The claims, measured

A count that can be wrong by one

A reported parastichy pair pins the divergence angle to a band 221°/mn wide only if both counts are right. Allowing either to be off by one adds the bands of every neighbouring pair whose counts share no factor, and those bands sit where their own lattices live: for 2/3 they swallow the whole range, and for 34/55 they are two bands as narrow as the true one at 109° and 113°, twenty-five degrees away. So a high count that may be wrong is not a blurred reading but a short list of sharp candidates, costing log₂ 3 bits. And on the Fibonacci pairs, two in every six — 21/34 and 34/55 among them — cannot be miscounted silently by one count at all, because every such miscount shares a factor.

Worth reading first: What a count is worth.

A published count is a pair of numbers, and what a count is worth measured how much a pair pins down the divergence angle of the plant it came from: a band 221°/mn221°/mn wide, so that 2 and 3 leave thirty-nine degrees open and 34 and 55 a little over a tenth of one. Every step up the Fibonacci pairs is worth a factor of φ2\varphi^2.

That essay ended on a condition that undid part of its own recommendation. The width is what a correct count leaves open. High counts are worth a thousandfold more than low ones, and high counts are exactly where the spirals are most numerous and most nearly parallel, which is where a person tracing them by eye — following each family round without an index — is most likely to be one out. So the question is what a report is worth when either count may be wrong by one.

The neighbours a miscount produces

A report of (m,n)(m, n) read with a tolerance of one allows eight other pairs: either count up or down by one, or both. Some of those are not pairs an ordinary lattice can show at all. If the two counts share a factor, the pattern would be whorled, several primordia arriving at once, and a report of 34 and 56 is a report of a pattern that arrives two at a time rather than a slightly wrong 34 and 55.

The rest share no factor, and each of those is the two shortest families of some lattice at some divergence angle. The same scan that measures a report’s band finds where: one band each. The question becomes where those bands fall relative to the true one.

Low counts blur, high counts split

What each report allows once either count may be wrong by one. The divergence axis from 20° to 180°. For each report, the dark band is what it allows if both counts are right and the pale bands what the coprime pairs one count away allow. 2/3 allows 38.85° exactly and 160.04° in 1 piece spanning 160.04°; 5/8 allows 5.53° exactly and 35.16° in 5 pieces spanning 101.69°; 13/21 allows 0.811° exactly and 2.44° in 3 pieces spanning 83.94°; 34/55 allows 0.118° exactly and 0.354° in 3 pieces spanning 28.41°. For the low pairs the wrong bands swallow the right one; for the high pairs they are separate and narrow.
Fig. 1 The divergence axis with the band each report allows if its counts are right, dark, and the bands its coprime neighbours allow, pale, for four reports.

For 2/3 the answer is the worst possible. One of its neighbours is 1/2, and 1/2 is the two shortest families at every angle from twenty degrees to a hundred and eighty: a 2/3 that might be wrong by one says nothing about the angle at all. For 5/8 the tolerant report allows 35.2 degrees in five pieces spread over 102. For 13/21 it allows 2.4 degrees in three pieces spread over 84, and for 34/55 it allows 0.354 degrees in three pieces spread over 28.

A miscount moves the report

For a high pair a miscount does not blur the report: it moves it. The divergence axis from 50° to 145°. For 21/34 and 34/55, the dark band is what the report allows if both counts are right and the pale bands what it allows if either is wrong by one. 21/34 allows 0.308° exactly and 0.931° in all, in 3 pieces: 20/33 at 54.37° and 22/35 at 82.13° beside the true band at 137.48°; 34/55 allows 0.118° exactly and 0.354° in all, in 3 pieces: 33/56 at 109.23° and 35/54 at 113.27° beside the true band at 137.52°. Each wrong band is as narrow as the right one and tens of degrees from it, so the reading does not widen; it becomes a short list of sharp candidates, and neither wrong candidate contains the golden angle.
Fig. 2 The two highest reports on a narrower stretch of the axis, with each neighbouring pair’s band labelled where it falls.

At 34/55 the two neighbours that share no factor are 33/56 and 35/54, and their bands sit at 109.23° and 113.27°, each about an eighth of a degree wide: as narrow as the true band at 137.52°, and twenty-four and twenty-eight degrees from it. At 21/34 they are 20/33 at 54.37° and 22/35 at 82.13°.

