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.
The test takes one measurement, and it is not a count.
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.
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.
Fig. 2 Stems grown at one, two and three organs per node. The symmetry is visible and the counts scale with it, which is why the two are usually treated as the same statement.
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.
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.
Fig. 4 For contrast, what a counter does with the same positions: follows chains of near neighbours and reports how many chains there are. It never asks what happens under a rotation.
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.
Fig. 5 The whorled rule at work rather than assumed: each organ of a whorl placed against what is already there, with the symmetry left to emerge.
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.
Fig. 6 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.
Fig. 7 The negative control, unrolled. One organ per height, so a rotation by any fraction of a turn has nothing to land on.
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.
Fig. 8 The object the measurement is made on: positions, and nothing else. No angle, no history, no record of what was removed.
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.
Fig. 9 The edge in question. At the ends of any finite pattern a rotation has no partner, whatever the pattern’s symmetry is.
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.
Fig. 10 The surface the lookup has to live on, and the reason: a stem has a seam, and the neighbours of a point near it are on the other side of it.
Fig. 11 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.
Fig. 12 The counter checked against a whorled pattern it is shown deliberately: the pair is recovered and so is the divergence, so the instrument is not failing to see jugacy when jugacy is there.
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.
Fig. 13 The reason that is the expected answer rather than a surprising one: nothing in the placement changes when organs are removed. One organ, one height, one minimum.
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.
Fig. 14 The arithmetic the true half of the inference lives in: a k-jugate pattern’s pairs are an ordinary pattern’s pairs multiplied through, all the way down.Fig. 15 And the census that shows the converse has room to fail in: which pairs appear at which divergences and which jugacies, with shared factors reachable from more than one direction.
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.
Fig. 16 The empirical fact the reversal rests on: swept across the rises, the pairs an ordinary stem gives are coprime everywhere.
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.
Fig. 17 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.
Fig. 18 Where the rule of thumb comes from and where it stops: the pair a counter returns as the divergence is swept, with the shared factors appearing at particular angles rather than everywhere.Fig. 19 And why those angles are where they are: the fractions with small denominators are the places a few consecutive steps nearly close, and they are sparse.
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.
Fig. 20 What would have to line up: every organ paired with another at a half turn’s remove and nearly the same height, throughout the run.
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.
Fig. 21 The arrangement the wrecked stem would have to be approaching, at a rise where organs really do pair off.Fig. 22 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”.
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.
Fig. 23 The evidence that a destination is a destination: after the transient, a fixed sequence of divergence angles repeating without end rather than a wander.Fig. 24 The pair extracted from the angles alone, as a cross-check on the pair extracted from the positions. Two instruments, and they agree on undisturbed stems.
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.
Fig. 25 The general shape of that: which state the rule settles into depends on where it starts and what it is disturbed by, and the reachable states are not all the stable ones.Fig. 26 And the states the rule can hold at all, laid out. The destinations of a cut are among them; the ones it arrives at unaided are a much smaller set.
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.
Fig. 27 The census the closure is set against: which jugacies the whorled rule produces at which rises, none of which the ordinary rule reaches at any divergence.
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.
Fig. 28 The six destinations again, with the three that count with a factor marked above the axis and the three that do not marked below.
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.
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
Three organs and no mirror— both name ablation, counting blind, control, falsifiability, honest limits, lattice, measurement, parastichy pair
Two accounts of one number— both name ablation, counting blind, honest limits, jugacy, lattice, measurement, negative result, parastichy pair
A period that is not a count— both name ablation, counting blind, falsifiability, honest limits, lattice, measurement, parastichy pair