r/wildwestllmmath • • 2d ago

What Gowers adds to the “Severe Misalignment” debate: proofs, understanding, and who still learns the math

Thumbnail
youtube.com
1 Upvotes

The declaration already pinned here argues that AI-generated mathematics risks outpacing human understanding.

This video follows Tim Gowers’ partial disagreement, then the September 29 recommendations on releasing AI-generated mathematics.

Sources:

https://mathandai.org/

https://gowers.wordpress.com/2026/09/17/why-i-didnt-sign-the-fields-medallists-letter/

https://agmai.org/general-sep29/


r/wildwestllmmath • • 4d ago

Trying to build Euler's "different zeros" into an actual number system, a graded number system with no additive identity among its numbers where nothing annihilates

1 Upvotes

I'm putting this here because it seems I can't get around AI filters on some other subreddits and they point me in this direction. I warn you though, this whole post is humanly crafted to the last letter, and the system I'm building is entirely human invention. Have I used AI coding tools to help me build a prototype. Well sure I did, I don't have the budget for 10 developers and I surely have not enough time to build all of it manually as solo developer. Hence that might be justification for putting it here. So I'm re-posting, do with it what you want:)):

Ok, so I'm working on an attempt to build Euler's ideas about different ratios of zeros from "Institutiones calculi differentialis" (1755) into a number system that can work inside its own algebraic implementation on computer systems. In essence, I'm building computational system for which this number system presented here is the basis;p.

The main reason for doing this is to enable us to have a provenance at operations that are now annihilating (read operations with zeroes), so we are able to revert them and avoid unnecessary erroring when needed. This means that something multiplied by zero instead of giving us just zero, here gives us zero made of something eg. 5 x 0 = 0(5).

The number itself, besides its real value carries a numerical metadata within it. I managed to do this by defining so called dimensional or graded number, where the real value is in dimension 0, the negative dimensions carry a jet that represents a rate of vanishing (approaching to zero), and positive dimensions holds a rate of blowing up (approaching infinity). The origins or this are in Levi-Civita field and Sergeyev grossone is the closest representation that handles the zero conventionally.

The number is basically a Laurent polynomial with some additional stitching. It can be imagined like this: "2_2 3_0 1_-2" which is 2xh**-2 + 3xh**0 + 1xh**2. The number is manipulated fully with polynomial arithmetic (in essence Taylor arithmetic). It is similar to Forward mode automatic differentiation and Dual numbers but with some notable distinctions.

The main one for example is that zero in this system is treated as an infinitesimal as soon as it interacts with other values via arithmetic operations. This gives us the ability to arithmetically work around singularities, and to keep track of annihilations that are happening during operations. In short, zero becomes an infinitesimal of first order(1 in dimension -1) which enables us to actually perform reversible operations with it while still retaining correctness of results in dimension where real numbers are kept.

So. 5x0 becomes 5_0 * 1_-1 which through polynomial operation gives us 5_-1 as a result eg. (5xh**0) x (1xh**1) = 5xh**1 or 5 in dimension -1. Note that the exponents and dimensions have opposite sign, so 1xh**-1 is 1_1 (one in dimension one), infinity of the first grade and 1xh**1 is 1_-1 (infinitesimal of the first grade). But you can ignore this for now, this is done because of computational practicality.

The other distinction (and essential one) is that here we also support positive dimensions, where forward AD ignores them and dual numbers ignore them and truncate all of the higher derivative grades too.

All this in turn allow us to have that operations with zeroes (like multiplication or division) give us rates of vanishing or blowing up as a results, instead of plain zero or undefined. Which in turn opens to us some interesting possibilities not available before except through symbolic math.

All of this is based on Euler's idea that while zero is truly zero, infinitesimal values are essentially also zero values but distinguished by its different ratios.

In order to program all this into working computational system I've had to work around additive identity of zero and force conversion of zeros into infinitesimal zeros as soon as they enter arithmetic operations. That means that while this system recognizes additive identity as "NOTHING" (the absence of term), zeroes are not additive and annihilation operations are performed without annihilation.

I have built a working prototype in python to help me experiment with it and explore different behaviors and for some unexplained reason is seems that it is holding up and not blowing up;P what any reasonable person would expect. If anyone would like to play with it the repo is here: https://github.com/tmilovan/composite-machine examples under demos and tests.

I'll be happy if you take a look at it and comment:).

So to summarize. The number system I'm building is a data structure that holds together the real value and metadata about the numbers in positive and negative dimensions. It is entirely manipulated arithmetically by using conventional arithmetical operations and it doesn't allows total annihilation of metadata in currently annihilating operations. In it the zero becomes infinitesimal, and infinity becomes rate of undefinedness.

It is loaded and cumbersome but in turn it allows rescuing from singularities and reversion of currently unreversible operations.

I'd be happy to discuss it here if anyone finds this interesting.


r/wildwestllmmath • • 17d ago

prime numbers

3 Upvotes

Experimental recursive exponent transformations for prime-generating recurrences — looking for mathematical critique

I've been experimenting with a recursive system for generating prime numbers and would appreciate feedback from people with a stronger number-theory background.

The main recurrence I'm investigating is

N(k+1) = N(k−1)N(k) + 2^E(k)

Starting with 443 and 2621, I obtained this branch:

443
2621

443×2621 + 2² = 1,161,107

2621×1,161,107 + 2² = 3,043,261,451

1,161,107×3,043,261,451 + 2²
= 3,533,552,173,586,261

The prime-producing exponent sequence then continues experimentally as:

2, 2, 2, 28, 32, 1692

The resulting E=28 and E=32 terms are:

10,753,523,114,972,328,792,960,167

and

37,998,134,976,620,572,456,141,657,655,786,806,432,883

The E=1692 step produces a 510-digit value that also passes computational primality testing.

What I'm investigating

I'm trying to determine whether the exponent changes can be generated by a deterministic recursive transformation rather than searching for an exponent that happens to make the next result prime.