So a high count that is wrong is not a blurred version of the right answer. It is a different sharp answer somewhere else. Neither wrong band at either pair contains the golden angle, and nothing about the band a wrong 34/55 allows would look less confident than the band a right one allows.

Why the wrong bands sit where they do

A pair (m,n)(m, n) is the two shortest families when both mm turns of the divergence and nn turns land close to a whole number of turns, which means the angle is close to 360°a/m360°\,a/m and to 360°b/n360°\,b/n for some whole numbers aa and bb at once. The band lives where those two fractions nearly agree.

For 34/55 they are 360°×13/34=137.65°360° \times 13/34 = 137.65° and 360°×21/55=137.45°360° \times 21/55 = 137.45°, and the band is between them. For 33/56 the nearest agreement is 360°×10/33=109.09°360° \times 10/33 = 109.09° and 360°×17/56=109.29°360° \times 17/56 = 109.29°, and its band is at 109.23°. For 35/54 it is 360°×11/35=113.14°360° \times 11/35 = 113.14° and 360°×17/54=113.33°360° \times 17/54 = 113.33°, with the band at 113.27°. Changing a count by one changes which fractions agree, and the agreement it lands on has no reason to be anywhere near the golden angle’s.

Why a low pair’s neighbour covers everything

The reason 2/3 is worthless under a tolerance of one is its neighbour 1/2. When the rise between successive primordia is large, only the first two offsets are short enough to be the two shortest families at all, whatever the angle, so 1/2 is what every lattice shows at a coarse enough rise. A report of 1 and 2 is a report that the lattice is coarse, and it carries nothing about the divergence.

A low count is therefore fragile in a different way from a high one. A wrong high count is confidently somewhere else; a wrong low count can be a count that was never able to say anything, and a tolerance of one admits that possibility.

The width falls, the span does not

The total width a tolerant report allows, against the distance its pieces are spread over. For each Fibonacci report read with a tolerance of one, the total width of divergence angle it allows and the span from its lowest to its highest candidate. 2/3: 160.04° in all over a span of 160.04°; 3/5: 63.07° in all over a span of 85.47°; 5/8: 35.16° in all over a span of 101.69°; 8/13: 10.61° in all over a span of 99.35°; 13/21: 2.44° in all over a span of 83.94°; 21/34: 0.931° in all over a span of 83.43°; 34/55: 0.354° in all over a span of 28.41°. The width falls by more than two orders of magnitude from 2/3 to 34/55; the span barely falls until 34/55, because the wrong candidates sit where their own lattices live rather than near the right one.
Fig. 3 For seven Fibonacci reports read with a tolerance of one, the total width of angle they allow and the span their candidates are spread over, on a logarithmic axis.

Read with a tolerance of one, the total width a report allows falls from 160 degrees at 2/3 to 0.354 at 34/55, more than two orders of magnitude. The span of its candidates falls from 160 degrees to 84 by 13/21 and stays there until 34/55, where it drops to 28. The candidates sit where their own lattices live, and a pair one count away from a Fibonacci pair belongs to a lattice nowhere near the golden angle.

That is why a single number stops describing the report. Its measure is still small. Its span is not.

What the tolerance costs, in bits

How many bits of the angle a report carries, exact and read with a tolerance of one. The information a report carries about the divergence angle, as log₂ of the 160-degree range over the width it allows. 2/3 carries 2.04 bits exactly and 0.00 read with a tolerance of one; 3/5 carries 3.47 bits exactly and 1.34 read with a tolerance of one; 5/8 carries 4.85 bits exactly and 2.19 read with a tolerance of one; 8/13 carries 6.24 bits exactly and 3.92 read with a tolerance of one; 13/21 carries 7.62 bits exactly and 6.04 read with a tolerance of one; 21/34 carries 9.02 bits exactly and 7.42 read with a tolerance of one; 34/55 carries 10.40 bits exactly and 8.82 read with a tolerance of one. The cost of the tolerance is 2.04 bits at 2/3, which is everything, 2.32 at 8/13, and 1.58 at 34/55 — within a hundredth of log₂ 3, the cost of not knowing which of three equally narrow candidates is the right one. On the Lucas pairs, 18/29 loses 2.80.
Fig. 4 The bits of divergence angle each Fibonacci report carries, exactly and read with a tolerance of one on each count.

