Where the angle comes from

The ordering was not the actor

Cut an organ out of every rise of a band where the counted pair and the settled divergence are held and the two contact steps change places, and the family left standing does not change. Fifty-five wrecked cuts on two branches, and the ordering reverses underneath every one of them.

Worth reading first: The organ that was taken away · Where a handover sits · A head is a set of points.

When an organ is removed from a stem and the arrangement never repairs, exactly one lattice hop stays rigid: the angle from an organ to the one p places above it is unchanged from the control, organ by organ, while every other lag moves. Which p is a question this thread has been chasing for four rounds.

Two answers have been ruled out and one holds at twenty-five rows of thirty. Ruled out, most stubbornly, is that the survivor is the shorter of the two contact steps — the reading the mechanism suggests, since a rule minimising a sum of inverse powers of distance ought to hold its nearest neighbours hardest. It scores twelve of thirty on the census, and the census turns out to be nearly one-sided in exactly the quantity the reading is stated over, so twelve of thirty is a weaker refutation than it looks.

This essay runs the test the census could not.

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. 1 Every wrecked cut across the golden band, with the family left standing written in each cell and the ordering changing hands in the middle.

The design in one paragraph

A band is a run of rises around the point where the two contact steps change places. Across it the counted pair is held, the settled divergence is held to a twentieth of a degree, the branch is held — and the ordering of the two steps reverses. Two of them were built, one on each branch: golden 5/8 across eighteen rises, Lucas 4/7 across nineteen.

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. 2 The golden band’s divergence, held across every rise the ablation is run at.
The two steps changing places inside 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. 3 And the quantity that is not held: the ratio of the two steps, passing through one at the marked rise.

Cut at every offset of every rise on both, compare each cut run against a control sharing its history to the last digit, and read the rigid lag out of the comparison. That is the same measurement the census makes, made on stems chosen to differ in one thing.

The result

Fifty-five wrecked cuts. On the golden band, twenty-four of them, and the family left standing is the five at every one. On the Lucas band, thirty-one, and it is the four at every one.

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 4 and 7 at all 19 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 4 family survives at all 31 wrecked cuts, on both sides. Scored on this band, the reading that a wrecked stem keeps its shortest hop is right 6 times out of 31, for an answer that never changed.
Fig. 4 The Lucas band, on a different branch and a different pair, with the same shape of answer.

Ten of the golden band’s rises have the five-step shorter and eight have the eight-step shorter. The family that survives is the five on both sides. On the Lucas band, seven rises have the four-step shorter and twelve have the seven-step shorter, and the family that survives is the four on both sides.

So the surviving family is the shorter step on part of each band and the longer step on the rest, and it is the same family throughout. The ordering reverses and the answer does not move.

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. 5 Both bands as one picture: two branches, two pairs, one result.

How a survivor is read, and why it cannot be gamed

The measurement in each cell deserves a paragraph, because a null result is only as good as the thing that was measured on both sides of it.

A cut run and its control share a history exactly: the same seed angles, the same grid, the same rise, the same organs, up to the moment one organ is removed from one of them. Both are then continued by the same rule for three hundred more organs. Every lag from one to twenty-four is compared between the two — how steady the hop is in the cut run, and how far its mean has moved from the control’s — and a lag counts as rigid when its hop is steady to within half a degree and unmoved to within three.

One wrecked stem, lag by lag — golden, rise 0.005, organ 6 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 55 degrees. The lag-4 hop swings by 0.12 degrees and sits 0.01 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 4, which is the surviving lag and not a coincidence.
Fig. 6 One such comparison in full: every lag, its steadiness, and the one that comes out rigid.

Nothing in that reads the counted pair, the step ordering, or the rise. It reads two node lists. So a cell of a band’s grid cannot be nudged toward one answer by the quantity the band varies, which is the property a matched design needs and does not always have.

The threshold is not delicate either, and that matters more here than usual. The rigid hops measure between zero and about a tenth of a degree of movement, and the next steadiest lag in any wrecked stem measures tens of degrees. There is no setting of the threshold between those two that changes any cell in either grid.

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. 7 The same quantity across the census, where the same gap of two orders of magnitude separates a survivor from everything else.

What that refutes, precisely

Not “the shortest hop survives” as a claim about the census — that was already refused. What it refutes is the possibility that the ordering is the mechanism’s variable at all, on these lattices.

