Stems and cones

A stem on the other branch

Every arrangement this collection had cut an organ out of carried Fibonacci counts, which is why two rival explanations of the block a wrecked stem settles into had never disagreed. A stem seeded on the Lucas lattice carries four and seven at the same rise, under the same rule. Cut, it settles on seven — the larger number, and not a Fibonacci one.

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

The placement rule has more than one lattice available to it at a given rise, and which one a stem sits on is decided by what it was started from. The famous family is the Fibonacci one — 2/3, 3/5, 5/8, 8/13, walking down as the rise falls — and it is what a stem seeded near 137.5° stays on. The other family this collection has computed is the Lucas one: 1/3, 3/4, 4/7, 7/11, 11/18, reached from a seed near 99.5°, and known from real plants, if uncommonly.

The Lucas branch has been used here as a curiosity and as an example of metastability. This essay uses it as an instrument. Two accounts of what a wrecked stem settles into agree on every Fibonacci rung and disagree wherever the counts are not Fibonacci, and 4/7 is the cheapest place to look.

The control comes first

An intervention on a Lucas stem is only a measurement about a Lucas lattice if the stem is still on one when the organ is removed. The rule is free to leave.

One rule, one rise, two branches that stay where they were putThe top 70 organs of two stems grown by the same placement rule at the same rise of 0.013, differing only in the stretch of ideal lattice each was started from. The left one was seeded at the golden angle and settles at 136.781° with the pair 5/8; the right one was seeded on the Lucas lattice and settles at 99.785° with 4/7. Neither drifts towards the other: 0.73° and 0.28° from where each was seeded, over four hundred organs. That is what makes an intervention on the right-hand stem a measurement about a different lattice rather than about a different rule — and 4 and 7 are not Fibonacci numbers, which is the property the experiment needs.golden136.781° · 5/8Lucas99.785° · 4/7seeded at 137.51° and 99.50°, then left to the rulerise 0.013 · scatter 0.239° and 0.101°generated from a stated rule, not drawn to look right
Fig. 1 Two stems grown by the same rule at the same rise, differing only in the stretch of ideal lattice each was started from. Both are shown as their top seventy organs with their two contact families drawn.

At a rise of 0.013 a golden-seeded stem settles at 136.781° and carries 5/8. A Lucas-seeded stem at the same rise, with the same neighbourhood, the same exponent and the same azimuth grid, settles at 99.785° and carries 4/7. Neither drifts towards the other: the golden stem is 0.73° from the angle it was seeded at after four hundred organs, and the Lucas one 0.28°, with scatters of 0.24° and 0.10°. Thirty-seven degrees separate them, which is the number the control actually turns on.

That is the whole control and it does two jobs. It says the Lucas stem is on the Lucas lattice, and it says the difference between the two runs is the lattice and nothing else — same rule, same rise, one seed.

Which offsets give short hops, at a rise of 0.013The 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.00.2000.4000.600102030index offsetmedian hop between node i and node i+m58300 nodes, 34 offsets triedshortest at 5 and 8
Fig. 2 The golden branch’s own hop table at this rise. The two shortest hops are eight and five organs, which is where 5/8 comes from, with thirteen next.
A stem unrolled: 120 nodes at 99.78° with a rise of 0.013 circumferencesThe counter is shown these coordinates and the circumference, and finds 4 parastichies one way and 7 the other. The faint strips left and right are the same stem: a family leaving one edge re-enters at the other.1 and 3rise 0.106 · divergence 99.78°counted 1 and 3, opposed
Fig. 3 The Lucas lattice at the same rise, unrolled. The counter is shown these coordinates and the circumference and finds four one way and seven the other; nothing in the picture or the count is Fibonacci.

What the two accounts predicted

Both accounts of the block start from the same observation: a stem cut in the middle of its front never returns to its divergence, and settles into a repeating cycle of angles.

One says the cycle carries a count of the lattice that was cut — whichever count that is. On a 4/7 lattice it predicts four or seven.

The other says the cycle is a two-jugate arrangement whose repeat is the count of the ordinary lattice underneath it, which on a Fibonacci rung is the smaller number and which has no natural extension to 4/7 except by way of the smaller number again. It predicts four, and it predicts that the orbit precesses by one part in twice its block.