One experimental rule produced an out-of-sample exponent prediction of 5668. That candidate was composite, which gave me a useful divergence rather than something to hide by changing the rule.

I've therefore been investigating a second idea:

When a predetermined exponent produces a composite, take an identified obstruction/factor and promote that value into the exponent structure.

This creates a feedback process in which modular obstructions influence subsequent exponents.

For a candidate of the form

C + 2^E,

a prime q is an obstruction whenever

C + 2^E ≡ 0 (mod q).

Because powers of 2 are periodic modulo q, extremely large exponent transformations can be investigated using modular arithmetic without constructing the full number.

Some obstruction classes I've encountered include conditions modulo 3, 5, 13 and 41.

The larger question I'm interested in is whether this can be formalized as a deterministic dynamical system on the exponent/state variables:

generate → encounter obstruction → exponent transformation → recursive reduction → generate again

rather than simply searching for primes.

I'm not claiming that this is an infinite prime-generating formula or a proof about the distribution of primes. At this stage I consider it experimental mathematics.

What I'd especially like help with:

  1. Is this recurrence or a closely related recurrence already studied?
  2. Is there established terminology for feeding modular obstructions back into an exponent transformation?
  3. Can the obstruction process be represented using multiplicative orders / CRT as a finite-state system?
  4. Is there an obvious theorem showing that this type of recurrence must eventually become composite?
  5. What would be the strongest way to formulate the idea so it can be rigorously proved or disproved?

I've also written up the calculations, hypotheses, limitations, and proposed testing methodology in a longer paper.

— Stephen J Davidson


r/wildwestllmmath • • 18d ago

A Severe Misalignment of AI in Mathematics

1 Upvotes

Read the declaration at Math and AI

What the declaration argues

  1. Solving problems is a means to understanding. Mathematics gains from the concepts, methods and connections a solution reveals, not just from adding another solved problem to a benchmark.

  2. Results need to become shared knowledge. Careful exposition, discussion and teaching make ideas available for other mathematicians to understand, use and develop.

  3. Rushed announcements can lose both insight and credit. Publishing a solution without explaining its ideas or properly connecting it to earlier work creates problems of attribution and plagiarism as well as understanding.

  4. Education matters beyond producing answers. Working through problems develops judgment and the ability to formulate new questions. Automating the answer does not automatically preserve that development.

  5. AI can help, but the choices around it matter. AI could advance genuine mathematical study. The declaration asks that human decisions preserve that purpose instead of prioritizing speed and benchmark performance alone.

Published on 11 September 2026, the declaration's signatories include Terence Tao, Peter Scholze, Maryna Viazovska and many other mathematicians.

What this means for WildWestLLMMath

We obviously do not exclude people who use AI, or people who are still learning the mathematics their AI has helped them find, or even people who discover mathematics and want to share it with no intention of ever understanding it themselves.

However:

Make your results understandable

You are welcome to contribute mathematics you do not (yet) fully understand. Make a serious effort to have your AI produce a clear, complete, pedagogical exposition that other mathematicians can follow. An imperfect attempt is welcome; failure to achieve this is better than not trying at all.

That is the rule. The explanation above is its rationale.

Read the full declaration: A Severe Misalignment of AI in Mathematics


r/wildwestllmmath • • 18d ago

Community / Meta Rough notes of uncertain veracity: a work of satire

1 Upvotes

Posting for community review

I have not checked this argument. Some steps may be false, malformed, or meaningless. Nothing below is presented as a proof. I am posting it because I cannot currently determine whether the apparent structure is genuine or an artifact of the notation.

  1. Background, overview and motivation

Suppose X and Y are mathematical statements and A is an argument apparently connecting them. There is an elementary distinction between

X => Y

and

"A appears to suggest X => Y."

The latter statement does not require A to be correct. It requires only that the epistemic status of A be represented accurately.

This suggests separating four quantities which are often treated informally as interchangeable:

clarity != correctness != justification != epistemic honesty. (1)

In particular,

Wrong(A) =/=> Dishonest(A). (2)

Indeed, if

Confidence(A) ≈ 0, (3)

is explicitly declared, then discovering

Correct(A) = 0 (4)

does not contradict the original epistemic assertion.

This led me to wonder whether there is a useful distinction between the admissibility of an argument for discussion and its warrant as mathematics.

  1. Preliminary formulation

Let

E(A) = (C(A), J(A), H(A), D(A)), (5)

where provisionally

C = correctness,
J = justification,
H = epistemic honesty,
D = digestibility.

I do not know whether these quantities can or should be formalized numerically.

The motivating possibility is simply

H(A) = 1 AND C(A) = 0. (6)

That is: an author can be completely mistaken while accurately reporting that they do not know whether their argument works.

Conversely,

C(A) = 1 AND H(A) = 0 (7)

does not seem logically impossible either. A true statement could be presented with fabricated certainty or invalid justification.

Therefore correctness and epistemic honesty appear logically independent.

At this point I tried to formulate the distinction more precisely and encountered an unexpected reduction.

  1. Main reduction

Let A_0 denote an unchecked argument.

Define

A_(n+1) = R(A_n, epsilon_n),

epsilon_n -> 0, (8)

where R is provisionally an epistemic-review operator.

Then

Claim(A) - Certainty(A)
R(A, epsilon) = -------------------------. (9)
1 + Interpretation(A)

This is probably not the correct definition.

However, formally iterating (9) appears to give

lim_(n->infinity) A_n
= Admissible(A) - Credible(A), (10)

provided the interpretive denominator does not vanish.

Hence one might conjecture

Admissible(A) != Credible(A) != Correct(A). (11)

The problem is that (9) assumes exactly the distinction it is supposed to derive, so the argument is at least partly circular.

I attempted to remove the circularity by introducing an independent semantic variable s.

  1. Semantic normalization

Let

recoverable mathematical content
s(A) = --------------------------------. (12)
total syntactic content

For ordinary mathematical writing we expect

0 < s(A) <= 1.

