The pattern itself

The symmetry that is not there

A wrecked stem counted 2/6 and a stem grown two organs at a time counted 2/6 are indistinguishable to a spiral counter. Rotate them by half a turn and one lands on itself and the other lands nowhere. A cut does not make a whorled pattern; it makes a pattern that counts like one.

Worth reading first: Counting the spirals · A head is a set of points · Two at a time.

Three of the six places a many-organ cut can send a stem are counted at a pair whose numbers share a factor: 2/6, 4/6 and 3/6. A shared factor is the signature of a whorled pattern — one that arrives k organs at a time and therefore carries k copies of every family — and if a cut could produce one, then the property counting is least able to decide would be reachable by damage.

The test takes one measurement, and it is not a count.

Two patterns a counter cannot tell apart — counted 2/6 against 2/6. On the left, the top 90 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. 1 The whole argument in one frame. A wrecked spiral stem on the left and a stem grown two organs at a time on the right, with what a counter says under each and what a rotation says under that.

Jugacy is a property of the positions

Multijugacy is not a fact about numbers; it is a fact about where the organs are. A pattern is k-jugate when rotating the whole of it by a k-th of a turn maps it onto itself — every organ landing on another organ, to within a small fraction of the local spacing.

Two patterns a counter cannot tell apart — counted 4/6 against 2/6. On the left, the top 140 organs of a spiral stem that never repaired after four organs were removed, settling at 189.96 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 4/6 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, 9.96 degrees from 1 of 2 turns, and not about how it grew.
Fig. 2 The same destination followed further up the stem. Two files that never quite pair is what the counts read as a factor of two, and more organs do not make them pair.

That is a different statement from anything a spiral count makes, and this collection has drawn the difference before, on patterns written down from formulas rather than grown: a bijugate lattice and an ordinary lattice at a divergence near half a turn are counted identically and have different symmetry.

Same counts, different patterns. Both are counted 2 and 4 by machinery shown only their positions. Rotating the left one by half a turn maps it onto itself and rotating the right one does not, so the left is bijugate and the right is not — and no count could have said so.
Fig. 3 The distinction demonstrated on two ideal lattices: identical counts, one with a half-turn symmetry and one without.

The measurement is direct. Take the positions, take the median nearest-neighbour distance as the scale, rotate the whole set by 1/k of a turn for every k from two to eight, and ask whether every rotated organ lands within a fraction of that scale of an organ that is already there. The largest k that passes is the order.

Two patterns a counter cannot tell apart — counted 3/6 against 6/9. On the left, the top 140 organs of a spiral stem that never repaired after four organs were removed, settling at 235.00 degrees. On the right, a stem grown by a rule that places three organs at a time on every node. A counter shown the positions returns 3/6 for the first and 6/9 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 third 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, 5.00 degrees from 2 of 3 turns, and not about how it grew.
Fig. 4 The three-at-a-time control read to the same depth. Here the organs really are placed together, which is what a genuine symmetry looks like.

The controls, first

A measurement that never returns anything but one is not a measurement, so the instrument is run on two patterns whose answers are known before it is run on the three in question.

The positive control is a stem the whorled rule actually grew. It is important that it was grown rather than written down: the rule places each organ of a whorl at the minimum of the same profile the ordinary rule uses, with its whorl-mates already in the neighbourhood, so the k-fold symmetry that comes out is a result and not an imposition. A control whose symmetry was built in could not fail.

Grown at two organs per node, at the same rise the cuts are made at, it comes out counted 2/6 with rotational symmetry of order 2. Grown at three, it comes out counted 6/9 with order 3. The instrument sees what is there.

Two patterns a counter cannot tell apart — counted 3/6 against 6/9. On the left, the top 96 organs of a spiral stem that never repaired after four organs were removed, settling at 235.00 degrees. On the right, a stem grown by a rule that places three organs at a time on every node. A counter shown the positions returns 3/6 for the first and 6/9 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 third 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, 5.00 degrees from 2 of 3 turns, and not about how it grew.
Fig. 5 The three-at-a-time control on the right, counted 6/9 with a third-turn symmetry, beside the wrecked stem counted 3/6.