Counted as information — the logarithm of the 160-degree range over the width a report allows — 2/3 carries 2.04 bits when both counts are right and none when either may be wrong. 8/13 carries 6.24 and 3.92, and loses 2.32. 34/55 carries 10.40 and 8.82, and loses 1.58, within a hundredth of log23\log_2 3.

That last number is not a coincidence. At 34/55 the three candidates are equally narrow, so the tolerant report is the exact report plus the question of which of three it is, and a three-way choice is exactly log23\log_2 3 bits. On the Lucas pairs the cost is larger: 18/29 loses 2.80 bits, because it has six coprime neighbours rather than two.

A second estimate picks the candidate

A choice among three sharp candidates tens of degrees apart is a cheap choice to make. Any other estimate of the angle, however rough, that lands nearer the true band than the nearest wrong one settles it.

How rough a second estimate of the angle can be and still pick the right candidate. For each Fibonacci report read with a tolerance of one, half the gap between the true band and the nearest wrong one: an estimate of the angle from anything else, good to that many degrees, falls nearer the true band than any candidate a single or double miscount produces. 2/3: 0.00°; 3/5: 0.00°; 5/8: 3.07°; 8/13: 5.84°; 13/21: 27.30°; 21/34: 27.53°; 34/55: 12.07°. At 2/3 and 3/5 the wrong bands overlap the right one and no estimate separates them; from 13/21 upward an estimate good to twelve degrees does.
Fig. 5 For each Fibonacci report, how coarse a second estimate of the angle can be and still fall nearer the true band than any band a miscount produces.

For 2/3 and 3/5 no second estimate helps, because the wrong bands overlap the right one. For 5/8 it has to be good to 3.1 degrees and for 8/13 to 5.8. For 13/21 and 21/34 an estimate good to 27 degrees suffices, and for 34/55 one good to 12. That is an estimate a person could make from a photograph with a protractor, or from the angle a round trip through the counts returns at a lower count.

Which miscounts announce themselves

The neighbours that share a factor are the other half of the story, because a miscount that produces one can be caught. A report of 34 and 56 is a whorled report, and a counter who knows the plant is not whorled knows the count is wrong.

How many of the eight share a factor depends on the pair, and not smoothly. At 5/8 three do; at 8/13 four; from 13/21 to 34/55 six do. On the Lucas pairs it runs the other way: at 11/18 and 18/29 only two of the eight share a factor, and six miscounts would pass as ordinary reports.

Two pairs in six cannot be miscounted silently

The sharper question is about single miscounts — one count wrong by one, the other right — since those are far more likely than both counts wrong at once. For each of the first twenty-four Fibonacci pairs from 2/3, the number of single miscounts that share no factor is two, except at two pairs in every six, where it is none.

How many single miscounts of a report share no factor and so pass unnoticed, pair by pair. For each of the first twenty-four Fibonacci pairs from 2/3 and thirteen Lucas pairs from 4/7, the number of pairs one count away — one count up or down by one, the other right — whose two counts share no factor. Such a miscount looks like an ordinary report. Among the Fibonacci pairs the count is two at every pair from 5/8 except two pairs in every six, where it is none: 21/34, 34/55, 377/610, 610/987, 6765/10946, 10946/17711, 121393/196418. At 34/55 the reason is visible: 33 is 3·11 and 35 is 5·7, and 21 is 3·7 and 55 is 5·11, so every single miscount of either count shares a factor with the other. Among the Lucas pairs the count is 2, 4, 2, 2, 4, 2, 1, 3, 2, 2, 3, 1, 2 — never none.
Fig. 6 The number of single miscounts that share no factor, for the first twenty-four Fibonacci pairs and thirteen Lucas pairs, with the pairs that have none shaded.

The protected pairs are 21/34, 34/55, 377/610, 610/987, 6765/10946, 10946/17711 and 121393/196418. At 34/55 the reason can be read off the numbers: 33 is 3 × 11 and 35 is 5 × 7, while 21 is 3 × 7 and 55 is 5 × 11, so miscounting either count up or down by one lands on a number sharing a prime with the other. None of the thirteen Lucas pairs from 4/7 is protected.