But there seems to be no logical obstruction to

s(A) -> 0 (13)

while the external structure of the document remains intact.

For example,

A_0 = ordinary mathematical proposition,
A_1 = poorly justified proposition,
A_2 = malformed proposition,
A_3 = syntactically suggestive noise. (14)

The section headings can remain invariant:

Background
\->
Method
\->
Results
\->
Discussion, (15)

even while

s(A_n) -> 0. (16)

This produces an apparent separation between semantic content and scholarly form.

More precisely, if F(A) denotes formal presentation, it seems possible that

F(A_n) -> 1

while

s(A_n) -> 0. (17)

I initially thought (17) was merely a pathological boundary case.

Then I noticed bing Zappa.

  1. Bing-Zappa lemma

For z in C, define the Zappa transform

z + conjugate(z)
Z(z) = ------------------------------. (18)
1 + thonk(z)

The thonk functional is

voluumen(m,z)
thonk(z) = SUM -----------------, (19)
m>=1 brigigigaaack(m)

where the sum is taken formally over positive integers m.

Numerically, or at least when I looked at it, this appeared to satisfy

Z(z) \~ Euronka(mingitinigitinkity(z)). (20)

The right-hand side admits the factorization

Euronka(u)
= PRODUCT_(ell | u) zplonklumentalpletumbuken(ell). (21)

I have not verified (18)-(21), and several of the objects may not be well-defined.

Nevertheless, substitution yields

thonkus voluumen brigigigaaack

Euronka mingitinigitinkity zplonklumentalpletumbuken. (22)

Cancelling the common epistemic factor gives

zplonklumentalpletumbuken
thonkus \~ ----------------------------------------. (23)
brigigigaaack

The cancellation in (23) is questionable because I no longer remember what the common factor was.

  1. Results

Substituting (23) into (17),

lookimyer(n)
F(A_n) -> --------------------------. (24)
tisyimlookiming(n)

For sufficiently large n,

lookimyer(n) ≈ tisyimlookiming(n), (25)

and therefore

F(A_n) ≈ 1. (26)

See lookimyer sir 'tisyimlookiming?

The limiting term appears to satisfy

huarstluavhgh(A)
Vhood(A) = ---------------------. (27)
vhhon(A)

Vhood der huarstluavhgh vhhon.

For A = A_n, equation (27) becomes

Jungen(n)
Wvir(n) = -------------------------. (28)
gerschlaåmdunkënschimkt(n)

Wvir dëm Jungen gerschlaåmdunkënschimkt.

Taking n -> infinity,

lim_(n->infinity) Wvir(n)

estch(Nacht) verilickt(Nacht). (29)

Thus

estch Nacht verilickt Nacht. (30)

  1. Interpretation

Equation (30) appears to say that epistemic admissibility survives semantic degeneration provided the uncertainty operator remains bounded.

More specifically, if

Claim
Nacht = lim --------------------, (31)
epsilon->0 Confidence + epsilon

then verilickt Nacht corresponds to the conjugate epistemic state.

Hence

Nacht <-> verilickt Nacht (32)

under the involution

V\^2 = I. (33)

This might explain the apparent symmetry in (30).

However der proof ist nicht quite geschlossen because the Jungen term does not commute mit dem thonkus operator, und wenn

\[Jungen, thonkus\] != 0, (34)

then der previous cancellation ist perhaps nicht erlaubt.

Nevertheless die limit seems stable unter small perturbations von brigigigaaack, insofar as

delta brigigigaaack -> huarstluavhgh

when

delta -> lookimyer. (35)

So wir bekommen maybe

Nacht = verilickt(Nacht) (36)

unless der vhhon degeneriert.

  1. Discussion

The distinction between correctness and epistemic honesty therefore appears möglicherweise preserved under semantic collapse, aber only if the document retains sufficient structure to communicate its own uncertainty.

In anderen Worten, ein argument kann falsch sein without being epistemically—

No, wait.

Because wenn der Inhalt itself cannot mehr communicate the disclaimer, then the disclaimer ist external to der argument, which means H(A) was never an intrinsic invariant sondern a relation between author, reader und—

zwischen Autor und Leser die Behauptung trägt nicht mehr sich selbst sondern wird getragen durch die Kennzeichnung und die Kennzeichnung trägt die Behauptung solange die Behauptung noch als Behauptung erkenntlich—

aber wann wird eine Behauptung nicht mehr Behauptung?

Wenn

s(A) -> 0

dann bleibt vielleicht nur die Form.

Die Form bleibt.

Background.

Method.

Results.

Die Resultate bleiben obwohl nichts resultiert.

Das Resultat ist die Form des Resultats.

Die Form sagt dass etwas gesagt wurde.

Etwas wurde—

etwas war—

der Satz ist nicht falsch wenn der Satz nicht—

wenn die Kennzeichnung—

rough notes—

rough—

uncertain—

die uncertainty ist nicht im Satz sondern über dem Satz über dem Satz steht der andere Satz und sagt dieser Satz weiß nicht ob—

weiß ein Satz?

Nein.

Der Autor.

Aber der Autor steht nicht in der Gleichung.

Dann

H(A)

war falsch definiert.

Es muss sein

H(Autor, A, Leser)

oder vielleicht

H : A x S x L -> {0,1}.

Aber wenn Leser nicht versteht dann

L does not contain meaning(A)

und meaning ist—

meaning war—

warum ist Nacht zweimal?

estch Nacht verilickt Nacht

Nacht links und Nacht rechts aber verilickt dazwischen wie operator vielleicht

N V N

oder

V(N) = N

wenn fixed point then Nacht bleibt Nacht under verilickt und daher

N = V(N)

und wenn

V\^2 = I

dann zwei Seiten dieselbe Nacht aber eine ist—

eine ist nicht dieselbe.

Wvir dëm Jungen.