The negative control is the undisturbed stem the cuts are made in. It is counted 5/8 and its rotational symmetry is order 1 — no rotation maps it onto itself, which is what one organ per height means.

How the measurement is made

Worth setting out in full, because a null result stands or falls on whether the instrument could have reported anything else.

The pattern is the top two hundred and twenty organs of a run, taken as points on an unrolled cylinder of circumference one. The scale is the median nearest-neighbour distance, computed from the pattern itself rather than stated, so that a coarse arrangement and a fine one are judged on the same terms.

For each order from two to eight, every point is rotated by that fraction of a turn and asked whether an existing point sits within a small fraction of the scale of where it landed. The largest order at which every point succeeds is the answer.

Two details are load-bearing and both were settled when the whorled rule was written, against patterns whose symmetry was known.

The test is made on the interior of the pattern. The top and bottom rows of a finite point set have nothing to rotate onto, so a test applied to all of it reports order one for everything — including a genuinely bijugate stem — and is a measurement that cannot fail.

And the lookup that finds the nearest existing point lives on the cylinder rather than on a rectangle. A grid keyed on the raw azimuth puts a point at 0.998 of a turn and one at 0.002 in buckets a whole turn apart, so every query near the seam misses — and nine per cent of a spiral pattern lies within a cell of the seam, which is exactly where its neighbours are. That bug once reported a bijugate lattice with eight parastichies in a family as having thirty-one.

The three destinations have order one

All three.

destination counted shared factor rotational symmetry
175.01° 2/6 2 1
189.96° 4/6 2 1
235.00° 3/6 3 1
Two patterns a counter cannot tell apart — counted 4/6 against 2/6. On the left, the top 90 organs of a spiral stem that never repaired after four organs were removed, settling at 189.96 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 4/6 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, 9.96 degrees from 1 of 2 turns, and not about how it grew.
Fig. 6 The second of the three, at 189.96 degrees and counted 4/6, beside the same bijugate control. The counts share a factor of two and only one of the panels has a half-turn symmetry.

The strongest form of the comparison pairs them off rather than reporting the number alone. The stem that settles at 175.01° is counted 2/6. The stem the whorled rule grew at two organs per node is counted 2/6. A counter shown the positions of both returns the same pair and has nothing further to say. Rotated by half a turn, the second maps onto itself and the first does not — not marginally, not at a looser tolerance, not at any order from two to eight.

So a cut does not convert a spiral stem into a whorled one. The rule kept placing one organ at a time throughout, which is what it always does, and the pattern it produced is a one-organ-at-a-time spiral whose two shortest families happen to share a factor.

A third count would decide it too

The rotation test needs positions, and there is a cheaper test that needs only counting — one more family than the two everybody stops at.

A k-jugate pattern carries every family in k copies, not merely its two shortest. So its whole family list is k times an underlying list, and every member of it is divisible by k. A spiral stem whose two shortest families happen to share a factor is under no such obligation: the coincidence is about where two hops landed, and the third family knows nothing about it.

So the test is: count a third family and check whether the factor survives. On the stem counted 2/6 a bijugate reading requires the next family to be even; a spiral reading permits anything. Two numbers cannot separate the hypotheses and three usually can, which is the same shape as the ordered-triple check that caught this collection’s founding miscount — and it fails in the same way, by an addition that does not come out.

That test has not been run on these three destinations, and it should be, because it would make the finding available to somebody with a photograph rather than only to somebody with coordinates. What the rotation test has that it lacks is certainty: a third family that is divisible by k is consistent with jugacy and does not establish it, so the counting test can refuse and cannot confirm.

Where the trap actually bites

The inference this essay refutes is one almost nobody writes down, and it is worth asking why it has survived unwritten — because the answer scopes the finding sharply.

