Where the angle comes from

The side the census sat on

Eight of the ten lattices the ablation census wrecks at were grown past their rung's handover, one before it, and one so close that the ordering it quotes differs by parts in a thousand. A reading scored over the step ordering was therefore scored against a quantity the census was nearly holding fixed.

Worth reading first: The survey this site cannot do · The organ that was taken away · A head is a set of points.

The ablation census is twelve lattices. Ten of them produce at least one stem that never repairs after an organ is removed, and those ten contribute thirty wrecked cuts between them. It is the table on which nearly every reading in this thread has been scored, and it was built to span the counted pairs and both branches, which it does: five pairs, two branches, rises from 0.032 down to 0.005.

Once each row carries the fraction of its own rung it was grown at, a property of the table appears that was invisible while the rise stood alone. Eight of the ten wrecking lattices sit past their rung’s handover. One sits before it. And one sits so close to a handover that its two contact steps differ by two and a half parts in a thousand, which is a lattice where the words shorter and longer mean nothing at all.

The column the census never carried. One row per lattice the ablation census was grown at. The bar shows where inside its own rung that rise sat, measured in the logarithm of the rise because the ladder is geometric, with zero the coarse transition and one the fine one. The mark on each bar is that rung's own handover, the rise where the two contact steps change places. Of the ten lattices that ever wreck, eight sit past their handover and one sit before it, with one sitting so close to one that the two steps differ by parts in a thousand. The rise was recorded in every table this collection has published; this fraction was in none of them.
Fig. 1 The ten lattices that wreck, each on its own rung, with the handover marked and the side each one fell on.

Counted by cuts rather than by lattices, because a lattice with five wrecking offsets contributes five rows to any score: twenty-five of the thirty wrecked cuts were made past the handover.

What that does to a reading

The reading in question is that a wrecked stem keeps its shortest hop. It came out of the mechanism, which minimises a sum of inverse powers of distance and so ought to hold its nearest neighbours hardest, and it was scored at twelve of thirty and refused.

The refusal stands. What the position column changes is what the twelve was evidence of.

The readings, and where in their rungs they fail. Each bar is one candidate account of which family a wrecked stem keeps, scored across every wrecked cut in the census. Under each bar are the positions inside their own rungs of the cuts it gets wrong, as percentages from the coarse end. The best of them is right 25 times of 30, and the positions of its failures are the point: two of them are the single lattice grown at the far fine end of its rung, which is also the only census row past three quarters of the way down. Nothing here rescues a reading. What it shows is that the table these readings were scored on varies a quantity nobody chose, over a range nobody stated.
Fig. 2 Every candidate account of which family survives, scored across the census, with the position of each failure.

Past a handover the shorter step belongs to the larger of the two counted families. So on twenty-five of the thirty rows, “the shortest hop survives” and “the larger family survives” are the same prediction. The census scores them at twelve and eleven, and those two numbers are close because on five-sixths of the table they are one number.

That is not a defect in the arithmetic of the score. It is a statement about what a score on this table can distinguish. Two readings that agree on twenty-five of thirty rows cannot be separated by more than five rows, whatever they say about the mechanism, and five rows is not a lot of evidence to hang a distinction on.

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. 3 The census itself, whose rows carry a ranking and did not carry the side.
Which lag survives, at every lattice and every offset. A row for each of twelve lattices and a column for each offset an organ is removed at, with the lag whose hop survived written in the cell. 30 cells never repair. The lag left standing is one of the two contact families at 29 of them, and at 17 it is the second shortest step on the lattice rather than the shortest, which is what refuses the reading that a rule holds its nearest neighbours. The ringed cells are the five the offset rule gets wrong. Two lattices carry no cells at all because no single removal wrecks them.
Fig. 4 The same table as a grid, with the reading that scores best marked on it.

How much a five-row difference can carry

It is worth doing the arithmetic rather than gesturing at it, because “only five rows” is the kind of phrase that can be used to dismiss anything.

Thirty cuts, of which twenty-five agree between the two readings and five disagree. On those five, the shortest-hop reading is right once and the larger-family reading is right none of the times — a difference of one row. A census of this size cannot resolve a difference of one row: with thirty binary outcomes, two readings differing by one are indistinguishable by any standard this collection would accept, and by most it would not.

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 Every wrecked cut, with the family kept and the ranking it sat in, which is the table the readings are separated on.