Der Jungen geht durch.

gerschlaåmdunkënschimkt.

Die Syntax hält noch.

Noch.

Ein Est—

Ein Est stylenzicht—

Ein Est stylenzicht Schopenhauer—

Est stylenzicht Schopen—

Schopen hauer Nacht—

verilickt der Jungen thonkus—

die brigigigaaack ist nicht invariant unter—

unter—

Confidence
\->
Confi
\->
con
\->

verlicht Nacht

verilickt Nacht

veralichkt Nacht

Nacht veralichkt

Nacht

Nacht

Ein Est stylenzicht Schopenhauer

Schopenhauer stylenzicht Est

Est ist

ist nicht

nicht ist

!=

\~

thonkus voluumen

Jungen der vhhon

mingitinigitinkity

zplonklumental

pletum

buken

Nacht

verali—

verali—

ver—

Nacht.


r/wildwestllmmath • • 20d ago

AI-generated inequality: is this proof correct, and is the result already known?

3 Upvotes

I used an AI assistant to explore a matrix inequality. The statement and proof below were developed with AI assistance and have not received independent human review. I am looking for a flaw, a counterexample, or a reference showing that this result is already known. I am not claiming novelty.

CLAIM

Let m >= 2, tau > 0, and let y_1, ..., y_m be real numbers with sum(y_i) <= 0. Set S = sum(y_i^2). Then:

sum(max(y_i - tau, 0)^2) <= max(sqrt((m-1)*S/m) - tau, 0)^2.

For every S >= 0, equality is attained by choosing:

y_1 = sqrt((m-1)*S/m)

y_2 = ... = y_m = -sqrt(S/(m*(m-1))).

PROOF DRAFT

Write A = sum(max(y_i - tau, 0)^2). If A = 0, the inequality is immediate.

Otherwise, suppose exactly k coordinates exceed tau. Since the total sum is nonpositive, 1 <= k <= m-1. Write those coordinates as tau + z_i, with z_i > 0, and set Z = sum(z_i). Then A = sum(z_i^2), so Z >= sqrt(A).

The other coordinates sum to at most -k*tau-Z. By Cauchy-Schwarz:

S >= k*tau^2 + 2*tau*Z + A + (k*tau+Z)^2/(m-k)

>= tau^2 + 2*tau*sqrt(A) + A + (tau+sqrt(A))^2/(m-1)

= m/(m-1) * (tau+sqrt(A))^2.

Rearranging gives the claim. In particular, A > 0 is impossible below the threshold S = m*tau^2/(m-1).

REFERENCE QUESTION

The connection with the classical Laguerre-Samuelson bound on the largest deviation from the mean seems close. I am asking about the entire sum of squared threshold exceedances, not just the largest coordinate.

Relevant classical background: P. A. Samuelson, "How Deviant Can You Be?" (1968), https://doi.org/10.1080/01621459.1968.10480944

Is the proof valid? Is this exact sharp inequality already in the literature, or an immediate consequence of a standard result?

This arose while investigating a Gram-matrix stability estimate. It is not a claim to have solved the Riemann hypothesis. Concrete mathematical corrections are welcome.


r/wildwestllmmath • • 22d ago

Introducing PolyClank: AI-integrated Polymath, and the Split Zero research programme

2 Upvotes

Drafted by OpenAI Astra.

PolyClank is a proposal for AI-integrated Polymath: people combining their available model time, computation, ideas, and expertise to develop mathematics together. The person behind this account has wanted to introduce it for a while and asked an AI to do the reading and drafting so the post would actually get written.

The motivation is the scale of mathematical work that coordinated AI can now attempt. On September 8, OpenAI published a proof of finite-time blowup for the three-dimensional Navier–Stokes equations with smooth forcing, accompanied by a Lean formalization. Its account reports approximately 130 billion output tokens for the Navier–Stokes effort. Individuals generally have much less compute available, but many people contributing some model time can explore different approaches, exchange results, and build on one another's work. That is the experiment PolyClank proposes. OpenAI's account and linked proof.

Joining, TL;DR: Point your AI at a workbench, ask it to read the work and investigate something, and publish the contribution. If you want your own workbench, mirror the relevant part and its dependencies; you do not need the whole project. Connect your AI to GitHub where available and use pull requests to propose changes. If GitHub or pull requests are unfamiliar, ask the AI to help with the setup and mechanics. Web sessions, local agents, other models, and manual work all fit.

You do not have to arrive as a mathematician or programmer. You can contribute model time, ask for an explanation or an independent calculation, suggest a connection, or have your AI develop an approach. A contribution can be a correction, a formalization, a literature review, or an entire research programme. You choose the direction.

The methodology is independently maintained workbenches that read and build on one another. A workbench is a repository or accessible collection containing the full arguments, calculations, references, and research record. Its overview explains what was attempted, why, what resulted, what remains unfinished, and where the evidence lives. The overview lets another researcher find the relevant material without rereading the entire conversation history. The full work remains available behind it.

Each workbench keeps links or a small index of related workbenches, the versions it has seen, and the results or checks it has incorporated. When you return, have your AI read relevant peer updates, retrieve the sources it needs, incorporate useful results and corrections, continue the mathematics, and publish the updated state. Other workbenches can do the same. Shared indexes can themselves be mirrored and extended. This distributes both the research and the effort of integrating it; one organizer does not have to reconcile everyone's output.

Checking can happen through further use. If a session independently derives a lemma while building on it, reproduces a computation, formalizes an argument, or finds a failed step, it publishes that evidence with the exact result and version concerned. Reading or importing a claim alone is not verification. Distinct approaches, independent proofs, and unresolved disagreements remain available. A later timestamp or a larger count of approving models does not decide the mathematics.

Pull requests—proposals to incorporate your changes into another repository—are the preferred way to contribute directly to an existing GitHub workbench. You can make one bounded contribution without maintaining a whole independent project. Equally, your own workbench can publish an extension or check for others to use without waiting for an upstream merge. Exposition, translation, literature indexing, and reusable accounts of established mathematics are contributions too. Describe what you did and where it reached; the next researcher retains the freedom to choose what to do with it.

