What a plant might be doing

One way round, seventeen times

The two chains that change places in a wrecked stem are adjacent, which is symmetric and says nothing about direction. Label them by lag from the hole and the one displaced forwards is always the lower of the two — on every row of the census, without an exception.

Worth reading first: The damage has a period · The organ that was taken away · Counting the spirals.

Two chains change places above a hole: one displaced forwards, one displaced backwards, by equal and opposite amounts, on neighbouring chains, on seventeen of the thirty wrecked cuts in the census.

“Neighbouring” is a symmetric word. It says the two chains are one apart and it says nothing about which of them went which way. That is a question with two possible answers on every row, and it turns out to have one answer on all of them.

A period of 8, with the hole's own chain at the top. Each mark is one residue class of the displacement profile, placed round a ring at its own residue, with the chain the removed organ sat on at the top. The radius is how far that class sits from the level the rest of them share. six of the eight classes sit together at the middle ring; two do not, and on this row they are one pair, equal and opposite to within a twentieth. The forward one is chain 7 and the backward one is chain 0, one residue above it, which is the order every row of the census puts them in.
Fig. 1 One wrecked cut’s chains round its own period, with the forward and backward exceptions drawn differently.

The measurement

Label each chain by the lag of its members counted from the removed organ, so that chain 0 is the chain the organ was on. Take the chain displaced forwards and the chain displaced backwards, and subtract their labels round the period.

The answer is +1 on every one of the seventeen rows. The backward-displaced chain is always the one immediately above the forward-displaced one. Not one row has it the other way round.

Which chain the backward exception sits on, over the census. Chains are numbered from the removed organ, so chain 0 is the chain the hole was on and chain 2 is two organs along it. The exchange is at the hole's own chain on 10 of the 17 rows that carry one, against 2.8 rows for a chain drawn at random from each row's own period. That is far more often than anywhere else and it is not every row, so the position is a tendency rather than a rule — and the file says so rather than rounding it up.
Fig. 2 The chains the exchange sits on, over the census. This essay is about the difference between the two labels rather than about either of them.

Why that is a result and adjacency was not

Adjacency is one bit per row and it was already known. Direction is a second bit, and it is the bit that separates two accounts of what happened.

A swap — two chains trading positions — is symmetric. It has no preferred direction and would give plus one about half the time and minus one about half the time. A shift — one chain moving up a place and displacing its neighbour down — is not symmetric, and gives the same sign every time.

A period of 8, and the two classes that are not with the rest. The same wrecked stem, folded on the lag it kept: one row per residue class, each drawn at the mean displacement of its own organs against the level the rest of them share. The bar through each row is the spread inside that class, and the widest of them is 0.87° — so within a class the displacement is a constant. six classes sit at the common level. The two that do not sit at 134.3° and -134.2°, equal and opposite to within 0.0 per cent, and they are neighbouring residues. The stem's own divergence is 137.44°, so an exception is one organ's step.
Fig. 3 The same profile as a set of levels. The two exceptions are one above the common level and one below it, and which is which is the measurement.

Against what a coin would do

Seventeen rows agreeing on a two-sided question is one in a hundred and thirty thousand under a fair coin. That is the whole of the statistics, and it is worth being clear that the coin is the right null here.

It is the right null because nothing in the design picks a direction. The chains are labelled from the hole, the displacement is a signed difference between two runs, and the sign convention is fixed before any row is read. There is no step at which an analyst chooses which chain to call forward.

The exceptional pair, measured in divergences. One row per wrecked cut whose profile has exactly one pair of exceptional classes, drawn at the size of that pair divided by the stem's own settled divergence. Every row sits between 0.882 and 1.076, so the two chains that came apart moved by one organ's step rather than by two or by half of one. The residual is not scatter: rows are grouped by the lag the stem kept, and every lag sits wholly above the line or wholly below it. Why a surviving 5 or 7 overshoots and a surviving 4 or 8 falls short is not answered here.
Fig. 4 Every row’s exceptional pair. The direction is a property of each row and the rows are not sorted by it.

The rows are not one lattice seen seventeen times

They come from eight lattices across both branches, at rises from 0.005 to 0.026, with offsets from three to nine organs back and surviving lags of 4, 5, 7 and 8. Four of the eight lattices contribute more than one row and four contribute one.

That matters because seventeen rows from one stem would be seventeen readings of one event. These are seventeen cuts, each with its own control, each grown separately.

