Where the angle comes from

A rule that cannot heal a hole

The placement rule corrects itself against a displacement — that is what the lag-one correlation of −0.6 has been saying for three phases. It does not correct itself against a deletion. Which organ is removed decides whether the stem is back on its lattice in twenty-four organs or never, and the boundary between the two is sharp, reproducible and in the middle of the front.

Worth reading first: The organ that was taken away · The sequence has a memory · Where the noise gets in.

The intervention does not end when the next organ has been placed. The organ is still missing, the stem keeps growing, and what it does over the next few hundred organs is a second experiment that costs nothing extra to run.

It has an obvious expected answer, and the expected answer is wrong for a third of the offsets.

The rule is self-correcting, and this site has the number

The expectation comes from a measurement three phases old. The divergence sequence of a stem grown by the rule has a lag-one autocorrelation of about −0.6: a divergence larger than the settled angle is followed by one smaller, and the deficit is made up almost at once.

The memory of a divergence sequence, at 0.75° of scatterWith no noise at all the lag-one correlation is 0.54: the rule corrects itself, so a lattice arrives with a memory in it. Matched at the same recorded scatter, placement noise leaves -0.10, jostle noise leaves 0.66, field noise leaves 0.47. The band is ±0.13, which is what an uncorrelated sequence of this length gives.-0.25000.2500.500123456lag, in nodescorrelation between a divergence and the one that many nodes laterno noiseplacement noisejostle noisefield noisesampling band4 runs each · 243 divergences per runmatched at 0.75° of scatter
Fig. 1 The statistic the expectation rests on. Consecutive divergences are strongly anticorrelated, which is what a self-correcting placement looks like from the outside: an organ placed to one side of its minimum leaves a gap that pulls the next one the other way.

That is a restoring force, and a restoring force is what heals a disturbance. A displaced organ is pulled back. Noise of any of the three kinds this site distinguishes leaves a pattern that is still the same pattern.

Where each kind's lattice gives wayThe largest amplitude at which every run still has a lattice, and the scatter it produces there. The amplitudes are incomparable — field 0.015 (fraction of the barrier), jostle 1 (degrees of azimuth), placement 0.8 (degrees of azimuth) — and the scatters agree to 19%. The boundary belongs to the pattern rather than to the disturbance: a lattice fails at about a degree and a half of scatter, and which of three mechanisms produced it does not move where.field1.64°intact to 0.015, broken by 0.02jostle1.72°intact to 1, broken by 1.4placement1.42°intact to 0.8, broken by 13 runs per amplitudescatters 19% apart
Fig. 2 And how much of it the pattern takes. All three kinds of noise cost the lattice at about the same recorded scatter, which the measurement phase read as the boundary belonging to the pattern rather than to the disturbance.

So the natural prediction is that a removal is a large disturbance which the rule undoes: a transient of some tens of organs, then the lattice again.

What actually happens, offset by offset

Each ablated stem is continued for three hundred organs and watched for a recovery — the first organ after which every later divergence stays within 1.5° of the settled 137.84°, with at least sixty of them to check, so that the last few angles of a wrecked run cannot be mistaken for a return.

Both edges of the front heal; the middle of it does notThe same removals, followed for 300 organs each. A cut one to three places back is undone within fifty organs and a cut ten to thirteen places back within sixty. A cut in between is never undone: the divergence sequence settles into an exactly repeating cycle of 4 or 8 angles and holds it for the rest of the run. The rule corrects a displacement and cannot correct a deletion.organ removed, counted back from the tiporgans placed before the stem is back on its lattice102243484never51256never7never8never9never105311591242137— the front ends here140150160rise 0.005 · pair 8/13generated from a stated rule, not drawn to look right
Fig. 3 How long each removal takes to be undone. The two edges of the front heal and the middle of it does not, and the boundary between the two behaviours is sharp: at four places back the stem never recovers, and at five it recovers in a hundred and twenty-five organs.

The pattern of it is worth setting out plainly, because it is not what a restoring force predicts.

Cut at the tip and there is nothing to heal. Removing the most recent organ costs nothing at all: the next primordium appears where the removed one was and the sequence continues, so the recovery time is zero. Two places back takes 24 organs and three places back 48.