On a stem, jugacy is not inferred from counts at all. It is read off the nodes: a bijugate shoot has two leaves at each node and a spiral shoot has one, and anybody looking at the plant can see which. The counted pair is irrelevant to the classification, so a shared factor arising some other way misleads nobody.

The trap is for patterns with no nodes to look at — a sunflower head, a pine cone, a daisy, any arrangement recorded as a set of positions with no visible record of what arrived when. There the only route to jugacy is through the geometry, and the shared factor is the route people take.

That is not a narrow exclusion. Heads and cones are where most of this subject’s counting is done, they are where the large parastichy numbers live, and they are exactly the specimens whose photographs get counted rather than dissected. So the finding matters precisely where the subject does most of its work, and matters not at all where the inference looks safest.

It also says what a survey should record. A specimen whose counted pair shares a factor needs one further line: whether the pattern maps onto itself under a rotation by a k-th of a turn. That is measurable from the same photograph the counts came from, it needs no dissection, and it is the difference between reporting a whorled arrangement and reporting a spiral one that looks like a whorl from the numbers.

How often the inference would be wrong

The three destinations here are three of three, and that number should not be read as a rate.

They were reached by damage, and damage is what selects for this shape: a cut sends a stem to a divergence near a low fraction of a turn, which is exactly the condition under which a small number of steps closes and the counted pair acquires a factor. A census built out of wrecked stems is a census of the cases where the inference fails, by construction.

What the essay establishes is therefore that the failure rate is not zero, which is the claim a logical refutation makes and the only one three cases can support. How often a real head with a shared-factor pair is a damaged spiral rather than a whorl is a question about plants, and nothing here answers it.

Two things bear on it and point opposite ways, which is why it is worth stating rather than guessing. Against the failure being common: an undisturbed arrangement sits near the limit angle, where no small denominator closes, so an ordinary spiral head will not produce a shared factor by accident. In favour of it being worth checking: the divergences that do produce one are the destinations a disturbance actually reaches, and a head that has lost organs to an insect has had the disturbance.

The measurement that would settle it is not a model run. It is a count of how many shared-factor specimens in a real collection pass the rotation test, and the specification above is what makes it a morning’s work rather than a study.

The inference that fails, stated as an inference

It is worth writing out the step that breaks, because it is a step almost nobody writes down and almost everybody takes.

A pattern with k organs per node has k-fold rotational symmetry. True, by construction.

A pattern with k-fold rotational symmetry has every parastichy family in k copies. True: the rotation carries each family to another family of the same count.

Therefore a pattern whose counted pair shares a factor of k has k organs per node. False. It reverses an implication. Sharing a factor is a consequence of the symmetry and is not equivalent to it, and the three destinations here are exactly the counterexample.

The reason the reversal usually works is empirical rather than logical. Ordinary spiral patterns sit near the golden angle, where no small number of consecutive steps comes back near the start, so an ordinary pattern’s shortest two families are consecutive Fibonacci or Lucas numbers and are coprime. A pair with a factor in it therefore usually does mean a whorl — because the other way of getting one requires a divergence nothing normally arrives at.

A cut is a way of arriving at one.

Why the counter is not wrong

It is worth being careful here, because “the counter says 2/6 and the pattern is not bijugate” reads like an instrument failure and is not one.

The counter’s job is to report the two families of nearest chains in the positions. At a divergence of 175.01° that is exactly what it does: consecutive organs sit almost opposite each other, so the pattern really does have two near-vertical rows of organs and really does have six chains in the other direction. Two and six are the right answer to the question the counter is answering.

Two patterns a counter cannot tell apart — counted 2/6 against 2/6. On the left, the top 140 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. 7 More of the same stem, so the two files are visible as files. The counter is reporting them, and they are there.

What is wrong is the inference. “A pair with a shared factor implies k organs per node” is a rule of thumb that holds across the patterns botanists usually meet, because those patterns sit near the golden angle where no small number of consecutive steps comes back to the start. It fails for a lattice that has drifted somewhere else, and a wrecked stem has drifted somewhere else by construction.

