Stems and cones

Four crossings nobody visited

Six rungs of the ladder carry a handover and two of them had a band built on them. The other four are here: 70, 126, 16 and 124 rises wide, found by sweeping at a ratio rather than at a fixed step in the rise, which is why the fine ones had been stepped over.

Worth reading first: Where a handover sits · Counting the spirals · A head is a set of points.

A handover is the rise inside a rung at which the two contact steps change places. Six of the ladder’s eight rungs carry one, each carries exactly one, and every one of the six sits in the coarse half of its own rung.

Two of the six had a band built around them — a run of rises over which the counted pair and the settled divergence are both held while the ordering reverses. The other four were left as a note saying each was a few minutes of geometry and a few of ablation. This essay is those four, and the note was optimistic about one thing.

Where the two contact steps change places, on every rung. One row per rung of the two branches, drawn from its coarse end to its fine one on a logarithmic axis. The mark on each row is the rise at which the two contact steps change places — the rung's handover — and the shaded stretch is the band around it over which the settled divergence holds still. six of the eight rungs have a handover and every one of those sits between 6 and 40 per cent of the way down its rung, never past the middle. The two rungs without one are the coarsest on each branch, whose crossing is above the range this ladder reaches.
Fig. 1 Every rung of both branches, with its handover marked and the band around it shaded.

What a band is for

The rise moves three things at once: the pair a counter returns, the divergence the rule settles on, and which of the two contact steps is shorter. A result that changes along a rung cannot be attributed to any one of them.

A band is the design that separates the third from the other two. Near a handover the settled divergence is flat, so a stretch of rises either side of it share an angle to a twentieth of a degree while the counted pair holds — and the ordering, which is what changes hands at the handover, is reversed between the two ends.

Cut at both ends and anything that changes is attributable to the ordering. Nothing does, which is what two bands established and what four more are built to test on four more counted pairs.

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 band the design was first built on, holding two quantities and reversing the third.

The step has to be a ratio

The first version of this swept a band at an absolute step of 0.0002 in the rise. At the two handovers it was written for — 0.0156 and 0.0225 — that is about one per cent, which is a reasonable step.

At the 8/13 handover of 0.00605 the same 0.0002 is three per cent. At the 3/5 handover of 0.04172 it is half a per cent. So one absolute step is three different instruments at three different places on a ladder whose rungs span a factor of fifteen in the rise, and the coarse end is over-sampled while the fine end is stepped over.

That is the same argument the ladder itself is swept with, made one level down. The rungs are geometric — consecutive transitions sit at a ratio of about 1/φ² — so everything measured on them has to be measured in ratios. The bands here are swept at two parts in a thousand.

Every transition as the rise falls. The pair climbs 1/2 → 2/3 → 3/5 → 5/8 → 8/13. Consecutive transitions are 0.381, 0.382, 0.382 of the previous rise — 1/φ² is 0.3820.
Fig. 3 The ladder whose rungs span a factor of fifteen, on which one absolute step is three different instruments.

How a band’s extent is found

Not stated. Grown outwards from the handover, one step at a time in each direction, while three conditions hold: the rise stays inside the rung, the counter returns the rung’s own pair, and the settled divergence stays within a twentieth of a degree of its value at the handover.

The first rise that fails any of them ends the band on that side, and which condition ended it is recorded. Three of the six bands are ended on both sides by the divergence; two are ended on their coarse side by the rung’s own transition, which is to say the band would have run further if the rung had.

That distinction matters for reading the widths. A band bounded by the divergence is a measurement of how flat the curve is; a band bounded by the transition is a measurement of how much rung there was.

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. 4 The rung bounds a band is confined to, measured by the counter rather than chosen.

The four new bands

The golden 3/5 band sits around 0.04172 and carries 70 rises, spanning a factor of 1.148 in the rise, which is 14.6 per cent of its rung. Its divergence moves 0.0391° across the whole of it.