So the honest statement about the shortest-hop reading, after the correction, has two halves. It is wrong — twelve of thirty is far from thirty of thirty, and the rows it fails on are not close calls. And it is wrong for reasons this table cannot fully attribute, because on most of its rows it is not making an independent prediction at all.

That distinction is not pedantry. A reading that fails because the mechanism does not work that way is a dead end; a reading that fails because it was tested against its own restatement is an untested reading. Only the first is a result, and the census on its own cannot say which of the two happened.

Both vary; only one of them varies enough to find. Each 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.
Fig. 6 The general form of the problem, drawn once for this collection: what a design can distinguish and what it cannot.

Why the census landed there, and why any census would

The obvious question is whether somebody chose badly, and the answer is that nobody chose at all — and that a person choosing sensibly would land in the same place.

A census row starts with a pair. Wanting a stem counted at five and eight, a person picks a rise that reliably gives five and eight, which means a rise comfortably inside the rung rather than near either boundary, because near a boundary the two candidate pairs have nearly equal steps and the counter’s answer is a decision about a near-tie. So rises get picked near the middle of their rungs.

The golden ladder, rung by rung. Each bar is one rung — a run of rises over which a counter returns one pair — drawn from its coarse end on the left to its fine end on the right, with the whole bar scaled to the same width so that positions inside different rungs can be compared. The mark on each bar is the rise at which the two contact steps change places, and it falls between 12 and 35 per cent of the way down on every rung that has one. The dots are the lattices this collection's ablation census was grown at, dropped onto the rungs they belong to. They are not spread across the bars; seven of them sit past the mark.
Fig. 7 The golden branch’s rungs with the census’s own rises on them, which cluster where a person picking a safe rise would put them.

And a handover is always in the coarse half — six of six on this ladder, at six to forty per cent. A rise picked near the middle of its rung is therefore past the handover as a matter of course. The sampling is not a mistake anybody made; it is what the sensible procedure produces, given a fact about the ladder that nobody had measured.

Where a rung's handover sits, over six rungs. The rise at which the two contact steps change places, as a fraction of the way down each rung from its coarse end, over every rung on both branches that has one. All six fall in the coarse half and none in the middle: the positions measure 6, 12, 15, 33, 35, 40 per cent. That is a fact about the arithmetic of the lattice rather than about any experiment run on it, because the crossing is where the two step lengths are equal and both are functions of the rise and the divergence alone.
Fig. 8 The fact that makes it inevitable: every measured handover in the coarse half of its rung.

That is worth separating from the more usual kind of sampling complaint. The census is not unrepresentative of the lattices somebody cared about; it is unrepresentative of a quantity nobody knew was a quantity. The correction is not “choose better rises” but “record the side, and if the reading is about the ordering, straddle a handover on purpose”.

The one row on the other side, and the one row with no side

Two rows are worth naming individually, because with only ten lattices each of them carries a tenth of whatever the table can say.

The lattice at a rise of 0.016, counted 5/8, sits at twelve per cent of its rung — just above the handover at fifteen. It is the only wrecking lattice on the coarse side, where the shorter step belongs to the smaller family. It wrecks at exactly one offset, and the family it keeps is the five.

Which offsets give short hops, at a rise of 0.018. The two lowest points are at 5 and 8, 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.
Fig. 9 The step ranking at the coarse end of that rung, where the smaller family has the shorter hop.

That single row is the whole of the census’s evidence about the coarse side. One cut. It is consistent with the shortest-hop reading and with the smaller-family reading and with the offset rule, all three, and it distinguishes none of them.

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. 10 What one such row is: a stem, an organ taken out of it, and a comparison against a control that shares its history.

The lattice on the Lucas branch at 0.008, counted 7/11, sits at thirty-three per cent of its rung — which is, to three decimal places, where that rung’s handover is. Its two contact steps differ by two and a half parts in a thousand. Any statement about which of them is shorter is a statement about the fourth significant figure of a quantity measured on a grid of 1,536 azimuth steps, and this collection’s own tolerance for calling two steps ordered is one per cent.

Which offsets give short hops, at a rise of 0.008. The two lowest points are at 5 and 8, 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.
Fig. 11 Two steps that close to equal: the ranking exists, and nothing should be built on it.