Cut at the far edge of the front and the stem recovers. Ten, eleven, twelve and thirteen places back take 53, 59, 42 and 7 organs. Five places back takes 125, which is the longest recovery measured and still a recovery — on three cut points of five, as the section on reproducibility below has to report.

Cut in the middle and it never recovers. Four, six, seven, eight and nine places back are still off their lattice after three hundred organs, with mean divergences of 186°, 228°, 184°, 186° and 182° and spreads of 54° to 83°.

A cut three back is undone after 48 organsThe divergences of a stem whose organ three places back was removed, against the same stem uncut. The sequence is thrown by 53° and is back within 1.5° of its settled 137.8° after 48 organs, and stays there for the remaining 252. This is the rule correcting itself: an organ placed to one side of its minimum leaves a gap that pulls the next one back.100200300050100organs placed after the removaldivergence, in degreesback on the latticerise 0.005 · cut 3 backgenerated from a stated rule, not drawn to look right
Fig. 4 A cut three places back, which recovers. The sequence is thrown by 53°, wanders for about fifty organs, and settles back onto the divergence it had before with the organ still missing. This is what the restoring force was expected to do everywhere.
A cut eight back is never undoneThe divergences of a stem whose organ eight places back was removed, against the same stem uncut. It never returns. What it settles into repeats exactly every 8 organs — 47°, 96°, 137°, 273°, 138°, 271°, 230°, 272° — and holds that cycle for the whole 300-organ run, with a mean of 186° and a spread of 83°. A rule that corrects a displacement does not correct a deletion.100200300050100organs placed after the removaldivergence, in degreescycle of 8rise 0.005 · cut 8 backgenerated from a stated rule, not drawn to look right
Fig. 5 A cut eight places back, which does not. The stem never returns to 137.8°. What it does instead is the subject of the next essay, and the thing to notice here is that it is not disorder — the trace repeats.

It is worth dwelling on how different those two behaviours look in the same axes, because the difference is not one of degree. A healed cut wanders for a few dozen organs and then produces divergence after divergence within a tenth of a degree of 137.84°, indefinitely. An unhealed one produces a sequence whose mean is nowhere near the settled angle and whose spread is comparable to the whole circle — and which is nonetheless not disordered at all, as the next essay takes up. Nothing in between was observed at any offset: no stem drifted slowly back, and no stem recovered and then lost it again.

Where the boundary is, and where it is not

The five offsets that never heal are 4, 6, 7, 8 and 9 out of a front thirteen organs wide. They are neither the contact offsets nor the non-contact ones: 5, 8 and 13 are the three shortest hops at this rise, and the set of unhealing offsets contains 8, excludes 5 and 13, and includes four offsets that are not contacts at all.

Which offsets give short hops, at a rise of 0.005The two lowest points are at 8 and 13, and those are the parastichy numbers. Offset 1 is high because a hop of one node is at least the rise, which is what makes a stem easier to count than a disc.00.2000.400102030index offsetmedian hop between node i and node i+m813300 nodes, 34 offsets triedshortest at 8 and 13
Fig. 6 The contact offsets at this rise, ordered by how close the two organs come on the surface. The set of removals a stem cannot undo does not line up with them, which is worth stating because it was the first hypothesis and it is wrong.

What the unhealing set does line up with is age within the front. Both ends of the front are safe and the middle is not. The reading that fits is geometrical rather than arithmetical: a hole at the very top is filled by the organ that was going there anyway; a hole at the bottom of the front is nearly enclosed by organs that remain, so almost nothing is missing; a hole in between is a real vacancy in the part of the surface the rule is actively placing against, and the organ that fills it is then itself out of position for the organs that come after.

That is a cascade rather than a displacement, and a restoring force that acts on displacements does not act on it. The rule is self-correcting against being pushed and is not self-correcting against being cut.

Take away the organ six places back, and the next one goes into the holeThe last 34 organs of a stem at a rise of 0.005, unrolled. The open circle is the organ removed — six places before the tip. The ring at the top is where the rule puts the next organ with every organ present; the filled mark beside it is where the rule puts it with that one missing. The two are 101.7° apart, against a local spacing of 25°, and the vacancy itself is 107.1° from the undisturbed answer. Nothing else differs between the two runs: same rise, same history, same rule.moved 101.7°open ring: where the next organ was going · filled: where it goes · large open circle: the organ removedrise 0.005 · cut 6 back · height ×6generated from a stated rule, not drawn to look right
Fig. 7 A cut six places back — inside the unhealing band. The vacancy is in the middle of the front, the next organ goes 102° to fill it, and by doing so it is 102° away from where the organs after it were going to place themselves against.