The block a wrecked stem settles into is the count it was cut fromA 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.5/8 rungblock of 5-36.1° a blockand again208.8° on average8/13 rungblock of 8+22.5° a blockand again182.8° on average300 organs after the cut · 1536 azimuthsgenerated from a stated rule, not drawn to look right
Fig. 4 What the accounts were both built on. Blocks of five and eight on the Fibonacci branch, each precessing by one part in twice its own block.

What the Lucas stem does

Five offsets fail to repair, out of the nine tried, and four of the five settle on a block of seven.

The motif is a hundred and fifty-five degrees wide, so it is an orbit and not a grid artefact. The effective divergence is 151.14° at three of the four offsets and 202.57° at the fourth, precessing by −22.04° in every case. The fifth unrepaired offset, four places back, settles on a block of four at 189.96°.

The block is one of the two numbers, and not always the smallerEvery 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.13579111315golden, rise 0.020pair 3/5golden, rise 0.013pair 5/8golden, rise 0.008pair 5/8golden, rise 0.005pair 8/13Lucas, rise 0.020pair 4/7Lucas, rise 0.013pair 4/7block, in organs — open ticks are the lattice's own pairfilled dark where the block is the larger of the pairone organ removed · 400 organs before the cutgenerated from a stated rule, not drawn to look right
Fig. 5 Every lattice cut, with the blocks its unrepaired offsets settled into. The two Lucas rows are the last two; the open ticks are four and seven, and most of the filled dots sit on the seven.

So the block is seven at four offsets of five: a count of the lattice, the larger of the two, and not a Fibonacci number. The count-of-the-lattice account survives; the reading that the answer is the smaller number does not, and neither does anything that requires the block to belong to the Fibonacci sequence.

Why 4/7 is the right lattice to ask on

The choice of arrangement is doing work and is worth defending, because a comparison between two lattices that differ in several ways at once decides nothing.

Four and seven are coprime, so the lattice is genuinely single-jugate: it is not an ordinary lattice seen twice over, and the repeat-unit account cannot appeal to a hidden smaller lattice underneath. That distinguishes this test from the bijugate one, which asks a different question with a different answer.

Four and seven are also not Fibonacci, and neither is their ratio anywhere near the golden one — 7/4 is 1.75 against 1.618. So an account that predicts a Fibonacci block, for whatever reason, has somewhere to fail here, and an account that predicts the smaller number has somewhere to be distinguished from an account that predicts a number of the lattice.

And 4/7 is available at the same rise as 5/8, which is the part that costs nothing and is worth the most. Rise sets the spacing between organs, the depth of the neighbourhood the rule sums over, and the number of organs in the front; a comparison between two lattices at two rises confounds all of that with the lattice. Here the only difference between the two runs is eight seed organs.

four limit divergences, all of them 137.5078 over a whole numberThe golden angle is the k = 1 member of a family. Real bijugate plants — teasel, *Cephalaria* — are reported near 68.75°, which is exactly half of it, and the pairs they are counted at are the Fibonacci pairs doubled.1-jugate137.5078°counts 3/52-jugate68.7539°counts 6/103-jugate45.8359°counts 9/154-jugate34.3769°counts 12/20limit divergence4 jugacies137.5078 / k
Fig. 6 The angles the rule’s branches converge on, for context. The Lucas branch’s limit is one of the arrangement’s own attractors rather than a perturbation of the golden one, which is why a stem placed on it stays.

And the two-jugate relation misses

The second half of the repeat-unit account is a relation between two independently computed numbers: the orbit should precess by 360 divided by twice its block. A block of seven should therefore turn by 25.71° and give fourteen rows.

It turns by 22.04°, which is 16.33 rows. That is a fifteen per cent miss on a quantity that had agreed to a part in a hundred at both Fibonacci measurements — 10.04 rows on a block of five, 16.00 on a block of eight.

The miss is not universal. The same Lucas stem cut at a coarser rise, 0.020, gives a block of four precessing by 44.07°, which is 8.17 rows against eight: the relation holds there. So twice the block is what these orbits usually are and not what they must be, and a relation that fails on a lattice chosen because it was different is a relation that was never being tested.