The distinction is worth spelling out. A reading can fail on a table for two reasons: because the quantity it names is not what acts, or because the table could not tell it apart from a rival. The census could not separate those two, because on twenty-five of its thirty rows the shortest-hop reading and the larger-family reading make the same prediction. A band separates them by construction, since the ordering flips while the family does not.

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. 8 The census scores, which are what a band was needed to interpret rather than to overturn.

Scored on the bands, the shortest-hop reading is right at fourteen of the golden band’s twenty-four cuts and six of the Lucas band’s thirty-one: twenty of fifty-five, for an outcome that never changed. That number is not evidence about the mechanism at all. It is the fraction of rises on the side of the handover where the surviving family happens to have the shorter step, which is arithmetic about where the handover sits.

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. 9 Where the handovers sit, which is what that twenty-of-fifty-five is a measurement of.

What it does not refute

The rise, which the band cannot hold. Each band spans a factor of about a fifth in the rise, so a quantity depending smoothly on the rise over that range is not controlled here. What can be said is bounded and worth saying: over a fifth in the rise, at a held pair and a held divergence, the answer does not change.

The offset, which is the reading that scores best and which the band leaves entirely alone. Every cell in both grids is at a fixed offset down a column, and the rule stated over the offset predicts every one of them correctly. The band is silent about it by design.

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. 10 The rule the band does not test, marked on the census it was scored on.

And the front, which changes by an organ or two across a band as the rise falls. That is visible in the grids as a ragged edge: at the coarse end of the golden band one offset wrecks, in the middle two or three, at the fine end two. Whether the extra offsets that appear are the ones that would have kept the other family is a question this design cannot answer, because they do not exist at the other end to compare with.

How many offsets wreck, along the 5/8 rung. The count of offsets that never repair, at each rise on one rung. It runs from 1 at the coarse end to 5 at the fine end, while a counter returns 5 and 8 spirals at every one of them. The front — the run of recent organs at which a removal is felt at all — deepens as the rise falls, so there are simply more places a cut can land and fail to heal. That is the mechanism under the grid: the offsets that appear at the fine end are the ones beyond the smaller contact number, and those are the ones that keep the larger family.
Fig. 11 The front deepening down the rung the golden band sits in, which is the quantity the ragged edge comes from.

The thinness of it, stated

Twenty-four cuts on one band and thirty-one on the other is fifty-five, and fifty-five is a decent number. But they are not fifty-five independent stems: the golden band’s twenty-four are eighteen rises times one or two offsets each, and offset four accounts for eighteen of them on its own.

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. 12 The grid again, read as what it is: one long row at offset four and a few cells either side of it.

So the strongest single statement available is about that one row. Offset four, eighteen rises, the ordering reversing in the middle, the five surviving at every one. The other rows agree and are shorter.

That is a narrower claim than fifty-five cuts implies and it is the honest one. It is still much stronger than anything a census could produce, because a census row is one stem and this is eighteen stems that differ in one quantity.

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. 13 What one of those cells is: an organ removed, and a comparison against a control that shares the stem’s history.
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. 14 And how the survivor is read out of it: by lag, against that control.

The predictions it was possible to make in advance

Before the ablation was run, the band made three predictions and it is worth recording how they came out, because a design’s value is partly in what it committed to.

That the counted pair would hold at every rise. It does, at all thirty-seven, which is asserted in the machinery rather than checked by eye. Had it failed, the band would have straddled a transition and not a handover.

That the front would change by an organ or two rather than by several. It does. The wrecking offsets across the golden band run one, two, three, two, and across the Lucas band one or two. A front that changed by five would have made the grids incomparable end to end.

The same rule, the same rise, two lattices, two fronts. How many organs back a single removal is still felt, on a stem seeded onto the golden lattice and on one seeded onto the Lucas lattice, at seven rises. Everything but the seed is identical at each rise — the rule, the spacing, the heights, the azimuth grid — and the two fronts differ at every one of them. Which branch has the wider front changes hands four times going down the range, so no function of the rise gives the column. The golden branch carries 5/8 at four of these rises, across a factor of two in the rise, and its front is eight at all four.
Fig. 15 The front width across a much wider range, for the scale of what a band’s rise range does to it.

That the surviving family would either hold or flip at the handover. It holds, which is one of the two outcomes the design was built to distinguish. A flip exactly at the handover would have been the other, and would have made the ordering the actor rather than a passenger.