The same factors, six pairs later

The pattern is not special to 34 and 55. At 377/610 and 610/987, the next protected pairs, 609 is 3×7×293 \times 7 \times 29 and 611 is 13×4713 \times 47, while 377 is 13×2913 \times 29 and 987 is 3×7×473 \times 7 \times 47. Miscounting 610 by one in either direction lands on a number sharing a prime with both of its neighbours in the sequence, exactly as miscounting 34 did.

Fibonacci numbers either side of a Fibonacci number factor through its neighbours’ factors in a cycle, and the cycle has length six. The pairs measured here show it holding for twenty-four consecutive pairs and do not prove it for all of them; the identities that would prove it are standard results about Fibonacci and Lucas numbers, and nothing in the argument above depends on more than the twenty-four checked.

What protection is worth

How often a report is wrong without announcing it, for four pairs. Each count is off by one, up or down equally, with the chance on the axis, independently. A wrong report whose counts share a factor announces itself; a wrong report whose counts share none looks like an ordinary one. At 8/13 a silent wrong report has a chance of 1.0e-2, 2.0e-2, 4.9e-2, 9.5e-2, 1.8e-1; at 13/21 a silent wrong report has a chance of 9.9e-3, 2.0e-2, 4.8e-2, 9.0e-2, 1.6e-1; at 21/34 a silent wrong report has a chance of 5.0e-5, 2.0e-4, 1.3e-3, 5.0e-3, 2.0e-2; at 34/55 a silent wrong report has a chance of 5.0e-5, 2.0e-4, 1.3e-3, 5.0e-3, 2.0e-2. At 8/13 and 13/21 it grows with the error chance itself, because a single miscount can be silent; at 21/34 and 34/55 it grows with its square, because only two miscounts at once can be.
Fig. 7 The chance a report is wrong and shares no factor, so passes as an ordinary report, against the chance each count is off by one, for four Fibonacci reports.

With each count off by one with a chance of one in twenty, a report of 8/13 or 13/21 is silently wrong about one time in twenty — 4.9 and 4.8 per cent. A report of 21/34 or 34/55 is silently wrong 0.13 per cent of the time. At an error chance of one in a hundred the two figures are one per cent and 0.005 per cent. On the protected pairs a silent miscount needs both counts wrong at once, so its chance goes as the square of the error. It is exactly half that square: both counts must move, and of the four ways two errors of one can combine, two land on the pairs that share no factor, 33/56 and 35/54. At a twentieth the square is a quarter of one per cent and half of it is the 0.13 per cent above.

That is a fact about arithmetic rather than about plants, and it happens to favour exactly the high counts that a census of spiral pairs most needs and is most likely to get wrong.

A second annulus catches the rest

The earlier essay suggested counting two adjacent annuli rather than one, because the counts change with radius and consecutive counts on a golden stem are consecutive Fibonacci pairs. That check has a precise form: counts (a,b)(a, b) in one annulus and (c,d)(c, d) in the next continue each other when c=bc = b and d=a+bd = a + b. Every one of the four counts appears in that relation, so no single miscount can pass it.

What counting a second annulus buys: a wrong reading passing with one pair against with two. Dashed: the chance a single report is wrong and shares no factor, so passes. Solid: the chance that two reports from adjacent annuli — the pair and the next pair a golden stem carries — are wrong and still follow on from each other, with each of the four counts off by one with the chance on the axis. At 8/13 with the next pair, 4.9e-5, 1.9e-4, 1.1e-3, 4.1e-3, 1.3e-2; at 13/21 with the next pair, 2.5e-7, 2.0e-6, 3.0e-5, 2.3e-4, 1.6e-3; at 21/34 with the next pair, never, never, never, never, never; at 34/55 with the next pair, 2.5e-7, 2.0e-6, 3.0e-5, 2.3e-4, 1.6e-3. No single miscount passes the relation between the two pairs, because every one of the four counts appears in it; at 21/34 with 34/55 no combination of errors of one does at all. Most of what the second annulus costs is readings that were right and are now flagged by an error in the other count, which is the price of the check rather than a failure of it.
Fig. 8 The chance a wrong reading passes as right, from one annulus and from two annuli whose pairs must follow on, against the chance each count is off by one.