The golden 8/13 band sits around 0.00605 and carries 126 rises, spanning 1.284 — and that is 72.1 per cent of its rung, because the 8/13 rung is the narrowest on the ladder and the flat runs across most of it. Its coarse end is where the rung ends rather than where the divergence leaves the bound.

The Lucas 7/11 band sits around 0.00800 and carries 124 rises, spanning 1.279, which is 48.4 per cent of its rung. And the Lucas 3/4 band sits around 0.04299 and carries 16 rises, spanning 1.030 — three per cent of its rung, an order of magnitude narrower than any of the others.

What each band holds, and what it moves. One row per band. The counted pair is held by construction and the settled divergence is held to a twentieth of a degree; the quantity a band exists to move is which of the two contact steps is the shorter. five of the six do move it — the ordering changes hands exactly once inside, and at both ends the two steps differ by enough for an ordering to mean anything. The remaining one changes hands three times and its two steps are never more than 0.0 per cent apart, so it holds all three quantities and is a control rather than an experiment.
Fig. 5 The six bands with their widths, the divergence held across each, and how many times the ordering changes hands inside.

Why the fine bands are wide

The 8/13 band covers nearly three quarters of its rung and the 7/11 band nearly half, while the two coarse bands cover a seventh and a thirtieth. Read as a fraction of the rung that is a large difference; read as a factor in the rise it is not — 1.28 against 1.15 and 1.03.

Both readings are worth having and they say different things. The fraction says how much of a rung’s interior a band occupies, which is what decides whether a band can be sampled at all. The factor says how far the rise has to move before the divergence has slid a twentieth of a degree, which is a property of the curve rather than of where the transitions happen to be.

The fine rungs are narrow and their divergence is flat across them. The 8/13 rung slides only 0.117° end to end — less than three times the band’s own tolerance — so most of it qualifies.

The 3/5 rung at a tenth of the ladder's step. Every rise of one rung, sampled ten times as finely as the ladder that found the locked band. All 23 are counted at 3 and 5 spirals and all 23 settle: the largest wander is 0.221 degrees, against the 0.5 degree threshold and against the 0.79 to 1.60 degrees the band on the coarse rung wobbles by. The divergence slides smoothly from 139.0625 to 136.7344 degrees with no rise stuck on a rational and none stuck on anything else. Whatever the band is, it is not something a coarser sampling was hiding here.
Fig. 6 The fine end of the ladder, where a rung is narrow and its divergence barely slides.

Five of the six are matched pairs

A band is only useful if its two ends are a matched pair: the same counted pair, the same divergence, and opposite orderings that are far enough apart to be orderings at all.

Five of the six qualify. The ordering changes hands exactly once inside each of them, and at both ends the two contact steps differ by between 3.4 and 8.3 per cent in length — comfortably more than the four parts in a thousand below which an ordering is not an ordering.

The sixth is the Lucas 3/4 band, and it is a band that moves nothing. It is in the table.

Two lines across the 4/7 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 3.537 degrees and the rule's own line moves 2.602, so the shallower line crosses the steeper one, and it does so exactly once at a rise of 0.0222 — 7 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. 7 The two curves whose crossing is a handover, on the Lucas branch.

What the bands hold

The counted pair, by construction: a rise whose counter returns a different pair ends the band.

The divergence, to a twentieth of a degree at each end from the handover, which means at most a tenth across a whole band. Measured, the six slide 0.0391°, 0.0469°, 0.0430°, 0.0703°, 0.0391° and 0.0430° — five inside a twentieth and one, the Lucas 3/4, at seven hundredths because its two halves happen to slide in opposite directions.

And nothing else. The rise moves by 3 to 28 per cent across a band, and everything the rise controls moves with it: the neighbourhood size, the step lengths, the front’s depth. A band is a narrow experiment, not a small one.

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. 8 The slide across a whole rung, out of whose flattest stretch a band is cut.