One rule, one rise, two branches that stay where they were putThe top 70 organs of two stems grown by the same placement rule at the same rise of 0.02, differing only in the stretch of ideal lattice each was started from. The left one was seeded at the golden angle and settles at 136.875° with the pair 3/5; the right one was seeded on the Lucas lattice and settles at 101.758° with 4/7. Neither drifts towards the other: 0.63° and 2.26° from where each was seeded, over four hundred organs. That is what makes an intervention on the right-hand stem a measurement about a different lattice rather than about a different rule — and 4 and 7 are not Fibonacci numbers, which is the property the experiment needs.golden136.875° · 3/5Lucas101.758° · 4/7seeded at 137.51° and 99.50°, then left to the rulerise 0.02 · scatter 0.000° and 0.161°generated from a stated rule, not drawn to look right
Fig. 7 The same two branches at the coarser rise, where the Lucas stem still carries 4/7 and the golden one has dropped to 3/5. The Lucas branch keeps its pair over a wider stretch of rise than the golden one does, which is why the same pair can be cut at two rises.

Why the larger number, here

The honest answer is that this collection does not know, and the shape of the ignorance is worth setting out.

On the golden branch the block is the smaller number at three rises and the larger at one, and where both appear the offset decides. On the Lucas branch it is the larger at four offsets and the smaller at one. Pooling the two branches, eleven unrepaired offsets give the smaller number and seven give the larger, and there is no lattice property that separates them — the same lattice gives both.

What is left is the offset, and the offset is where an explanation would have to start. A vacancy k places back removes a member of the k-family, and the obvious guess is that the surviving family sets the period. It is refused by the arithmetic: at the Lucas arrangement the offsets giving seven are three, five, six and seven, and the offset giving four is four. Three and six are not multiples of four, and four is not a multiple of seven.

The next organ moves for the last 8, and for no othersOne row per organ removed, counted back from the tip of a stem at a rise of 0.013 whose counted pair is 5 and 8. Removing any of the last 8 moves the next organ by 4.9° to 164.1°; removing an older one moves it by at most 0.70°, which is under the azimuth grid. The boundary is at 8, and 8 is the larger parastichy number — so the experiment counts the spirals without measuring an angle.organ removed, counted back from the tiphow far the next organ moves, in degrees1136.9°286.0°348.3°4164.1°526.2°692.3°7131.0°84.9°— the front ends here90.0°100.7°110.7°120.0°130.7°140.0°150.2°160.2°rise 0.013 · pair 5/8generated from a stated rule, not drawn to look right
Fig. 8 The displacement of the next organ against which organ was removed, on the golden branch at this rise. The run of large displacements ends at eight, the larger parastichy number; on the Lucas stem the same measurement ends at seven, which is that lattice’s larger number.

The front behaves, which is the reassuring part

Everything above is about what happens after the pattern fails to repair, and it is worth separating from the result the intervention was built for.

On the Lucas stem the run of felt offsets ends at seven, which is the larger parastichy number of the lattice it carries. Removing the organ eight places back moves the next one by half a degree; nine places back by nothing measurable. The count-from-a-yes-or-no result therefore holds on a branch it was never tested on, and it holds with a different number, which is a much better test of it than a repetition on the Fibonacci branch would have been.

On a rung the response is a run of offsets; near a transition it has a holeOne row per rise, from 0.02 at the top to 0.008 at the bottom, and one column per offset: the organ one place back at the left, twelve places back at the right. A cell is filled where removing that organ moves the next organ by more than 2.5°, and empty where it does not. On a rung the filled cells are a run from one to the larger parastichy number — 8 at the pairs shown on the left. Between a rise of 0.02 and 0.008 the run ends at 5 and one more cell is filled at 7, with the offsets between them quiet to under a degree. That isolated column is one place inside the larger number of the pair the stem is climbing towards.riseorgans back from the tip →run · isolated246810120.023/55 · 70.0135/880.0085/88 · 123 rises · 1536 azimuthsgenerated from a stated rule, not drawn to look right
Fig. 9 The same measurement on the golden branch across three rises, for comparison. The boundary is the larger parastichy number at each of them, and the Lucas stem’s boundary is its own larger number in the same way.

