed 8-state pattern exactly, every time, with no variation for selection to act on; and the evolution loop, which selects Lenia genomes for persistence plus novelty across a handful of generations, over a hand-specified two-parameter genome space. Neither is what Plasmata is after. Plasmata's hereditary attractors, if and when parent-ablation and multi-generation transmission tests exist to certify them, would be a lineage that emerged from physics itself, not from a rule table or a parameter space this project chose in advance — a different, harder question, not a fancier version of either loop.
The falsification battery — a rigor standard, shared
Plasmata states its promotion standard as a method, not an impression: "Driver independence, cutoff survival and numerical convergence — not visual complexity — govern promotion." A candidate fails if, in the site's own words, it is "locked to the footpoint driver, disappears under grid refinement, or fails matched no-drive and phase-scrambled controls." Three separate ways to fail, each aimed at a different illusion: a pattern that only exists because something outside it keeps feeding it energy, a pattern that only exists at one particular grid resolution and vanishes at a finer one, and a pattern that a matched control — the same setup with the drive off, or with its phases scrambled — would have produced anyway. The positive controls named in the program section are excluded from any emergence claim for the same reason: proving the instrument can detect a designed structure isn't evidence that an undesigned one is real.
That standard is this project's own, run on a different substrate. Every claim in this atlas is scoped to what an actual test asserts, with the bound and the measured endpoint both named rather than a vague impression of "it works"; every widget is a display snapshot of a tested engine, not a standalone animation; and the About page keeps a running account of exactly what's measured, what's schematic, and what's still an open question. Plasmata's driver-independence and phase-scrambled controls are the same falsification instinct this project applies to its own claims: before a result counts, cut whatever might be secretly doing the work and see whether the result survives losing it. Two sections from here, that exact move — cut the drive, scramble the phases — runs live on two toy signals, so the logic is something to watch rather than just read about.

live chamber

footpoint drive off

phase-scrambled drive

high damping
The battery, in pictures: Plasmata's live chamber beside its own no-drive, phase-scrambled, and high-damping controls. The no-drive chamber is nearly dark — as of this capture, nothing in it self-sustains without the driver, which is the control's whole point.
Captured from the live Plasmata site, 2026-08-19.
Alfvén waves — this project's own toy physics
This project's own Alfvén-wave engine (packages/engine/src/alfven.ts)
is the toy physics behind the Plasmata instrument on this page: two
counter-propagating Elsässer fields, z⁺ and z⁻, on a periodic 1D line,
each a pure spectral phase rotation at speed ±v_A with no interaction
between them in this ideal, 1D, constant-v_A case — a decoupling that is
exactly why a z⁺ packet and a z⁻ packet pass through each other
unchanged.
That pass-through is Plasmata's own "counter-packet collision" positive control, in miniature: on the real site, colliding wave packets test whether an interaction leaves behind a persistent localized remnant; here, the same collision is exact enough to test directly, to floating-point precision. Every step is a spectral rotation, not a finite-difference approximation, so there is no discretization error at all — only rounding, which is why the claims below are tested to 1e-9.
Four facts this project's test suite checks, each to a stated bound: a launched packet's centroid moves at v_A to within 1e-9 after 100 steps; two packets launched toward each other cross, and the full two-packet run over 300 steps matches a single composed 300·dt step of that same state to within 1e-9 per cell; a single Fourier mode's amplitude decays at exactly exp(−ηω²t) over 200 steps, within 1e-9 relative error; and, at zero damping, total energy drifts by less than a relative 1e-9 over 500 steps. Every one of these bounds is scoped below the grid's Nyquist wavelength, per the engine's own documentation — a smooth packet built at the widths this widget launches carries negligible energy at that limit, so the exactness holds for everything actually on screen.
Launch a z⁺ and a z⁻ packet toward each other above and watch them cross without disturbing one another — the same counter-packet test Plasmata's own chambers run, at a scale small enough to check exactly.
The battery, run on two toy signals
This exhibit (packages/engine/src/battery.ts) demonstrates the LOGIC of
Plasmata's falsification battery on two toy candidates only — it makes
no claim about, and does not reproduce, any actual candidate from
Plasmata's own chambers. driven is a standing pattern sustained by
continuously forcing one grid cell at a fixed frequency, damped the
whole time by the same resistivity the Alfvén section above uses — left
alone, that damping would erase the pattern, so the driver is the only
thing keeping it alive. packet is the same ideal (undamped) Alfvén
packet from the section above, launched once and otherwise left alone,
never forced by anything after that first launch.
Cut the drive and the difference is immediate and measured, not just visual: 300 steps after the cut, the driven candidate's energy ratio falls to 0.396 (seed 1) — the driver-locked pattern's tell — while the self-propagating packet's ratio stays at 1.000, unaffected by losing a driver it never depended on. Phase-scrambling the packet is the other control: it preserves the packet's total energy to within a relative 1e-9 while its coherence — a peak-to-RMS measure of how sharply localized it still is — collapses to 0.474 of its pre-scramble value. Same energy, destroyed shape: exactly the distinction a driver-locked pattern and a self-propagating one make visible under the same two cuts.
The energy-ratio readout under each candidate above is the same post-cut energy ratio named among Plasmata's own metrics in the heredity section — just measured here on a forced cell and a launched packet instead of an actual coronal-loop or fluctuation-bath candidate. These two toy signals are not what Plasmata is testing for real. Its own persistent rack runs six chambers continuously against matched no-drive, phase-scrambled, and high-damping controls, on actual coronal-loop and fluctuation-bath physics rather than a single forced cell and a launched packet — see the live site for those.
The first three sections describe Plasmata itself — sourced from its own site, not built or tested by this project. The last two are this project’s own contribution: a toy Alfvén-wave engine and a falsification-battery demo, held to the same tested-claim standard as every other engine in this atlas.
Explore the rest of the taxonomy on the Atlas map, run the Alfvén and battery widgets in the Lab, or visit Plasmata itself. The fidelity of every claim on this page — what’s measured, what’s a sourced summary, and what’s an open question — is accounted for on the About page.