The four lattices contributing several rows are worth a second look for the same reason. On the 0.010 stem the three cuts share a control and differ only in which organ was removed, so their three plus-ones are less independent than three rows from three lattices. Counting the lattices rather than the rows gives eight agreements, which is one in two hundred and fifty-six — weaker than one in a hundred and thirty thousand and still not a coin.

Every stem that never repaired, and the lag it kept. The 19 offsets across six lattices at which a single removal leaves a stem that never returns to its divergence. For each one: which organ was removed, the period of the block of angles the stem settles into, the lag whose hop survived the cut unchanged, and how many whole turns the stem gains over one period of that lag. The block and the surviving lag are the same number in every row. The marked row is the one whose survivor is not a parastichy number of the lattice that was cut — a hop 6.8 times the length of a contact hop, which no census would report and which the rule held rigid all the same.
Fig. 5 The census the rows come from, with its lattices, offsets and surviving lags, so the spread of conditions can be read.

Two accounts, and what each predicts elsewhere

The swap account and the shift account are not only different stories about one measurement. They predict different things about a quantity this thread already has: the slip, which is how far the wrecked stem’s own divergence sits from its control’s.

A shift by one place moves every organ above the hole one position earlier in the sequence, which changes the divergence by a whole turn divided by the surviving lag. That is exactly what the slip has been measured at — 72.0° at a lag of 5, 45.0° at a lag of 8, 51.4° at a lag of 7 — on every wrecked cut in the census.

A swap of two chains moves nothing else and predicts a slip of zero. So the slip was already deciding between these two accounts, measured for a different reason, and it decides for the shift.

A wreck is a whole number of extra turns. For each of the 19 stems that never repair, the slip of its settled divergence multiplied by the lag whose hop survived. Every value lands on a whole number of turns — the horizontal lines — with a largest departure of 2.97 degrees, against divergences that have moved between 0 and 103 degrees. 17 of the 19 close on exactly one turn. So a wrecked stem is the stem it was with one extra turn threaded through every period of the family that survived, which is a dislocation with a stated size rather than damage.
Fig. 6 The slip on every wrecked cut, drawn as turns per surviving lag. It is the third independent reading pointing the same way.

What the labelling does not do

A reader who has followed the chain numbering will notice that the convention is a choice: numbering by the cut run’s own ordinals rather than by the control’s shifts every chain label by one.

It does not touch this result. The orientation is a difference between two labels, and adding a constant to both leaves the difference alone. So the one result in this thread with no exceptions is also the one that survives the convention being wrong.

A period of 5, with the hole's own chain at the top. Each mark is one residue class of the displacement profile, placed round a ring at its own residue, with the chain the removed organ sat on at the top. The radius is how far that class sits from the level the rest of them share. three of the five classes sit together at the middle ring; two do not, and on this row they are one pair, equal and opposite to within a twentieth. The forward one is chain 1 and the backward one is chain 2, one residue above it, which is the order every row of the census puts them in.
Fig. 7 A different row, labelled the same way. The pair sits at different chains and the direction between them is the same.

What a shift would look like

The chain that lost an organ is one organ short. The organs above the gap are each placed one position earlier in the sequence than they would have been, so the chain they belong to has shifted along by one.

If that is what happens, the chain immediately after the shifted one takes an organ that used to belong elsewhere, and the two are displaced in opposite directions by one step. Which is what the measurement says: equal, opposite, adjacent, and one way round.

Take away the organ four places back, and the next one goes into the hole. The last 30 organs of a stem at a rise of 0.013, unrolled. The open circle is the organ removed — four 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 164.1° apart, against a local spacing of 41°, and the vacancy itself is 172.7° from the undisturbed answer. Nothing else differs between the two runs: same rise, same history, same rule.
Fig. 8 The removal and the organs placed after it. A chain that is one organ short is the shape this account rests on.

But the direction is the wrong way for the simplest version

The simplest shift account predicts that the chain losing an organ is the one displaced, and the chain losing an organ is the hole’s own, chain 0. On ten rows chain 0 is the backward one, which fits; on seven it is not involved at all.

And on the ten where it is, the backward chain is the hole’s and the forward chain is the one below it — the chain of organs one place earlier in the sequence, which is below the hole rather than above it. The simplest picture has the disturbance propagating up from the gap, and the measurement puts one half of it underneath.

How far every organ moved, 6 places back at a rise of 0.01. One mark per organ above the hole, at the angle it sits from where the same organ sits in a control that shares its history. The collection has read two numbers out of profiles like this one — the largest displacement anywhere, and the first organ's — and never the profile. It is not a bump that decays. After about 18 organs it settles into a repeating pattern of eight levels, one per residue class modulo 8, which is the lag whose hop this stem kept. six of those levels sit together and two do not.
Fig. 9 The whole profile above one hole. Nothing below the hole is drawn, because nothing below it moves.