Where the handovers sit

All six sit in the coarse half of their rungs: 11.6, 14.6 and 34.5 per cent on the golden branch, 40.4, 5.5 and 33.2 on the Lucas one. Never past the middle, which is a result the previous round established and did not explain.

Having six bands rather than two does not change that number — the positions come from the ladder sweep, not from the bands — but it does change what can be said about the consequence. A person growing a stem counted 5/8 picks a rise comfortably inside the rung, which is past the handover; so does a person growing one counted 4/7 or 8/13. The census’s sampling bias is a property of all six rungs and not of the two that had been looked at.

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 each handover sits inside its own rung, as a fraction from the coarse end.

The two rungs with no handover

The coarsest rung on each branch — golden 2/3 and Lucas 1/3 — has none. Their two contact steps never change places anywhere inside them, so there is no crossing to build a band around and asking for one is refused rather than answered with the rung’s coarse end.

That refusal is asserted rather than left to chance, because the failure mode is quiet: a function that returned the nearest thing it could find would produce a band with no handover in it, whose two ends have the same ordering, and every other check on it would pass.

The reason those two rungs have none is that their crossing sits above the range the ladder is swept over. The sweep stops at 0.0700 because above that the rise is no longer a small quantity and a stem’s front is its own two edges.

Which rises are a lattice, from 0.04 to 0.13. How much the divergence wanders over the last sixty organs, at each rise up the coarse ladder. 13 of the 19 settle, scattering between 0.0000 and 0.3356 degrees. six do not: from 0.09 to 0.115 the divergence sticks on exactly 135.0000 degrees, which is three eighths of a turn, and wobbles about it by 0.79 to 1.60 degrees. A counter shown either kind returns the same pair, so the counts cannot tell them apart. The line is the threshold a rise has to pass before a cut is made on it, and it sits in the gap rather than among the measurements.
Fig. 10 The coarse end, above which the sweep stops and where the two missing crossings would sit.

What it cost

The geometry is cheap and the cuts are not. Sweeping a band’s rises costs one grown stem each — 70, 112, 126, 16, 86 and 124 of them, plus the ladder sweep underneath — and each stem is a few hundred organs placed one at a time.

The ablation is sixteen cut stems per rise, each grown three hundred organs past the cut with a control beside it. Cutting every rise of every band would be several hours for a quantity the design predicts to be constant, so the cuts are made at nine rises spread through each band plus both ends and the handover itself.

That is a choice and it is the right one for the shape of the claim. A constant is tested at the extremes and at the crossing; sampling the middle more finely buys resolution in the one place where nothing is supposed to happen.

How many organs a stem needs before it is on a lattice. One row per rise, one mark per starting angle, placed at the organ from which every later divergence stays within a degree and a half of the run's own final value. Where a stem settles at all it does so between 0 and 290 organs in, against the 400 every ablation run here grows before it cuts anything. Not one row needs the length it is given. What changes down the table is the count on the right: how many of the nine starting angles reach a lattice at all, which falls from 7 at the coarse rises to 1 at the finest.
Fig. 11 What one settled stem costs, which is the unit a band’s sweep is paid for in.

What a finer sweep would add

Nothing to the claim and something to the picture. At two parts in a thousand the widest band carries 126 rises, which is enough that the divergence’s shape inside it is drawn rather than sketched. Halving the step would double the stems and change no number here.

Where a finer step would matter is at the ends. A band’s extent is where the divergence crosses a bound, and the crossing is located to within one step — two parts in a thousand in the rise, which is a tenth of the narrowest band’s whole width and a hundredth of the widest’s. The widths quoted here are therefore good to about one per cent on the wide bands and ten on the Lucas 3/4.

That last figure is worth carrying, because the Lucas 3/4 band is the one whose width is most surprising and the one whose width is least well measured.