That row contributes four of the thirty cuts. It has been scored in every table here as though its ordering meant something, and it does not. Marking it as unordered rather than dropping it is deliberate: dropping rows that inconvenience a reading is how a score gets made true, and the four cuts are perfectly good evidence about everything except the ordering.

What survives the correction

Most of the thread, and it is worth being specific about which parts and why.

That the survivor is one of the two contact families is untouched. That reading is about which lags exist, and the counted pair fixes those; the ordering between them is not in the claim.

A cell's neighbours are its spiral families. Left: part of a 700-point golden, 137.508° head, with every contact between two cells drawn and coloured by the difference between the two nodes' placement indices. Right: the share each difference takes, across all 1459 contacts between interior cells. They are the parastichy numbers — 34, 55, 21, 89, 13, 8 — and the pair a person would count is 34 and 55. The six sides Euler forces are shared out among four of them, 5.64 edges per cell.
Fig. 12 Why that one is robust: the organs an organ touches are the members of its two contact families, whichever of them has the shorter step.

That a wrecked stem keeps exactly one hop rigid is untouched for the same reason, and more strongly: it is measured against each stem’s own control, so it makes no comparison across lattices at all.

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. 13 The measurement that reading rests on, which is a comparison inside one pair of runs.

The offset rule — the smaller count while the cut lands no further back than it, the larger beyond — is scored at twenty-five of thirty, and the position column does not move it. Its five failures sit at eighty-nine, eighty-nine, nineteen, sixty-six and thirty-three per cent, which is a spread rather than a cluster: two of them are the single lattice at the far fine end of the 8/13 rung, one is the unordered Lucas row, and two are the pair of runs that closed the class.

The offsets where the removed organ belonged to one family. Each row is a stem that never repaired, with the family of the organ that was taken and the family that survived. An organ five places back on a stem counted at 5 and 8 spirals lies on the tip's five-chain, so the question can be asked there; an organ four places back lies on neither chain and it cannot. Of 30 wrecked offsets in the census, 9 remove a member of exactly one family and 21 remove a member of neither. On every one of the 9 the family that lost a member is the family left standing, which is the opposite of what the reading predicted.
Fig. 14 The other reading scored on the same rows, which is about whose neighbour was removed rather than about which step is shorter.

What does not survive is the strength of the case against the shortest-hop reading. Twelve of thirty on a table that is nearly one-sided is weaker evidence than twelve of thirty on a balanced one, and this collection said the first while sounding like the second.

The experiment the correction implies

If a census cannot distinguish the ordering from the family, then the way to test the ordering is to hold everything else and move only that — which is what a handover is for. Grow a band of rises around one, where the pair is constant and the divergence is held to a twentieth of a degree, and cut at every offset on both sides.

A divergence that does not move across the 5/8 band. Measured at every rise of a band on the golden branch, where a counter returns 5 and 8 spirals throughout. The settled divergence moves by 0.0469 degrees across the whole band, which is a fraction of the azimuth grid step and a fortieth of the slide across the rung it sits in. The ratio of the two contact steps does move: it falls to 1.0013 and the ordering changes hands at a rise of 0.0156, so above that rise the shorter step belongs to the 5 family and below it to the 8 family. Two of the three quantities that vary along a rung are therefore held here and the third is not, which is what makes the ends of this band a matched pair.
Fig. 15 The band, on the golden branch: a run of rises whose settled divergence does not move.
The ordering changes and the survivor does not. Every offset that wrecks, at every rise of the band, with the family left standing written in the cell. The counted pair is 5 and 8 at all 18 rises and the settled divergence is held to a twentieth of a degree, so the one quantity moving across the columns is which of the two contact steps is the shorter — and it changes hands at the marked rise. The cells do not: the 5 family survives at all 24 wrecked cuts, on both sides. Scored on this band, the reading that a wrecked stem keeps its shortest hop is right 14 times out of 24, for an answer that never changed.
Fig. 16 And the ablation across it, with the family that survives written in every cell.

Done on two bands, on two branches, at fifty-five wrecked cuts: the survivor does not change while the ordering flips underneath it. That is the test the census could not run, and it answers the question the census could only gesture at.