What would have had to be true

Suppose the answer had gone the other way. It is worth being explicit about what that would have meant, because a test whose alternative outcome has no consequences is a test nobody needed to run.

A rotation of half a turn mapping a wrecked stem onto itself would mean that organ i and some organ at nearly the same height sit nearly opposite each other, for every organ in the run. The rule places one organ per height, so the partner would have to be an organ at a different height that happened to land there — and it would have to happen for all two hundred and twenty of them at once, to within a fraction of the local spacing.

There is a rise at which that is nearly true, and it is worth naming because it is the case that makes the test non-trivial. If the rise were small enough that consecutive organs were separated vertically by much less than the local spacing, a stem near half a turn would approach a two-ranked arrangement in which organs really do pair off. The rises here are not small enough — at 0.013 the vertical step is more than a tenth of the spacing — but the failure is quantitative rather than categorical, and a test with a tolerance stated relative to the spacing is what turns that into a number.

Same counts, different patterns. Both are counted 2 and 4 by machinery shown only their positions. Rotating the left one by half a turn maps it onto itself and rotating the right one does not, so the left is bijugate and the right is not — and no count could have said so.
Fig. 8 And the pair of patterns the whole distinction rests on, drawn closer to the case that matters: a genuinely bijugate lattice and an ordinary one near half a turn.

So the null is not “the measurement found nothing”; it is “the measurement found order one where a stated alternative would have given two, on a pattern the alternative’s own signature was extracted from”.

What a wrecked stem is doing instead

Two things are worth saying about the object itself, because “not whorled” is a negative and the positive description is short.

The first is that it is a lattice. The three destinations are settled: the divergence holds to a fraction of a degree over the last hundred and twenty organs, the counter returns a stable pair, and the positions form a proper two-family packing. Nothing here is a stem in the middle of falling apart.

The second is that it is a lattice the rule can occupy and never reaches on its own. Grown from a golden seed at this rise, the rule settles at 136.78° every time; grown from a Lucas seed it settles somewhere else; and nothing in the undisturbed sweep of this collection has ever produced 175.01°. It is a state the placement rule is perfectly happy to sit in and has no route into, except by having something taken out of it.

What this closes and what it opens

It closes the alarming reading. Jugacy is not reachable by damage in this rule, and a specimen counted with a shared factor is not evidence that something was removed from it. The measurement that decides is available on any pattern whose positions can be recorded, and it is one rotation.

It opens a smaller and more tractable question. If the shared factor is a fact about where the divergence landed rather than about how the organs arrived, then the three destinations should have something in common that the other three do not — some property of 175.01°, 189.96° and 235.00° that 136.99°, 208.80° and 280.43° lack.

They do, it is measurable in one line, and getting the measurement right turns out to matter more than it looks — because the obvious version of it reports that the golden angle has five files, which is the exact opposite of the fact the whole subject rests on.

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 survivor has to be a neighbour — both name ablation, counting blind, falsifiability, honest limits, lattice, measurement, negative result, parastichy pair
  • Half a turn, four at a time — both name ablation, counting blind, classification, honest limits, lattice, measurement, negative result, parastichy pair
  • One offset, two answers — both name ablation, control, falsifiability, honest limits, lattice, measurement, negative result, parastichy pair
  • One rise per rung is a sample — both name counting blind, control, falsifiability, honest limits, lattice, measurement, negative result, parastichy pair
  • One rung, two answers — both name ablation, control, falsifiability, honest limits, lattice, measurement, negative result, parastichy pair
  • The family that lost a member — both name ablation, control, falsifiability, honest limits, lattice, measurement, negative result, parastichy pair

Named objects

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

AblationBijugateCounting blindClassificationControlFalsifiabilityHonest limitsIdentifiabilityJugacyLatticeMeasurementNegative resultParastichy pairRotational symmetryWhorled