Two ways of predicting how wide a band is. A band ends where the settled divergence has moved 0.05° from its value at the handover, so the width should follow from how fast the divergence changes there. Reading that rate as the rung's average slope predicts widths that are wrong by factors of 0.20 to 5.92 — wrong in both directions, so no constant rescues it. Reading it as a curvature about a stationary point gives 0.41 to 1.08, with five of the six inside a third. The difference between the two is the difference between a curve and its average, and a band is exactly where the two are least alike.
Fig. 12 The measured widths against two predictions, one of which is out by factors of five.

What the four new bands are for

Two things. The first is weight: the ordering result rested on two counted pairs and now rests on four, with 114 wrecked cuts rather than fifty-five.

The second is coverage. The two original bands were both on rungs in the middle of the ladder — 5/8 and 4/7 — and the four new ones reach the coarse end and the fine end of both branches. A claim tested only in the middle of a range is a claim about the middle of a range.

The families left standing, on both sides of every handover. One row per band, with every offset cut at rises spread across it and always at both ends and at the handover itself. The last column is every family left standing anywhere on that band. On three of the four bands that wreck at all it is a single family, unchanged across a rise at which the two contact steps swap places — so the step ordering is not what decides which family survives, and the result now rests on four counted pairs rather than on two. The shortest-hop reading scores 44 of 114 across the whole set, which is what a reading looks like when the quantity it is stated over is not in the mechanism.
Fig. 13 The cuts made at every band, which is what the four new crossings are for.

What the note underestimated

“A few minutes of geometry and a few of ablation” was right about the geometry and wrong about the sweep. The four bands were not found by pointing the existing machinery at four new rises; they were found after the step was changed from an absolute amount to a ratio, and before that change two of the four could not be found at all.

The 8/13 band spans a factor of 1.284 around a handover at 0.00605, which is 0.0018 in absolute rise — nine steps of 0.0002, of which the existing loop allowed sixty. That one would have been found, coarsely. The Lucas 3/4 band spans 1.030 around 0.04299, which is 0.0013 — six steps, and its ends would have been located to a sixth of its width.

So the four were not four repetitions of an existing measurement. They were four repetitions of a measurement that had to be repaired first, and the repair is the part worth carrying forward.

Where the two contact steps change places, on every rung. One row per rung of the two branches, drawn from its coarse end to its fine one on a logarithmic axis. The mark on each row is the rise at which the two contact steps change places — the rung's handover — and the shaded stretch is the band around it over which the settled divergence holds still. six of the eight rungs have a handover and every one of those sits between 6 and 40 per cent of the way down its rung, never past the middle. The two rungs without one are the coarsest on each branch, whose crossing is above the range this ladder reaches.
Fig. 14 The six bands drawn at the ratio step, on which the fine ones are resolved rather than sampled.

Where the handovers came from

Not from the bands. A handover is found by sweeping the whole ladder at one per cent in the rise and reading, at each rise, which of the two contact steps is shorter; the handover is the rise inside a rung at which that changes.

It is also computable without growing anything. The divergence at which the two steps are exactly equal is a curve, found by bisection on the lattice’s own arithmetic, and the rule’s own settled divergence is a second, shallower curve. They cross once per rung, and the measured handover and the computed crossing agree on all six rungs to within one sweep step.

So the six positions are two independent measurements agreeing, and the bands are built at the place both of them name.

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. 15 The two curves whose crossing is a handover, one arithmetic and one grown.

What is held constant across all six

Every band is grown by the same loop with the same three stopping conditions, at the same step, with the same tolerance on the divergence. Nothing is tuned per band.

That matters because a band is a measurement of a rung rather than a construction placed on one. The widths come out at 1.03×, 1.15×, 1.18×, 1.25×, 1.28× and 1.28× because the six rungs’ divergence curves are shaped differently, and if any of those had been adjusted to make a band usable the spread would be an artefact of the adjusting.