Both bands, on two branches and two pairs. One row per band. Each runs from its coarse end on the left to its fine end on the right, with the rise at which the two contact steps change places marked, and the family that survives every wrecked cut written at the end. The 5/8 band on the golden branch keeps the 5 at all 24 of them and the 4/7 band on the Lucas branch keeps the 4 at all 31. Two branches, two counted pairs, one result: the quantity the band varies is not the quantity that decides the answer.
Fig. 17 Both bands, on two branches and two counted pairs, with the same answer.

It is also a much cheaper experiment than the census, which is the part worth remembering. Thirty-seven stems and a hundred and fifty cuts, all at one rung each, against a census spanning the whole ladder. A design that varies one thing does not need to be large.

The general shape

This is the second time in two rounds that a result here has turned out to be partly about how the tables were built rather than about what they measured. The first was that a census taking one rise per rung samples everything the rise moves; this is the specific version of that with a name attached to the quantity.

What the finer grid does to the rises already published. The 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 earlier work 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.
Fig. 18 An earlier instance of the same shape: a quantity the instrument fixes rather than measures.

Both have the same fix and it is not a methodological principle so much as a habit: before scoring a reading over a quantity, ask what the range of that quantity was in the rows being scored. Here the answer was a range of nearly zero, and it took one column to see.

Every transition as the rise falls. The pair climbs 1/2 → 2/3 → 3/5 → 5/8 → 8/13. Consecutive transitions are 0.381, 0.382, 0.382 of the previous rise — 1/φ² is 0.3820.
Fig. 19 The ladder every one of these rows was drawn from, whose interior structure was not measured until it was needed.

The uncomfortable version is that the census was published, quoted and built on for three rounds before anybody asked. Nothing about the question required new machinery — the hop ranking was already in every row of the table — and what was missing was the idea that a ranking has a place as well as a value.

The block is one of the two numbers, and not always the smaller. Every lattice a single organ was removed from, one row each: golden, rise 0.020 carrying 3/5; golden, rise 0.013 carrying 5/8; golden, rise 0.008 carrying 5/8; golden, rise 0.005 carrying 8/13; Lucas, rise 0.020 carrying 4/7; Lucas, rise 0.013 carrying 4/7. The two open ticks on each line are that lattice's own parastichy numbers; the filled dots are the blocks the stems that never recovered settled into, one per offset that failed. The claim this table was built to test is that the block is the smaller of the two, which held at the two rises it was first measured at. It does not hold here: 3/5 gives 5, 5/8 gives 5 and 8, 4/7 gives 4 and 7. What survives is weaker and still worth something — every filled dot but 1 sits on one of that row's own ticks, so the orbit carries a count of the lattice it was cut from, and which of the two it carries is decided by the offset rather than by the pattern.
Fig. 20 One of the tables built on it, whose own reading is about the pair rather than the ordering and is untouched by any of this.
The block a wrecked stem settles into is the count it was cut from. A stem is cut in the middle of its front and followed for 300 organs. It does not come back to its lattice; what it does instead is repeat a fixed sequence of divergences exactly, to the resolution of the azimuth grid. Each row shows that sequence twice over, one bar per organ, drawn to the same scale. At the 5/8 rung the sequence is five angles long and advances -36.1° per block; At the 8/13 rung the sequence is eight angles long and advances 22.5° per block. Every block is the smaller number of the pair that was cut, so the second attractor carries the first one's count — and every precession is one part in twice the block, which makes each of these a two-jugate arrangement with 10 and 16 rows.
Fig. 21 And the destinations those rows feed, each measured at a rise whose position in its rung is now on the record.

What the correction is not

It is not a retraction. Everything published on this table is still there and most of it is unaffected, which is the ordinary case when a sampling problem is found: the tables were built for a question about the counted pair, they answered it, and a later question turned out to need a coordinate they did not carry.

The spiral counts four different divergence angles produce. Fibonacci counts come from one angle. The Lucas angle — which the same dynamical model reaches on a different branch — gives 47 and 76, and neither number is a Fibonacci number.
Fig. 22 The question the census was actually built for, which it answers as well as it ever did.

It is not an argument for larger censuses. A census of thirty lattices instead of ten, built the same way, would sit past its handovers on twenty-five of thirty rows exactly as this one does, and would carry three times as much of the same one-sidedness. Size does not fix a design; the band experiment fixes it, and the band is smaller.