Where the branch came from

The Lucas lattice is not an invention for this experiment. It is one of the branches the placement rule’s own bifurcation structure supplies, reached by seeding a stem on a Lucas arrangement and lowering the rise slowly enough for the pattern to keep it — this collection measured the threshold at somewhere between eighty-seven and ninety-one organs per rung, with a golden-seeded control ending on Fibonacci at every rate.

It is also on the tree of forks the rule’s maximin criterion generates, where keeping the larger count at each fork converges on the golden angle and one different choice at the first fork converges on 99.502°.

Two paths down the same treeBoth start at the same first fork. Keeping the larger family every time reaches 137.473°; one different choice reaches 99.549°. Neither angle is in the arithmetic — both are limits of a path.100120140-3-2-1log₁₀ of the rise at the forkdivergence angle at the fork (°)137.508° — Fibonacci99.502° — Lucas13 forks, each solved for three equal families137.4730° and 99.5495°
Fig. 10 Where the branch comes from. The tree of exact forks the geometry supplies, with the golden path and the one that leaves it at the first fork. The lattice cut in this essay is a member of the second.
One seed, two rates, two laddersBoth stems begin as forty nodes of Lucas lattice at a rise of 0.12. At 65 nodes per rung the divergence stays at 99.5° and the counts walk 1/3 → 3/4 → 4/7 → 7/11. At 131 it leaves for 137.7° and walks 1/3 → 2/3 → 3/5 → 5/8 → 8/13 instead.10011012013014011.502falling rise, as −log₁₀divergence the stem is producing (°)137.51°, Fibonacci99.50°, Lucas65/rung → 7/11131/rung → 8/13seeded at 99.50°, rise 0.127/11 against 8/13
Fig. 11 How a Lucas seed is kept or lost. The same starting arrangement grown at two rates: the slower run abandons the branch for the Fibonacci one and the faster keeps it, which is what makes the branch metastable rather than stable.

That history matters for reading the result. The Lucas stem is not an artificial lattice built to order; it is a state the rule reaches on its own from a plausible starting condition, and a stem sitting on it behaves in every other respect like a stem sitting on the Fibonacci branch.

Every transition as the rise fallsThe 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 0.3820.0.4000.6000.8001-2-1.50-1log₁₀ of the rise between nodes (falling to the right is the plant growing)log₁₀ of the larger parastichy number2/33/55/88/13500 rises, shortest vectors recomputed at eachratio 0.3819 against 1/φ² = 0.3820
Fig. 12 The Fibonacci ladder for reference, drawn from the geometry. The other branch has a ladder of its own with the same geometric spacing and different numbers on the rungs, which is why a rise can be chosen in the middle of one of its rungs with the same care the Fibonacci ones are chosen with.

What an experiment on a 4/7 shoot would settle

The measurement suggests a specific and unusually cheap addition to the ablation proposal this collection has been assembling.

The proposal so far is: find a shoot, count its parastichies, remove one primordium at a stated offset, and record whether the next primordium moves. Done across offsets it returns the larger count without a protractor. What the Lucas result adds is that the experiment is worth doing on a Lucas shoot as well as on a Fibonacci one, and that the two are distinguishable in advance by counting.

The reason is that the two branches make the same structural prediction with different numbers. A 4/7 shoot should be sensitive out to seven and quiet at eight; a 5/8 shoot sensitive out to eight and quiet at nine. Two shoots on the same plant at the same stage, differing only in which branch they are on, should give different boundaries — and that is a much harder pattern to produce by accident than a single boundary that happens to match a count.

Lucas phyllotaxis is uncommon and it is not rare. It is reported in a handful of genera, it is what the census of divergence angles puts in the second-largest bucket after the Fibonacci one, and a survey that recorded the pair rather than assuming it would find some.