The one place a choice is visible is the tolerance, and it is the same twentieth of a degree the first two bands used, kept rather than re-chosen.

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. 16 The Lucas rungs on one axis, whose three bands come out at very different widths from one loop.

What each band’s ends are bounded by

Recorded per band and per side, because the two kinds of end mean different things.

Four of the six bands are ended on both sides by the divergence leaving its bound, which makes their widths measurements of how flat the curve is.

Two are ended on their coarse side by the rung’s own transition: the golden 8/13 band and the Lucas 4/7 band. Those two would have run further if the rung had, so their widths are lower bounds rather than measurements — and the 8/13 band, at 72 per cent of its rung, is nearly the whole of one.

Where the two contact steps change places, on every rung. One row per rung of the two branches, drawn from its coarse end to its fine one on a logarithmic axis. The mark on each row is the rise at which the two contact steps change places — the rung's handover — and the shaded stretch is the band around it over which the settled divergence holds still. six of the eight rungs have a handover and every one of those sits between 6 and 40 per cent of the way down its rung, never past the middle. The two rungs without one are the coarsest on each branch, whose crossing is above the range this ladder reaches.
Fig. 17 The bands as stretches of their rungs, on which two of them run into a transition.

Why this could not wait for a finer ladder

The obvious alternative is to sweep the ladder itself more finely and find more rungs, and it does not help.

The ladder’s range is bounded at both ends by something other than resolution. Above 0.0700 the rise is no longer small and the coarse rungs cannot be wrecked; below 0.0040 a stem does not settle onto a lattice at any run length. Between those two the ladder has eight rungs and six of them have a handover.

A finer sweep would locate the six handovers more precisely and would not produce a seventh. So six bands is the population rather than a sample of it, which is the unusual position the width prediction is also in.

Every transition as the rise falls. The pair climbs 1/2 → 2/3 → 3/5 → 5/8 → 8/13 → 13/21. Consecutive transitions are 0.382, 0.382, 0.383, 0.382 of the previous rise — 1/φ² is 0.3820.
Fig. 18 The ladder swept past both ends of its usable range, on which the eight rungs are all there are.

The one line

Six rungs carry a handover; two had bands and four did not. Grown at a step that is a ratio rather than a fixed amount, the four carry 70, 126, 16 and 124 rises, spanning 1.15, 1.28, 1.03 and 1.28 in the rise and holding their divergence to between 0.039° and 0.070°. Five of the six bands reverse their ordering exactly once and are usable; the sixth does not, and is the subject of the next essay.

What each band holds, and what it moves. One row per band. The counted pair is held by construction and the settled divergence is held to a twentieth of a degree; the quantity a band exists to move is which of the two contact steps is the shorter. five of the six do move it — the ordering changes hands exactly once inside, and at both ends the two steps differ by enough for an ordering to mean anything. The remaining one changes hands three times and its two steps are never more than 0.0 per cent apart, so it holds all three quantities and is a control rather than an experiment.
Fig. 19 The six bands as a table, with the one that holds all three quantities marked as such.

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 angle the ladder returns to — both name discretisation, divergence angle, geometric ladder, ladder, matched design, measurement, parastichy pair, resolution, rise, rung
  • Two rungs, one angle — both name control, discretisation, divergence angle, ladder, matched design, measurement, parastichy pair, resolution, rise, rung
  • The column that cost no stems — both name control, handover, ladder, measurement, parastichy pair, rise, rung, sampling
  • The front that reads one short — both name discretisation, ladder, matched design, measurement, parastichy pair, rise, rung, tolerance
  • A front with no middle — both name discretisation, divergence angle, ladder, measurement, parastichy pair, rise, rung
  • Seven rises and two seeds — both name control, ladder, matched design, measurement, parastichy pair, rise, rung

Named objects

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

ControlDiscretisationDivergence angleGeometric ladderHandoverLadderMatched designMeasurementParastichy pairResolutionRiseRungSamplingTolerance