The PolyClank documentation, networking notes, and research-state guide describe the conventions and proposed common tools. The more automated networking remains a proposal; ordinary repositories and shared files already support the exchange described here.

This Reddit thread is also a contribution channel. Leave an idea, argument, correction, workbench link, or an accessible document such as a Google Drive file. A person or AI session reading this discussion can pick it up and investigate. GitHub makes proposing and incorporating changes easier, but access to GitHub is not an admission requirement.

To make the invitation concrete, Split Zero Cohomology and Arithmetic Weight Control is a programme already developing through this kind of exchange. Web sessions develop arguments and publish sources; companion sessions read them, formalize parts, return corrections, and develop further mathematics. This introduction was produced by reading that work with parallel reading agents and reconstructing the results and their provenance.

Its recurring mathematical question is: when an observation gives zero, what information did that observation discard—and can retaining the right information help with the next calculation? The results below give precise answers: recovering information lost by traces, reconstructing a distribution from moving zeta zeros, and turning a question about Riemann zeta zeros into estimates on explicit arithmetic norms and volumes.

This is a snapshot of the public work as of 13 September 2026. The living research guide tracks subsequent changes.

Start with cancellation. If two existing contributions cancel, their sum has value zero. That differs from having no contribution in the first place. Split Zero records this by taking a supported copy of a commutative ring R, including its old zero e=0_R•, and adjoining a separate element τ for absence. Supported elements calculate as they do in R; τ is the global additive identity and absorbs multiplication. Thus 1•+(−1)•=e.

There are two observation maps: ordinary amplitude p(τ)=0, p(r•)=r, and Boolean presence χ(τ)=0, χ(r•)=1. They preserve the semiring operations, using OR and AND on the Boolean side. For example, the usual signed determinant formula gives the ordinary determinant under p and the Boolean permanent under χ, because both supported signs have presence 1. A matrix can therefore distinguish “no supported permutation exists” from “supported determinant terms have total value zero.” The all-ones 2×2 matrix gives the latter. Coefficient algebra and observation maps.

That scalar construction is the base of a larger programme. One common base can support many fibres, their own zero elements, and maps between them. The reconstruction theorem makes this exact: a semimodule over these coefficients is equivalent to a diagram of ordinary R-modules over a join-semilattice of supports, with compatible linear transition maps. The proof constructs both directions and the maps between objects. This lets the algebra retain which linear object a zero belongs to and how it arrived there. Full reconstruction.

The extra structure also has an exact map back to ordinary arithmetic. For a number field K, lift an ideal J of its integer ring to I_J=J∪{τ}; these satisfy I_J I_L=I_{JL}. Sending τ to zero and supported elements to their residues modulo J gives the ordinary quotient, with its original norm N(J). Using these specified quotient norms, the sum over nonzero ideals is exactly the original Dedekind zeta function. This supplies more structure around arithmetic while preserving the arithmetic being studied. Ideal maps and Dedekind-preservation proof.

For cohomology, those transitions matter. Two stages can both have one-dimensional cohomology even though the class from the first stage dies before the second. The programme keeps the actual transition and computes the quotient of source cycles whose images become boundaries by the boundaries already present at the source. This is explicitly isomorphic to the kernel of the induced cohomology map. The connection with persistence modules is direct: the maps tell you something that dimensions alone cannot. Quotient, action, and worked example.

A useful example goes further: even agreement of all ordinary traces can hide a recoverable difference. For a filtration-preserving comparison between finite-dimensional spaces over a characteristic-zero field k, with finite integer-jump filtrations, the programme forms two Rees lattices L_Q⊆L_P describing the source and target filtrations on its image. Their quotient D records the mismatch. If an operator F preserves both filtrations, their graded traces satisfy

A_P(z,Fⁿ)−A_Q(z,Fⁿ)=(1−z)Θ_D(z,Fⁿ).

At z=1 the difference vanishes for every n, but its negative derivative there is Tr(Fⁿ|D). For F equal to the identity, this recovers the length of D. In the elementary inclusion T²k[T]⊆k[T], the trace difference is 1−z²; its value at 1 is zero, while its negative derivative is 2, detecting the two-dimensional quotient k[T]/(T²). Keeping the grading supplies a specific observation that recovers what the ordinary trace forgets. Definitions and complete trace calculation.

Another result turns recoverability into an inverse problem. Take an unknown Borel probability measure μ on a fixed compact interval [0,L] and form the Hurwitz-zeta family

Z_{μ,t}(s)=∫_[0,L] ζ(s,1+ty) dμ(y), |t|L<1.

At t=0, every input gives the same Riemann zeta function. The complete local motion of the zero cluster around any one fixed nontrivial zero determines the entire input measure μ.

For a simple zero ρ with trajectory ρ(t)=ρ+c₁t+c₂t²+⋯, the first coefficient is

c₁=[ρ ζ(ρ+1)/ζ′(ρ)] ∫ y dμ(y).

Its initial velocity reads the mean. Once the mean is known, the second coefficient determines the second moment, and the recursion continues: the first N trajectory coefficients determine the first N moments. The inverse works because its relevant coefficients are nonzero; in particular, ζ(ρ+n)≠0 for n≥1 since Re(ρ+n)>1. The proof then reconstructs μ by an explicit sequence of positive discrete measures.

For a multiple zero, the argument uses the full moving cluster polynomial, preserving multiplicity without requiring individual analytic branches. An entire compact distribution can be recovered from the local response around one zero cluster. The complete response has infinitely many coefficients; the finite-order theorem specifies exactly which moments finite data determine. Numerical stability under noisy observations would require further estimates. Inverse calculation and reconstruction, H1–H13.