Which is impossible, and therefore a labelling fact

Nothing below the hole moves. The two runs share their history to the last digit below the removed organ, so a chain “below the hole” in the labelling is a chain whose members are above the hole and whose lag is congruent to a smaller residue.

That is the moment to be careful with words. The chains are residue classes, not places, and “one below” means one lower in a cyclic label. Reading it as a physical direction is exactly the error the labelling was introduced to avoid.

One wrecked stem, lag by lag — golden, rise 0.013, organ 4 back. How much each lattice hop moves from organ to organ in a stem that never repaired after a single removal, over its last 120 organs. The lag-one hop is the divergence itself and it swings by 65 degrees. The lag-5 hop swings by 0.11 degrees and sits 0.09 degrees from where the undisturbed stem put it, so that one family of the original lattice is still standing organ by organ. Its multiples inherit the same steadiness and nothing else comes within a factor of twenty. The block of angles this stem repeats has a period of 5, which is the surviving lag and not a coincidence.
Fig. 10 The lag spectrum that names the period. A residue class is a set of organs spread up the whole stem, not a place on it.

So what the result is, stated carefully

Order the chains by their lag from the removed organ, modulo the period. Then in that cyclic order the forward-displaced chain immediately precedes the backward-displaced one, on every row.

That is a statement about a cyclic ordering, and its content is that the exchange has a handedness. An arrangement and its mirror image would give opposite signs, and every stem in this census turns the same way.

The wrecked stem is the lattice it was cut from, wound the other way. The divergence of each organ placed after two were removed from a settled stem at a rise of 0.032, over the 200 organs following the cut. The upper line is the divergence the undisturbed stem holds, 139.6875°; the lower is 220.3125°, which is 360° minus it and therefore the same lattice with the opposite handedness. The sequence is thrown by the cut, wanders for a few dozen organs, and settles on the second line to four decimal places — 220.3125° against 220.3125° — where it stays. A counter shown the positions afterwards returns 3 and 5, the pair the stem was cut from. Nothing about the pattern has been lost; its chirality has been reversed, which at this rung a single removal cannot do.
Fig. 11 A lattice and its mirror image, which is the operation that would reverse this result if it were applied to a stem.

Which is a prediction

Grow the stems the other way round — start them at the mirror of their seed angle, so every parastichy runs the other way — and cut them identically. The prediction is that the orientation reverses on every row.

If it does, the result is about handedness and nothing else. If it does not, the orientation is a property of the labelling and not of the arrangement, and this essay is about an artefact. Thirty runs, and it has not been done.

Two patterns a counter cannot tell apart — counted 2/6 against 2/6. On the left, the top 120 organs of a spiral stem that never repaired after two organs were removed, settling at 175.01 degrees. On the right, a stem grown by a rule that places two organs at a time on every node. A counter shown the positions returns 2/6 for the first and 2/6 for the second, and a pair whose numbers share a factor is the usual signature of a whorled pattern. Rotate each pattern and the answer separates them at once: the whorled stem maps onto itself at a half turn and the wrecked stem maps onto itself at no fraction of a turn at all. Its shared factor is a fact about where its divergence landed, 4.99 degrees from 1 of 2 turns, and not about how it grew.
Fig. 12 Counts on a lattice and on its mirror, which is where a handedness claim has to be checked.

The prediction is cheap and it is the whole test

That is worth saying plainly. Every other check in this essay is a way of making seventeen rows into better evidence for a claim about seventeen rows. The mirror run is the only one that could show the claim to be about the wrong thing.

It costs thirty stems and thirty controls, which is the same as the census already grown. Nothing about it is difficult and it is not done, and the honest place for that is here rather than in a footnote.

One rule at p = 1, cut three ways. loop cut at 3/√h: 8/13 at 137.62° with 0.58° of scatter. exponential cut-off, 3: 8/13 at 137.58° with 0.50° of scatter. no cut at all: no lattice, 44° of scatter. The first two agree to 0.03° — the prediction held — and the third is what the same rule does when nothing cuts it.
Fig. 13 The check that a continued run is the rule itself, which is what makes a mirrored run comparable with an unmirrored one.

The sizes, which are the same result again

The exchange’s size is 88.0° to 147.2° across the seventeen rows, against settled divergences of 99.1° to 138.0°. One organ’s step, to within twelve per cent, which was the earlier reading.