Reading 8/13 with 13/21, a wrong pair of readings passes with a chance of 0.11 per cent at an error of one in twenty, against 4.9 per cent from 8/13 alone. Reading 13/21 with 21/34, it passes 0.003 per cent of the time. Reading 21/34 with 34/55, no combination of errors of one passes at all.

What the check costs

The second annulus is not free, and the cost is worth naming. A reading of two annuli has four counts rather than two, so it is more often flagged: at an error of one in twenty, the two annuli are right and consistent 81 per cent of the time, where one annulus is right 90 per cent of the time. Most of the difference is readings that were right in one annulus and caught an error in the other.

That is the price of a check rather than a failure of it. A flagged reading is a reading to redo, and a reading that passes wrongly is a published number that is confidently wrong — which a count carries no error argues is the worse outcome, and which at high counts the tolerant bands above show is worse still.

What miscounts do to a census

A survey that counts many heads and tallies their pairs is where these errors accumulate, and they accumulate unevenly. With each count wrong by one a twentieth of the time, a survey of golden heads counted at 13/21 records 90.3 per cent of them correctly, 5.0 per cent as pairs sharing a factor and 4.8 per cent as ordinary pairs that are not Fibonacci.

The same survey counted at 21/34 or 34/55 records 90.3 per cent correctly, 9.6 per cent as pairs sharing a factor and 0.13 per cent as ordinary pairs that are not Fibonacci. So a census taken high on the golden heads almost never manufactures a non-Fibonacci ordinary pair — and manufactures a whorled plant about one head in ten. A census that tallies whorled patterns without checking them against the plant’s own arrangement would find far more of them than there are, and the excess would be a signature of the counting rather than of the plants.

What this changes about counting further out

The recommendation to count high survives, and it changes shape. A high count is worth a thousandfold more when right. When it may be wrong by one, it is worth somewhat less, and the whole of the loss is a choice among a few distant candidates that any rough second estimate resolves. So the practical recommendation is to count high and record one more thing: either a rough angle, or the count in the next annulus.

What it does not survive is a report of a low pair that might be wrong. A 2/3 read with a tolerance of one is consistent with every angle there is, and no second estimate short of measuring the angle directly recovers anything from it.

What this does not say

It does not say how often counters are wrong by one, or whether errors in the two counts are independent. A person who loses track of one spiral family is likely to lose track in the same way on the other, which correlates the errors, and correlated errors are exactly the case the square law for protected pairs does not cover. It does not treat miscounts of two or more.

Nor does it say that a count’s error is equally likely up or down. Counting the spirals found an earlier version of the counter used on these heads returning the two smallest offsets rather than the two shortest families, a systematic error that is not an error of one at all, and a scheme that catches errors of one says nothing about it.

The claim, reduced

A report read with a tolerance of one allows the bands of its coprime neighbours as well as its own. For low pairs they swallow the true band; for high pairs they are as narrow and tens of degrees away, so the tolerance costs a choice among a few candidates — log23\log_2 3 bits at 34/55 — that a rough second estimate resolves. Two Fibonacci pairs in every six, 21/34 and 34/55 among them, admit no silent single miscount, and two annuli whose pairs must follow on admit no silent single miscount anywhere.

What would withdraw it

A coprime neighbour of a high Fibonacci pair whose band overlaps the true one. A tolerant report at 34/55 losing more than the cost of choosing among its candidates. A protected pair with a single miscount that shares no factor. A single miscount that passes the two-annulus relation. Each is checked whenever the bands are measured.

Still open: a miscount by more than one

Every tolerance here is one. A counter tracing a high family by eye is as likely to drift by two as by one, and the neighbours at a distance of two include pairs such as 32/55 and 34/57 whose arithmetic is different: some share factors with the true pair’s counts that no neighbour at one does, and the bands they add may fall closer to the truth.

The measurement is the same tolerant reading at a tolerance of two and three: how many candidates each high report then allows, whether they stay separated by more than a rough estimate can resolve, and whether any Fibonacci pair remains protected once a single count can drift by two.

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.

Named objects

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

CoprimeDivergence angleFibonacciHonest limitsIdentifiabilityLucas numbersMeasurement errorParastichy pairSilent failureSurvey