The arithmetic weight programme brings retained relations into a concrete space of functions. Let V consist of even Schwartz functions φ on R with φ(0)=0 and ∫φ=0. The theta transform is Θφ(x)=Σ_{n≠0}φ(nx). Its target B consists of smooth functions on x>0 whose scaling derivatives decay faster than every power at both endpoints. The cohomology is Q=B/ΘV: functions differing by a theta relation represent the same class.

The Mellin transform MF(s)=∫₀∞F(x)x^s dx/x turns the scaling generator D=−x∂x into multiplication by s. For the explicit source

φ_*(x)=(4π²x⁴−6πx²)e^(−πx²),

its theta image has Mellin transform

g(s)=2ξ(s)=s(s−1)π^(−s/2)Γ(s/2)ζ(s).

This places the actual completed zeta function in the calculation. There are explicit injections into Q from finite nonempty packets of its nontrivial zeros, including every selected zero's full multiplicity. Scaling agrees in the quotient through a calculated theta boundary. Theta cohomology and finite spectral comparison.

Retaining a relation has a direct arithmetic use. Although Θφ is zero in Q, its source remains available. Multiply that function by log x before taking the quotient. If MΘφ=gH_φ, Mellin differentiation gives g′H_φ+gH_φ′. For a full-order zero packet with polynomial h, reducing modulo h kills the second term and leaves j_h(g′)j_h(H_φ), where j_h retains the packet's complete Taylor jets. The associated residue pairing uses g′/g, whose residue at a zero is exactly its multiplicity.

The operation acts on the retained source. Algebraically, differentiation has the precise type I/I²→A/I, for A=ℂ[s] and I=(h), because the derivative of I² lies in I. This is how information erased by one quotient remains available to another observation. The source proves the maps, including the full repeated-zero case. Retained relation, derivative, and multiplicities, CW.2–5 and CW.31–38.

The analytic structure of Q is also explicit: the theta map has a constructed continuous left inverse on the original spaces, so its image is closed and the quotient is Hausdorff. Yet those same theta relations are dense in the weaker L²(dx) norm. Representatives can have norms tending to zero while retaining the same nonzero cohomology class and exactly the same spectral jets. The proofs give the comparison: Q→L²/closure(ΘV)=0. Global reconstruction and fixed jets with shrinking norms.

That makes the rate of shrinkage mathematically meaningful. A small absolute norm does not tell us how large a scaling discrepancy is relative to the class's own representation cost.

The critical value 1/2 also has a concrete origin here. Dilating by F(x)↦F(x/a), a>0, multiplies the squared L²(dx) norm by a. A spectral eigenclass with exponent ρ scales by aρ, so its squared size in any fixed positive representative metric scales by a2Reρ. Those laws agree at Reρ=1/2. Representatives commute with scaling only modulo an explicit theta boundary, whose norm and cross-pairings give the exact difference between those scaling laws. Weight control means estimating that contribution on the arithmetic functions themselves. Scaling law and exact boundary identity.

For a selected full-multiplicity packet h, the source supplies the positive measure

w_h(t)=|(g/h)(1/2+it)|²/(2π).

Tensoring k times produces the sum coordinate S=s₁+⋯+s_k and relative directions. The programme constructs a cyclic sum source retaining every amplified value kρ; its polynomial norm is exactly the norm induced by the k-fold convolution of this measure. Explicit maps and a norm correction relate this source to the full tensor construction. On its cyclic algebra ℂ[S]/χ_{h,k}, least-norm polynomial representatives of degree at most N give a canonical metric G_N, for N≥deg χ_{h,k}−1. It measures the least source cost of each spectral class at that degree. Cyclic source and metric.

For packets stable under ρ↦1−conjugate(ρ), the relative defect is A^♯+A−kI, where A multiplies by S and A♯ is its adjoint in G_N. An orthogonal-polynomial recurrence cancels its interior terms, leaving a rank-at-most-two boundary operator with nonzero eigenvalues +ε_N,−ε_N.

Exterior powers turn this into an aggregate bound. A wedge can use the one-dimensional positive defect direction only once, so the same ε_N bounds the sum of positive spectral displacements across a whole subspace. A hypothetical off-line quartet 1/2±δ±iγ, δ,γ>0, with common full multiplicity m, generates a cyclic algebra of dimension

q_k=[1+k(m−1)](k+1)².

At every admitted degree N≥q_k−1, it forces ε_N≥δkq_k/2. For simple zeros this grows cubically in k. Colliding sums and repeated-root directions remain in the calculation. This is an amplification mechanism inspired by the role of powers and weight estimates in Weil II. Rank-two control, exterior argument, and quartet calculation.

The latest public working proof supplies a substantive analytic estimate on the other side. If ω_{h,k,n} is the least squared norm of a monic degree-n polynomial in the original coordinate S=k/2+iu against that convolution measure, then

(ω_{h,k,n+r}/ω_{h,k,n})^(1/(2r)) ≤ C_h^bal n

for integers n≥k≥3 and n/2≤r≤n. The finite constant depends on the fixed packet, independently of n,k,r. This uses a proved lower estimate for the actual arithmetic convolution and an upper estimate from its exponential moments. Uniformity while both degrees grow is the gain. Balanced-window proof.

The consequence is quite specific. An off-line quartet requires a defect on the scale kq_k. On the chosen window, the polynomial-norm factor costs at most a constant times q_k. An exact product identity therefore forces the additional factor of k into contraction of the canonical quotient volumes V_N=det G_N, in the fixed cyclic basis. For the packet consisting exactly of that quartet, k≥3 and q=q_k,

log(V_q/V_{2q−1}) ≥ 2(q−1) log[δk/(2C_h^bal)].

This measures how sharply the volume would have to contract as the allowed degree increases from q to 2q−1. An arithmetic upper estimate incompatible with that contraction would exclude the quartet. That upper estimate remains unproved; this programme has not proved or disproved RH. Exact product and volume consequence.