Every open question here needs under 28 specimens. The sample size at which each comparison reaches 80 per cent power at a 5 per cent false-positive rate, from the exact binomial rather than a normal approximation. The census question — do plants show consecutive Fibonacci pairs far more often than the geometry does — needs 4: 14.7% is the share of divergence angles giving a consecutive Fibonacci pair at a fine rise; 90% is what a grown history gives.
Fig. 23 The arithmetic of sample size, which answers a different question from the one a confounded design has.

And it is not a claim that the position is doing anything causal. Nothing here says a stem grown at eighty per cent of its rung behaves differently from one grown at twenty because of where it sits. The position is a coordinate that happens to correlate with a quantity a reading was stated over, which is exactly what makes it a confound and exactly what stops it being a mechanism.

The distinction matters for what gets recorded. A confound is fixed by a design; a mechanism would be fixed by an explanation, and this collection has neither the explanation nor a reason to think one is owed. What the tables need is the extra column and the occasional band, both of which are cheap. What they do not need is a story about why eighty per cent of a rung is a different place to be, because the experiment that would have supported one found nothing.

What is still open

Whether a census straddling handovers on purpose would find anything the bands do not. The bands are narrow — eighteen and nineteen rises, a few per cent of a rung each — and they hold the divergence by construction. A census that sampled each rung at, say, five per cent, twenty, forty, seventy and ninety would vary the position and the ordering and the divergence together, which is the confound this thread started with, but it would at least have rows on both sides of every handover.

Which family survives, along the 5/8 rung. The family a wrecked stem keeps, at every offset that wrecks and every rise on one rung. A counter shown any of these stems returns 5 and 8 spirals, at all twelve rises, so nothing in the pair distinguishes the columns. The cells say otherwise: at an offset of 4 the stem keeps the 5-family at the coarse end of the rung and the other one at the fine end. The offsets that wreck at all grow from 1 to 5 as the rise falls, because the front deepens, and the extra offsets are the ones that keep the larger number. So the rule stated over the offset alone is a rule with the rise left out of it.
Fig. 24 The nearest thing to that census which exists, which sweeps one rung finely and finds the survivor changing along it.

And whether the same one-sidedness is in the other tables. The front-depth work, the jugacy work and the noise work all grow stems at rises chosen the same way, by the same procedure, for the same reason — so the presumption is that they sit past their handovers too, and the presumption has not been checked row by row. That is an afternoon’s arithmetic on tables already published, which is precisely the kind of debt this essay exists to point at rather than to leave implied. The reason to name it here rather than to quietly do it is that the answer is only interesting if it is written down before the checking starts: the presumption is that they sit past their handovers too, and a presumption recorded in advance is a prediction rather than a summary.

The band that never heals is what two fixed edges leave over. Each row is one rung. A stem is grown to 400 organs, one organ is removed, and the stem is followed for 300 more. A filled mark is an offset the stem recovers from, with the number of organs it took printed above it; an open ring is an offset it never recovers from. At the 3/5 rung, a front of 5, every offset heals. At the 5/8 rung, a front of 8, the offsets 4, 5 never heal. At the 8/13 rung, a front of 13, the offsets 4, 6, 7, 8, 9 never heal. What is the same at every rung is the two edges: the first three offsets heal, and so do the last few of the front. What is left in the middle is the band, and it widens because the front does.
Fig. 25 One of those other tables, whose three rises are three positions as well as three pairs.

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.

  • A stem too fine to settle — both name counting blind, claim testing, control, honest limits, negative result, parastichy pair, rise, rung, underdetermination
  • One rung, two answers — both name ablation, control, honest limits, lattice offset, negative result, parastichy pair, rise, rung, underdetermination
  • The family that lost a member — both name ablation, claim testing, control, honest limits, lattice offset, negative result, parastichy pair, rung, underdetermination
  • The front deepens down a rung — both name ablation, claim testing, control, honest limits, lattice offset, negative result, parastichy pair, rise, rung
  • The organ that was nobody's neighbour — both name ablation, claim testing, control, honest limits, lattice offset, negative result, parastichy pair, rung, underdetermination
  • Two accounts of one number — both name ablation, counting blind, claim testing, honest limits, negative result, parastichy pair, rise, rung, underdetermination

Named objects

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

AblationCounting blindCensusClaim testingControlHandoverHonest limitsLattice offsetNegative resultParastichy pairRiseRungSamplingSelection effectUnderdetermination