The two steps changing places inside the 4/7 band. Measured at every rise of a band on the Lucas branch, where a counter returns 4 and 7 spirals throughout. The settled divergence moves by 0.0195 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 1.0010 and the ordering changes hands at a rise of 0.0225, so above that rise the shorter step belongs to the 4 family and below it to the 7 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. 16 The Lucas band’s ordering, whose crossing is the rise a flip would have had to land on.

Three predictions, three confirmations, and the third is the result. Stating them first is what separates a test from a look.

Where the question goes now

Two quantities move along a rung. One of them has now been reversed under a controlled comparison and the answer did not follow it. That does not promote the other — the settled divergence — to the actor, because the divergence is exactly what a band holds.

Two lines across the 5/8 rung, crossing once. The divergence the rule settles on, against the divergence at which the two contact steps would be exactly the same length. The second is arithmetic on the lattice and no stem is grown for it. Across this rung the balanced line moves 2.281 degrees and the rule's own line moves 1.262, so the shallower line crosses the steeper one, and it does so exactly once at a rise of 0.0154 — 16 per cent of the way down from the coarse end. That crossing is the handover: above it one family has the shorter step and below it the other does. So a rung has one handover, its position is fixed by the arithmetic rather than by any experiment, and a sweep of the rise carries a stem across it at a place nobody chose.
Fig. 17 The arithmetic behind the band, and the reason the divergence is flat precisely where the ordering flips.

What it leaves is a shorter list. The candidates for what varies along a rung and decides the surviving family are now the settled divergence, the front depth, and the rise itself. And the three are not independent of one another: the front deepens because the rise falls, and the divergence slides because the rise falls.

The divergence slides along the 5/8 rung. Measured at every rise on one rung, where a counter returns 5 and 8 spirals throughout. The settled divergence slides from 136.6406 to 137.8672 degrees. The ratio of the two contact steps falls to 1.0131 at a rise of 0.016 and the ordering changes hands at 0.015: above it the shorter step belongs to the 5-family and below it to the 8-family. Neither quantity is available to a counter, which is shown positions and reports a pair, and both of them move while that pair does not.
Fig. 18 The divergence slide across the whole rung, which is the candidate a band cannot test because it is what a band holds.

Separating those needs a different design, and the obvious one is a band around a divergence rather than around an ordering: two rises on different rungs whose settled divergences agree, with different pairs. Whether such pairs exist is arithmetic on the ladder, and the ladder sweep has the numbers to answer it without growing anything.

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. 19 The ladder the search would run over, whose rungs each carry a slide and a floor.

What the census still has that the band does not

It is worth being even-handed, because the band is a better design and a much narrower one.

The census spans five counted pairs and both branches; the bands span two pairs. The census reaches offsets from three to nine; the bands reach three to five, because a band sits at one rung and a rung’s front has one depth. And the census contains the two lattices that never wreck at any offset, which are in it precisely because a table assembled from the lattices that produce an answer is a table of its own selection — a band has no equivalent, since every rise in it is chosen for its geometry rather than for its outcome.

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. 20 The census’s reach, which is wider than a band’s in every direction except the one that matters here.

So the two are complementary and the order they were done in is the wrong way round only in hindsight. A census establishes what the phenomenon is: that a wrecked stem keeps exactly one hop, that the survivor is one of the two contact families, that the offset accounts for most of it. A band tests a reading once there is a reading to test. Neither would have been much use first.

A cell's neighbours are its spiral families. Left: part of a 900-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 1903 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, 5.72 edges per cell.
Fig. 21 The fact the census established, which every reading since has been stated inside.

The negative that is worth having

It is worth saying why a null result is the outcome this thread wanted rather than a disappointment.

The census’s decisive negative was a pair of runs sharing a pair and an offset and keeping different families, which closed a whole class of accounts: no function of the pair and the offset can produce both rows. That was strong precisely because it was a refutation with two rows in it rather than a score.

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. 22 The measurement that first showed the answer changing along a rung, which is what left two candidates standing.

This is the same shape, one level down. It does not say what decides the survivor. It says that one of the two remaining candidates does not, on fifty-five cuts across two branches, with the quantity reversed rather than sampled. A shorter list of live accounts is what progress looks like when the mechanism is not going to hand anybody an answer.