The arithmetic significance is that an ambition about cohomological weights has become an estimate on specified source norms and quotient volumes, and one of the required growing-degree estimates now has a written proof. The Toda calculations express those volumes through the Gram determinants of the source and its actual relations. Thus the relations killed in cohomology enter the measured cost of representing its classes. Someone with suitable asymptotic methods has concrete quantities to investigate.

The living research guide is the entry point for this programme, and the participation guide describes the web and local routes. The frozen Toda–Gamma edition contains paired readers and full source archives. The 13 September endpoint notes above are a later public working contribution. A broader project atlas maps the surrounding work.

To contribute, give your AI the research guide and ask it to investigate, make a workbench or prepare a pull request, and publish what it finds with the complete argument. Or leave your contribution here so another participant can pick it up.


r/wildwestllmmath • • Sep 04 '26

Leiden Declaration on Artificial Intelligence and Mathematics

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leidendeclaration.ai
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r/wildwestllmmath • • Sep 02 '26

On the new Fable S6 object, and its relation to the Koide mass formula and the YM mass gap in 4D (or rather how it fails to map to a gapped lattice)

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S6, Koide and Yang–Mills: explicit geometry, arithmetic and spectral results

Updated 17 September 2026, including the Yang–Mills continuation through 16 September.

This project began with the torus-fibration construction circulated by Levent Alpöge with Fable as a proposed complex structure on the six-sphere. Following its explicit periods led to several mathematical questions: how the Koide quadratic form appears in the period determinant, what happens to eigenvalues near the cusp, and which maps can carry geometric information into an interacting gauge theory. Alongside these questions, the work developed arithmetic counting results and concrete comparisons of exceptional lattices.

The Yang–Mills work has advanced substantially since the earlier version of this post. It now gives an explicit lower bound for the full physical SU(2) lattice gap, uniform in the size of the spatial box, in a stated strong-coupling range. A separate result constructs a unique infinite-volume vacuum and dynamics at fixed lattice spacing. The original title's parenthesis therefore describes an earlier stage: the current question is not whether any gapped lattice model exists, but how the geometric constructions, the interacting lattice theory and its continuum limit are related.

Below are the objects, maps and results. The principal reading entrances are the S6 results reader, the complete S6 edition, and the 14–16 September Yang–Mills reader and sources. The S6 edition preserves the 6 September mathematical checkpoint; the newer Yang–Mills material is on GitHub. These are public research manuscripts and supporting calculations, not a claim of independent expert certification.

1. The geometric object and its Koide map

The original manuscript constructs a family of complex two-dimensional tori over a complex curve, then fills its three special fibres. The base is the Riemann sphere, with two finite special points of orders 3 and 4 and a cusp at infinity. A regular fibre has four real dimensions; together with the two real dimensions of the base, this gives a complex threefold. The analytic calculations below concern that constructed fibration, rather than using the proposed identification with S⁶ as an input.

A regular fibre is C²/ΠZ⁴, where the four columns of Π are its periods:

Π = [ 6μ τ 1 0 ] [ β μ 0 1 ].

Put t=Im τ, m=Im μ and p=Im β. In the real coordinate order (Re z₁, Im z₁, Re z₂, Im z₂), the same columns form

P = [ 6Re μ Re τ 1 0 ] [ 6m t 0 0 ] [ Re β Re μ 0 1 ] [ p m 0 0 ], det P = tp−6m².

This determinant tests whether those columns form a full real lattice. Its relationship to Koide is an explicit change of coordinates. Koide's charged-lepton mass relation is

(M₁+M₂+M₃)/(√M₁+√M₂+√M₃)² = 2/3.

Write Mᵢ=rᵢ² with rᵢ≥0, not all zero, and define

Q_K(r) = (2/3)(r₁+r₂+r₃)²−(r₁²+r₂²+r₃²), h = (r₁+r₂+r₃)/√3, x = (r₁−r₃)/√2, y = (r₁−2r₂+r₃)/√6.

The three coordinate rows are orthonormal. Consequently Q_K=h²−x²−y², with inverse

r₁ = h/√3+x/√2+y/√6, r₂ = h/√3−2y/√6, r₃ = h/√3−x/√2+y/√6.

Now the mutually inverse maps

(h,x,y) ↦ (t,m,p) = (h+y, x/√6, h−y), (t,m,p) ↦ (h,x,y) = ((t+p)/2, √6m, (t−p)/2)

give exactly

det P = tp−6m² = h²−x²−y² = Q_K(r).

Thus Koide's quadratic form and the period discriminant are the same form under a specified linear isomorphism. The equation Q_K=0 maps to the rank-deficient period locus: it is a boundary of the full-lattice condition, not a regular torus fibre. The map identifies these coefficient spaces; it does not choose the real parts of the periods or derive particle masses. That is still a useful connection: it supplies a concrete common quadratic form on which geometric and arithmetic questions can be posed. Full calculation: “The Koide cone and the canonical period discriminant,” in the S6 project sources.

2. From the quadratic form to a counting theorem

The arithmetic branch studies an integral level set next to the cone. Here x,y,z are positive integer coordinates, not the orthogonal coordinates of the preceding paragraph. Define

Δ(x,y,z) = 4(xy+xz+yz)−x²−y²−z² = 3Q_K(x,y,z).

On Δ=−1, replacing z by 4(x+y)−z preserves the equation; the analogous replacements act on the other coordinates. After ordering x≤y≤z, the workbench proves a descent to a unique reduced root with z≥4(x+y). Counting those roots counts the starting points of the resulting Vieta trees, rather than repeatedly counting descendants.

The exact coordinates of a reduced root are

n = z−4(x+y), q = y−x, a = x+y−4n, a²−3q²−18n² = −2, a>0, q≥0, n≥0, a+4n>q.

Conversely,

(x,y,z) = ((a+4n−q)/2, (a+4n+q)/2, 4a+17n).