The cascade can be watched happening. Take the cut six places back. The next organ goes 102° from where it was going, into the vacancy. The organ after that is now placed against a neighbourhood whose most recent member is 102° out of position, so it too is displaced, and by a comparable amount; and the one after that against a neighbourhood containing two displaced organs. Within four organs the front has been rebuilt out of organs none of which is where the undisturbed stem would have put it, and there is no arrangement of the ones that remain that the rule can walk back to. The restoring force is still there — the lag-one correlation is still negative on the wrecked stem — and it is restoring towards a different lattice.

That is the sense in which a deletion is not a large displacement. A displacement leaves the neighbourhood intact and moves one member of it. A deletion changes what the neighbourhood is, and every organ placed afterwards inherits the new one.

Noise does not rescue it, which is what makes it an attractor

A deterministic model that gets stuck in a bad state is a suspicious object. Real apices are not exact, and a rule that only fails when it is run without noise would be reporting a property of the arithmetic.

So the same cut was made with a jostle in the run — the third kind of noise, the realistic one, where each organ is placed exactly and then the organ it sits on grows, so what the next organ computes against has moved.

Three disturbances, three places to get inThe rule reads its neighbours, builds a profile of the energy at every azimuth, takes the least of it, and records a position. field noise enters at the profile; jostle noise enters at the neighbours; placement noise enters at the record. Two of the three are upstream of the choice and can change which minimum is taken; the third is downstream and never can.upstream of the choicethe neighboursalready placedthe profileenergy by azimuththe choicethe least of itthe recordwhat a ruler readsfield noisejostle noiseplacement noiseone rule, three entry pointsthe order is the argument
Fig. 8 The three places a disturbance can enter the rule. A jostle is the one an apex actually has: it is invisible in what a botanist measures and present in every decision the rule makes afterwards.

At a jostle of 0.1° the wrecked stem’s tail is 186° ± 83° — indistinguishable from the noiseless run. At 0.4°, which is nearly the amplitude at which the lattice fails on its own, it is 149° ± 92°: still nowhere near 137.8°, and now with the disturbance doing most of the spreading.

Noise does not put the stem back. Whatever state a mid-front cut leaves it in, that state is stable — an attractor with a basin, rather than a knife edge the arithmetic happened to balance on.

Placements that went to a different minimum, per thousandThe rule's own counterfactual, run beside it: where would this node have gone with the noise taken away and everything else left alone? Placement noise displaces the node after the argmin, so the answer is always "here" — 0.4°, 0.8° all give zero. A jostle and a field perturbation are upstream of the choice and change one or two placements in a thousand while the lattice is still intact.field 0.0052.10.70° of scatterfield 0.00750.01.00° of scatterfield 0.010.01.12° of scatterjostle 0.41.10.87° of scatterjostle 0.81.11.12° of scatterplacement 0.40.00.94° of scatterplacement 0.80.01.42° of scatter3 runs each · a basin change is half a local spacingplacement noise: zero by construction
Fig. 9 The statistic that separates a disturbance which changes what the rule chooses from one that merely moves where it puts the answer. A jostle changes the choice once or twice in a thousand placements; a single deletion changes it permanently.

It is worth being precise about what “stable” means here, because the site has a statistic for it. basinChanges asks how often a disturbance sends an organ to a different minimum than the same neighbours would have handed back with the disturbance taken away — the rule’s own counterfactual, run alongside it. A jostle changes the choice once or twice in a thousand placements while the lattice is intact; placement noise, which arrives after the choice, changes it exactly zero times at every amplitude tried, including amplitudes that have already destroyed the pattern.

A deletion changes the choice once, at the moment of the cut, and then never has to change it again — because after the cascade the rule is choosing correctly among a set of organs that is no longer the one it started from. The comparison puts the intervention in a different class from all three kinds of noise: it is the only disturbance in this collection that moves the pattern from one attractor to another and leaves it there.

The recovery times are not a rate

The eight offsets that heal do so in 0, 24, 48, 125, 53, 59, 42 and 7 organs, reading outwards from the tip. Two things about that list are worth stating and one is worth refusing to state.