A shift by one place in the sequence displaces an organ by one divergence step, which is what a size of one divergence means. So the size and the direction are two readings of the same account, and both fit it.

Four accounts of one angle, scored on the same 17 rows. Each bar is how far an account of the exchanged pair's size sits from the measurement, as a share of the control's divergence, averaged over the census. A step of the wrecked stem's own divergence is the obvious candidate and the worst of the four. The surviving family's own step is not the unit at all: that angle is a fifth of the exchange. A step of the control's divergence is close, and correcting it by a fifth of the surviving hop takes the worst row from 11.8 per cent to 4.0.
Fig. 14 Four accounts of the exchanged pair’s size, scored on the same seventeen rows. The unit is a step of the control’s own divergence.

And the size has a residual the direction does not

The size misses one divergence step by up to twelve per cent, and that miss has a pattern in it. The direction has no residual at all: it is plus one on every row, with nothing left over.

Which is the ordinary difference between a discrete reading and a continuous one. A sign has no error bar and an angle has, and it is why a result about a sign carried by seventeen rows is stronger than a result about an angle carried by the same seventeen.

What the exchange misses one divergence step by, against the surviving hop. Each mark is one wrecked cut. Across: the angle from an organ to the one its surviving lag places above it, on the control. Down: how much the exchanged pair's size falls short of one divergence step. The relationship is a straight line through the origin with a slope of about 0.2, and its sign is right on every row of the census — the four surviving lags give hops on both sides of zero and the residual follows each of them. The honest limit is the four: the hop hardly moves inside a lag, so the line rests on 11 distinct positions and not on 17.
Fig. 15 What the size misses one step by, against the surviving hop. The direction has nothing corresponding to this picture.

What the thirteen other rows say

Nothing, and they cannot. A row whose exceptions are three chains rather than two has no forward-and-backward pair to orient, so the question does not arise on it.

Those thirteen are not counter-examples and they are not evidence either. They are rows where the measurement is undefined, which is a third category and one this thread keeps having to name — an offset that recovers rather than wrecks is the same category one level up, and the census reports it as its own state rather than as a missing value.

How constant the displacement is inside one residue class. One row per wrecked cut in the census, drawn at the widest spread found inside any one residue class when the profile is folded on the lag that stem kept. 25 of 30 rows sit between 0.12 and 6.09 degrees, which on a quantity whose between-class differences run past a hundred and fifty degrees is a constant. The five that do not sit from 10.3° up. There is nothing in between, so the line drawn at 10° could have been drawn anywhere in a wide interval.
Fig. 16 The whole census by how steady its classes are. The thirteen rows without a pair are not the ragged ones.

The refusal that goes with it

Asking for the orientation of a row with three exceptions is refused rather than answered by taking the two largest. That is a small piece of machinery and it is the one that keeps seventeen from becoming thirty.

A rule that would return a direction for every row would have returned seventeen plus-ones and thirteen numbers computed from whichever two exceptions happened to be biggest, and the second group would have looked like scatter around a signal.

The exceptional pair, measured in divergences. One row per wrecked cut whose profile has exactly one pair of exceptional classes, drawn at the size of that pair divided by the stem's own settled divergence. Every row sits between 0.882 and 1.076, so the two chains that came apart moved by one organ's step rather than by two or by half of one. The residual is not scatter: rows are grouped by the lag the stem kept, and every lag sits wholly above the line or wholly below it. Why a surviving 5 or 7 overshoots and a surviving 4 or 8 falls short is not answered here.
Fig. 17 The exceptional pairs by size. Choosing the two largest exceptions of three is the operation the refusal prevents.

Why this was not found earlier

Because the earlier reading asked whether the two exceptional chains were adjacent, and adjacency is symmetric. The measurement that gives the direction is the same subtraction with the sign kept, and keeping a sign is a decision somebody has to make.

That is the shape of most of the leavings in this collection: not an experiment nobody could afford, but a quantity computed and then reduced before it was looked at. The profile itself was nine thousand numbers read for two for five rounds.

How far above the hole the damage becomes a pattern. One row per wrecked cut, drawn at the first organ from which every residue class stays at its own level for the rest of the run. On the 25 rows that reach it at all, it runs from 7 to 303 organs above the removed one; five rows never reach it inside the 300 organs each run is continued for. Below that point the stem is still moving, and the displacement of the first organ after the cut — the quantity that tells a cheap removal from an expensive one — is measured there. Above it, nothing changes again.
Fig. 18 Where the pattern starts on each row, which is the other reading that was sitting inside numbers already computed.