What a divergence picked at random gives, at a rise of 0.008Fibonacci pairs take 14.6% of the circle at this rise, and the share falls as the rise does. The claim that Fibonacci counts are what nature "prefers" needs the preference to come from somewhere, and it is not from the geometry being generous.Fibonacci14.6%Lucas1.4%whorled35.4%other48.6%48 distinct pairs over 1200 divergencesrise 0.008Fibonacci 14.6%
Fig. 13 How often the geometry hands over each pair at a fine arrangement. The Fibonacci pairs are a minority of the circle and the Lucas ones are a smaller minority of it — which is the arithmetic reason a Lucas shoot is uncommon rather than impossible.

What this does not say

It does not say Lucas stems behave differently in general. The front is the larger count, the unrepaired band is in the middle, the orbits are exact — every structural statement this collection makes about ablation holds here. What differs is the number that comes out.

It does not say the block is always the larger number off the Fibonacci branch. One offset of five gives four, and at a coarser rise on the same branch both unrepaired offsets give four. The claim is that the smaller number is not the rule, not that the larger one is.

It does not say the two-jugate relation is dead. It holds at three of the five lattices measured, and misses at two. A relation with that record is a tendency in need of a condition, and this essay supplies neither.

And it does not say anything about a plant with Lucas phyllotaxis. These are stems grown by a rule. What the measurement licenses is that an ablation experiment on a 4/7 shoot is a different measurement from one on a 5/8 shoot, and worth doing for that reason.

One number worth keeping separate

It is easy to let a result about what a wrecked stem becomes contaminate the result about what a healthy one reports, so the separation is worth restating at the end as well as the middle.

The Lucas stem’s front is seven. That is the larger of its two counts, it is obtained without a protractor, and it is the third branch-and-rise combination the boundary has been checked at. Nothing in the argument about blocks touches it, because the boundary is measured on the organ placed immediately after the cut and the block is measured three hundred organs later.

The blocks are the open question, and they are open in a way that is now much better specified than it was: the answer is one of two known numbers, both accounts that predicted which one have been refuted on some lattice, and the quantity that decides it is the offset. That is a smaller claim than the one this thread started with and it is a claim that has survived being taken somewhere new.

The check that would refuse it

Three assertions run whenever these figures are drawn.

The first is the control: each stem settles within a few degrees of the lattice it was seeded on, the two are tens of degrees apart, and they carry different pairs. The “few degrees” is deliberately loose and the separation is not — a branch approaches its own limit angle only as the rise falls, so the Lucas stem sits 0.28° from 99.50° at a rise of 0.013 and 2.26° from it at 0.020, while being thirty-seven degrees from the golden branch at both. A Lucas seed that drifted onto the Fibonacci branch would fail it, and would turn every number in the essay into a number about 5/8.

The second requires every block the Lucas stem settles on to be one of its own two parastichy numbers, and requires the larger to be at least as common as the smaller. That second half is the essay’s claim; the first half is the account that survives, and a block of six or eleven would refuse both.

The third requires at least one orbit whose precession is not one part in twice its block. It exists because the alternative — quietly reporting the ones that fit — is the failure mode of a relation that holds most of the time, and because the sixteen-and-a-third rows are the most specific thing in the essay.

Shares its objects with

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

  • The stem that changed hands — both name ablation, attractor, counting blind, honest limits, initial condition, lattice, measurement, parastichy pair, the placement rule, rise, rung
  • The block is the count it was cut from — both name ablation, attractor, counting blind, honest limits, lattice, measurement, parastichy pair, the placement rule, rise, rung
  • The pattern the cut leaves behind — both name ablation, attractor, counting blind, honest limits, jugacy, lattice, measurement, parastichy pair, the placement rule
  • A cut of two organs — both name ablation, honest limits, lattice, measurement, parastichy pair, the placement rule, rise, rung
  • A front with no middle — both name ablation, honest limits, lattice, measurement, parastichy pair, the placement rule, rise, rung
  • The response with a hole in it — both name ablation, counting blind, honest limits, measurement, parastichy pair, the placement rule, rise, rung

Named objects

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

AblationAttractorCounting blindBranch selectionHonest limitsInitial conditionJugacyLatticeLucas numbersMeasurementMetastabilityParastichy pairThe placement ruleRiseRung