The two: it is not monotone in the offset, and its largest member sits directly beside the unhealing band. Five places back is the last offset before the band begins and it takes 125 organs — two and a half times any other recovery, and on two cut points of five it does not recover at all — which is what a boundary looks like from the safe side. Thirteen places back takes seven, which is what a boundary looks like from the far side of the front, where the cut was barely a cut.

The refusal: these numbers are not a decay constant and should not be fitted to one. A recovery time here is the first organ after which the sequence stays inside 1.5° of the settled angle for at least sixty organs, which is a threshold-crossing on a trace that wanders rather than a time constant of an exponential. Changing the threshold to a degree or to two degrees moves the individual times by tens of organs while leaving the verdicts — healed, not healed — untouched. The verdicts are the measurement; the times are a description of the traces.

That distinction matters more here than it usually would, because a recovery time is exactly the kind of quantity a reader would want to compare against a plastochron. Two and a half plastochrons versus a hundred and twenty-five is a real difference and it is the one to carry away; the difference between 42 and 53 is not.

What the sharpness costs, and what it buys

The boundary between healing and not is one organ wide — five recovers, four does not — and a boundary that sharp deserves a check that it is not an accident of where along the stem the cut was made.

It is not, with one exception that is worth more than the rule it breaks. The whole table was repeated at five cut points forty organs apart, and fifteen of the sixteen offsets give the same verdict at every one of them.

The sixteenth is five places back, which recovers at 125 organs at three cut points and does not recover within three hundred at the other two. Five is the offset immediately beside the band that never heals. So the one place the verdict moves with where the cut was made is the boundary — which is where a boundary should be soft, and it is the only evidence here that the band has an edge rather than a wall.

The table was also repeated at 4,608 azimuths, where the front’s width and every displacement inside it agree with the coarse grid to within a quarter of a degree.

What the finer grid does to the rises already publishedThe two rises this site has argued from and the one it published as having no answer, each read at both azimuth grids, five stems apiece. A filled mark agrees with the position counter, a half mark contradicts it, an open mark is a refusal. At 0.013 and 0.005 the readings are identical at both grids, so nothing already written depends on the sample count. At 0.008 they are not: 384 azimuths gives 5/8, 5/8 and 1152 gives 8/13, 8/13, against a counter that says 5/8. That rise was chosen in the previous phase because the three shortest lattice offsets there are within a fifth of each other, and a stem with no answer answering differently on a different grid is the object behaving as it was said to.risefive stemsthe position counter0.0133845/85/85/85/85/85/80.01311525/85/85/85/85/85/80.0053848/138/138/138/138/138/130.00511528/138/138/138/138/138/130.0083845/85/85/80.00811528/138/135/8the previous phase's settingsgenerated from a stated rule, not drawn to look right
Fig. 10 The sample grid deciding an answer, from the phase that caught it doing so. Here it decides nothing: the recovery table is the same at 1,536 azimuths and at 4,608, which is what allows the sharpness to be reported rather than hedged.

What it buys is a second observable an experiment could put to a plant, and one that is easier than the first. The displacement of the next organ needs a measurement made within one plastochron of the ablation. The failure to heal needs no timing at all: it is visible in the finished shoot, weeks later, as a stretch of stem whose divergences never return to what they were below the wound.

Both vary; only one of them varies enough to findEach organ's step exponents, divided by its own mean so the two are comparable. The ogive's run over 15 per cent of their mean across 5 rings. The convex head's run over 1.15 per cent across 5 — inside the band a 3 per cent error on each ring position leaves, so no ruler separates it from a flat disc.0.9000.95011.050123which step of the ladderexponent ÷ its meanan ogive — 15%a convex head — 1.15%what 3% per ring allows5 rings on the ogive · 5 on the head15% against 1.15%
Fig. 11 What a real specimen supports, from the survey thread. A quantity that shows in a finished shoot rather than in a single internode is the kind this collection has repeatedly found to be the only kind a herbarium sheet can settle.