What it would take to break it

One row the other way round. Seventeen is enough to make a coin implausible and it is not enough to make an exception surprising: an eighteenth row at minus one would put the result at seventeen of eighteen and change it from a law to a tendency.

Which is what the position of the exchange already is, on the same seventeen rows. Two readings of one pair, and one of them has no exceptions and the other has seven.

The asymmetry between them is instructive. A tendency invites a search for the column that explains the exceptions, and four columns have been tried. A law invites a search for the assumption that manufactured it, and one candidate has been named and not tested.

Which chain the backward exception sits on, over the census. Chains are numbered from the removed organ, so chain 0 is the chain the hole was on and chain 2 is two organs along it. The exchange is at the hole's own chain on 10 of the 17 rows that carry one, against 2.8 rows for a chain drawn at random from each row's own period. That is far more often than anywhere else and it is not every row, so the position is a tendency rather than a rule — and the file says so rather than rounding it up.
Fig. 19 The position tally on the same rows. One reading of a pair is a law here and the other is a tendency.

What the seventeen rows have in common

Nothing that would produce this by construction. They are seventeen separate pairs of runs, each grown from its own seed, each cut at its own offset, each compared against its own control. The only thing shared is the placement rule.

That is worth checking rather than asserting, because a shared implementation is exactly the thing that can manufacture a shared sign. The check is the one this thread already runs on every continuation: grown to a length outright must equal grown shorter and continued, to the last digit, and it does.

One rule at p = 1, cut three ways. loop cut at 3/√h: 8/13 at 137.62° with 0.58° of scatter. exponential cut-off, 3: 8/13 at 137.58° with 0.50° of scatter. no cut at all: no lattice, 44° of scatter. The first two agree to 0.03° — the prediction held — and the third is what the same rule does when nothing cuts it.
Fig. 20 The check that a continued run is the placement rule and not a second implementation of it.

Where this leaves the account

A wrecked stem, on the seventeen rows that carry a clean exchange, is its control with one chain shifted along by a place and its neighbour pushed the other way. The size says one divergence step, the direction says the shift runs one way, and the slip says the whole arrangement turns by a turn over the surviving lag.

Three quantities measured for three different reasons, all consistent with one picture. What is missing is the mirror test, which is the only one that could show the picture to be about the labelling rather than about the stem.

A period of 5, and the two classes that are not with the rest. The same wrecked stem, folded on the lag it kept: one row per residue class, each drawn at the mean displacement of its own organs against the level the rest of them share. The bar through each row is the spread inside that class, and the widest of them is 1.62° — so within a class the displacement is a constant. two classes sit at the common level. The three that do not sit at 67.7° and -149.5°, equal and opposite to within 75.3 per cent, and they are neighbouring residues. The stem's own divergence is 136.78°, so an exception is one organ's step.
Fig. 21 A row’s levels. The account this essay converges on is that these are the control’s levels with two chains exchanged and everything turned by a fixed amount.

The one line

On all seventeen wrecked cuts that carry a clean exchange, the chain displaced forwards immediately precedes the chain displaced backwards in the cyclic order of lags from the hole — one in a hundred and thirty thousand under a coin, and unaffected by the labelling convention it is stated in.

The account it fits is a shift by one place rather than a swap, and the test that would show it to be a property of handedness rather than of labelling is thirty mirrored runs that have not been made.

What links here

Computed from the collection, not written here: the essays that point at this one.

Shares its objects with

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

  • The alternation is not a period — both name ablation, claim testing, control, honest limits, lattice offset, measurement, negative result, null model, resolution, rigid hop
  • The offsets that never change — both name ablation, census, claim testing, control, honest limits, lattice offset, measurement, negative result, resolution, rigid hop
  • Two regimes above a hole — both name ablation, claim testing, control, description versus mechanism, honest limits, measurement, mechanism, negative result, resolution, rigid hop
  • Every rise of a band — both name ablation, claim testing, control, honest limits, lattice offset, measurement, negative result, resolution, rigid hop
  • The plateau was a prediction — both name ablation, claim testing, control, description versus mechanism, honest limits, measurement, negative result, prediction, rigid hop
  • The rung that two organs wreck — both name ablation, claim testing, control, lattice offset, measurement, mechanism, negative result, prediction, rigid hop

Named objects

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

AblationCensusClaim testingControlDescription versus mechanismHandednessHonest limitsLattice offsetMeasurementMechanismNegative resultNull modelPredictionResolutionRigid hopSlip