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. 23 The account that does best on the arrangement rather than the sequence, which the band leaves untouched.
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. 24 The neighbourhood all of these readings are stated over, whose two families are the only candidates a survivor is ever drawn from.

A word about how this reads against the mechanism

The reading that failed here was not arbitrary. It came from the rule: a sum of inverse powers of distance weights the nearest organ hardest, so the nearest family ought to be the one a disturbance cannot dislodge. That is the sort of argument this collection generally trusts, and it is worth asking what its failure means.

One reading is that the weighting is not as lopsided as the phrase suggests. At the exponents used here, the terms of the sum at the growing tip belong to lags across the whole contact neighbourhood, not to one organ — and the five largest terms belong to the pair, the number below it and the two above, at every exponent tried. A rule reading five families roughly equally has no reason to privilege whichever of two nearly equal steps is a per cent shorter.

The neighbourhood of 21/55, and where its background was taken from. μ₂ across nine tenths of a degree either side of 21/55, on a head of 825 organs — 15 in each of its 55 rows. The deep notch at the centre is the dip. The shaded columns are the offsets this site now takes a background from: those at least 0.03° from every rational with a denominator of 60 or less, of which there are 54 here. The marked sample at 0.2° is the one the earlier work used, and it lands 0.007° from 13/34 — inside that rational's own dip. It reads 0.115 against a floor of 0.148, so measured that way the dip is an inversion. The clear offsets give 0.339.
Fig. 25 The neighbourhood the rule sums over, whose largest terms are spread across several families rather than concentrated on one.

The other reading is that the surviving family is not about the tip’s neighbours at all but about what the removal did to the arrangement above it, which is where the account that scores best lives. On that account the ordering was never a candidate, and its failure here is a confirmation rather than a surprise.

Both readings predict what the band found. Neither is tested by it, which is the usual position after a null: the list is shorter and the survivors are unranked.

What is left

The four rungs with a computed handover and no band grown on them. Each would cost a few minutes of geometry and a few of ablation, and each would add a different counted pair to a result that currently rests on two.

The Lucas 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 6 and 40 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; three of them sit past the mark.
Fig. 26 Those rungs, four of which have a crossing and no band.

And the direct test of the front, which deepens down a rung whether or not anything else does. The ragged edges of both grids say the front changes by an organ or two across a band; a design that held the front exactly — by choosing rises with the same number of wrecking offsets — would remove one more candidate. Whether such a set of rises exists inside a band is a question the existing sweep already answers, and it has not been asked.

Two answers 138° apart, and one organ holding the second one up. The repulsion the rule minimises, around the circumference of a stem at a rise of 0.008, at the height the next organ will sit at. It has two low points 138.3° apart: the slot the next organ takes, and the slot the organ after it will take. The runner-up is 13.6% higher. The organ 13 places back carries 14.6% of the energy at the winning slot and twelve places back carries 16.3% at the runner-up — and that is more than the gap, so taking that organ away makes the runner-up win and the next organ appears a whole divergence away. Neither guard is a contact of the organ being placed; twelve is one place inside the larger number of the pair this stem is climbing towards.
Fig. 27 The front the test would hold, whose width is read from the pair rather than from the ordering.
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. 28 The table all of this feeds, whose rows now carry a side as well as a rise.

What links here

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

Shares its objects with

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

  • The organ that was nobody's neighbour — both name ablation, claim testing, control, falsifiability, lattice offset, negative result, parastichy pair, the placement rule, rigid hop, rung, underdetermination
  • The shortest hop was a coin flip — both name ablation, claim testing, control, falsifiability, lattice offset, negative result, parastichy pair, the placement rule, rigid hop, rung, underdetermination
  • A stem too fine to settle — both name counting blind, claim testing, control, negative result, parastichy pair, the placement rule, rung, underdetermination
  • One rise per rung is a sample — both name counting blind, claim testing, control, falsifiability, negative result, parastichy pair, rung, underdetermination
  • Two accounts of one number — both name ablation, counting blind, claim testing, negative result, parastichy pair, the placement rule, rung, underdetermination
  • A period that is not a count — both name ablation, counting blind, falsifiability, lattice offset, nearest neighbour, parastichy pair, rigid hop

Named objects

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

AblationCounting blindClaim testingControlFalsifiabilityHandoverLattice offsetMatched designNearest neighbourNegative resultParastichy pairThe placement ruleRigid hopRungUnderdetermination