There is a third use, and it is the one that makes this worth a phase rather than a paragraph. The first essay’s experiment measures a number — the front’s width, which is the larger parastichy number. This one measures a map: which removals a pattern can undo. Two accounts that agree about the first can disagree about the second, and the transported-error account has nothing to say about either, since in it no organ’s position is a function of which organs exist. So the two experiments are not one experiment run twice; they are a count and a susceptibility, and a plant that gave the first and not the second would be saying something specific about how its apex differs from the rule.

Three things this does not say

It does not say a plant cannot heal an ablation. Surgical experiments on apices are a century old and the usual report is that the pattern reorganises and carries on. This says something narrower and checkable: in a model whose only response to a vacancy is to re-take the minimum, the vacancy’s position in the front decides whether the pattern comes back, and the boundary is one organ wide. A plant that heals every ablation is evidence about what a real apex does that the model does not — regrowth of the wound, a plastochron that is not fixed, a primordium whose radial position is free — and that is a more useful finding than agreement would have been.

It does not follow from the first essay’s result. The front is thirteen organs wide and the unhealing band is five of them, and nothing in the front’s width predicts which five. Both facts came out of the same runs and only the first was expected.

And it does not explain which five offsets fail. Age within the front is the description that fits, and it is a description rather than a mechanism: it says where the unhealing band is and not why it ends where it does. A cut four places back fails and a cut five places back recovers, and nothing measured here distinguishes those two positions except that one of them is a contact offset — which cannot be the reason, since eight is a contact offset and fails.

A phase that wanted the mechanism would need to watch the cascade organ by organ at many more cut points than the seven used here, and would probably want a smaller quantity than a verdict: how far out of position the k-th organ after the cut is, as a function of both k and which organ was removed. That is a surface rather than a table, it is affordable, and it is the obvious next thing to compute.

Two stems at 0.75° of scatter, one angle at a timeThe divergence of each node, with the slow climb of the ladder removed. Both stems scatter by about 25.97° and a botanist would report them identically. The jostled one wanders in runs — its lag-one correlation is 0.70 — and the one with placement noise alternates about the mean at 0.21, because a displacement of one node enters two consecutive divergences with opposite signs.jostle noise — correlation 0.70placement noise — correlation 0.21243 nodes each, both at 25.97° of scattercorrelations 0.70 and 0.21
Fig. 12 The standing lesson of this thread arrived at once more: two stems with the same recorded scatter can differ in everything that matters. A healed cut and an unhealed one differ in the divergence itself, which is the first time in three phases that the difference has been visible to a protractor.
A cut 13 back is undone after 7 organsThe divergences of a stem whose organ 13 places back was removed, against the same stem uncut. The sequence is thrown by 3° and is back within 1.5° of its settled 137.8° after 7 organs, and stays there for the remaining 293. This is the rule correcting itself: an organ placed to one side of its minimum leaves a gap that pulls the next one back.100150200250300050100organs placed after the removaldivergence, in degreesback on the latticerise 0.005 · cut 13 backgenerated from a stated rule, not drawn to look right
Fig. 13 And the fastest recovery in the table, at the far edge of the front: seven organs, from a displacement of 2.6°. A cut there is almost not a cut.

Shares its objects with

Essays that name at least two of the same things, and that neither author linked.

  • A disturbance the organs share — both name artefact, autocorrelation, divergence angle, ensemble, equilibrium, honest limits, lattice, measurement, noise, the placement rule, self correction, tolerance
  • A disturbance with a memory — both name artefact, autocorrelation, divergence angle, ensemble, honest limits, lattice, measurement, noise, parastichy pair, the placement rule, self correction
  • The disturbance that travels — both name autocorrelation, divergence angle, ensemble, honest limits, lattice, measurement, noise, parastichy pair, the placement rule, self correction, tolerance
  • The grid was in the number — both name artefact, autocorrelation, divergence angle, ensemble, honest limits, measurement, noise, the placement rule, rise, tolerance
  • Two readings from one stem — both name artefact, autocorrelation, divergence angle, ensemble, equilibrium, measurement, noise, rise, self correction, tolerance
  • A comb is evidence of a rule — both name autocorrelation, divergence angle, equilibrium, lattice, measurement, noise, parastichy pair, the placement rule, self correction

Named objects

A flat tag is an object no other essay names yet.

AblationArtefactAutocorrelationDivergence angleEnsembleEquilibriumHonest limitsLatticeMeasurementNoiseParastichy pairThe placement ruleRiseSelf correctionTolerance