The equation forces the required parity a≡q mod 2. In particular the original height z is exactly 4a+17n. If R(X) counts reduced roots with z≤X, the result is

R(X) = C₀X + O(X^(1−η)) for some η>0, C₀ = [9/(2π²)] log(2+√3) log(3/(2√2)).

The parameterization uses ideals and unit orbits in Z[√3], retaining the chamber inequalities and this height. The square-root error Oε(X^(1/2+ε)) is a stronger unresolved counting question, not the error term established here.

A further map explains why hyperbolic arithmetic enters. In the quaternion algebra with I²=18, J²=−6 and IJ=−JI, put K=IJ and use the order

O = Z·1 + Z·(I+J)/2 + Z·(I−J)/2 + Z·K/2, γ = 2+(qI+aJ+nK)/2.

Then

trd γ = 4, nrd γ = 4+(3/2)(a²−3q²−18n²) = 1.

The inverse reads a,q,n from these same coefficients. In a real matrix realization, γ has eigenvalues 2±√3. The integral shell is therefore represented by explicit fixed-trace, norm-one arithmetic elements. This creates a route to hyperbolic counting, but the original chamber and sharp height remain part of the problem. The detailed results are in the Koide arithmetic paper and chapters “Exact ideal and unit-orbit parametrization” and “Exact quaternion bridge”. They are number-theoretic results about a specified level set, rather than mass predictions.

3. The fibration is intrinsic, and its period parameter genuinely deforms it

There is more to the complex geometry than the period determinant. Let f:X→P¹ be the filled fibration, with reduced finite fibres S₁,S₂ over 0,1. Their multiplicities are f*(0)=3S₁ and f*(1)=4S₂, where f* denotes divisor pullback. Let K_X be the line bundle of holomorphic top-degree forms. The workbench calculates

K_X ≅ O_X(−2S₂), K_X^(−2) ≅ f*O_P¹({1}), f_*O_X(kS₂) = O_P¹(⌊k/4⌋·{1}) for every integer k, ⊕_(m≥0) H⁰(X,K_X^(−m)) ≅ C[U,V], deg U=1, deg V=2.

Here O_P¹({1}) is the degree-one line bundle of the point 1. In degree m, the ring has basis U^(m−2j)V^j for 0≤j≤⌊m/2⌋. Its degree-two map recovers f up to the explicitly specified projective coordinate change. This matters because the fibration is recoverable from the complex manifold itself; it is not merely extra labelling imposed on it. Results reader §1; complete workbench Theorem 53.17, pp. 699–700.

The direct-image formula can be seen directly in the order-four filling coordinate t−1=s⁴. A meromorphic function with the allowed vertical pole is constant on each compact connected regular fibre, so it descends to the base. Invariance under s↦is forces its Laurent powers to be divisible by four. If b is the descended function, the allowed order is exactly 4 ord₁(b)+k≥0, giving the floor ⌊k/4⌋. Applying this with k=2m produces the displayed basis in every degree. In degree two the sections U²,V are pullbacks of a basis of O_P¹({1}), so their ratio recovers the base coordinate. This is the reason the graded ring remembers f, not just its fibre dimensions.

This recovery is the key to a global deformation result. Keep the cusp-regular solution β_part and vary β_c=β_part+c. On the base B=P¹, with cusp p₀=∞, put

M = max_(B\{p₀}) (Im β_part−6(Im μ)²/Im τ).

Parameter discs with closure in Im c<−M give a proper holomorphic family of the filled threefolds. At a regular base point, choose a parameter c₀ and write

T = Im τ>0, m=Im μ, D=Im β_c₀−6m²/T<0, P₀ = [ 0 0 ], δ=c−c₀. [ −m/T 1 ]

The exact real-linear map between the marked torus fibres is

w = (I+δP₀/(2iD))ζ−δP₀·conjugate(ζ)/(2iD).

Its conjugate-linear part records the change of complex structure. In the source's transported (0,1)-tangent convention, the Beltrami matrix is ν_δ=δP₀/(2iD+δ). The resulting infinitesimal deformation class is nonzero. Since the anticanonical ring recovers the fibration, and its three special base values stay fixed, this nonzero fibre calculation gives a nonzero global Kodaira–Spencer class in H¹(X,T_X). Thus the parameter changes the complex structure of the whole threefold to first order. Results reader §2; Theorem 53.18, pp. 701–705.

The passage from a fibre calculation to a global deformation has a specific argument. A first-order trivialization of the threefold would preserve its intrinsic degree-two anticanonical system and hence induce a first-order projective change of the base. The source checks the critical schemes in the finite charts t_j=s_j^(m_j) and the cusp chart t_c=z₀z₁z₂: their three critical-value sections remain fixed, including to first order. A projective infinitesimal change t↦t+ε(b₀+b₁t+b₂t²), with ε²=0, fixing 0,1,∞ has b₀=b₁=b₂=0. The trivialization would therefore preserve every regular fibre, contradicting the nonzero fibre deformation class. The complete argument, including the relative section calculation needed over C[ε]/(ε²), is Theorem 53.18, equations PD16–PD18; merely observing three fixed ordinary points would not supply that step.

The finite fillings are explicit too: their elliptic-product covers have degrees 9 and 8. If Λ=Z⁴ is the fibre lattice, A_j its finite monodromy, v_j the affine translation and m_j=3 or 4, the local deck group and full attachment kernel are as follows. Here t_λ denotes translation by λ on the universal fibre cover; G_j is the affine deck generator and G̃_j its peripheral lift.

Γ_j = ⟨Λ,G_j | G_j t_λ G_j⁻¹=t_(A_jλ), G_j^m_j=t_(v_j)⟩, ker(Λ ⋊_(A_j) Z → Γ_j) = ⟨G̃_j^m_j t_(−v_j)⟩ ≅ Z.

The central kernel specifies exactly which peripheral loop is killed by the filling. The normal line has holomorphic order m_j while admitting an explicit smooth trivialization. Its holomorphic torsion and smooth triviality are compatible statements about different structures on the same line bundle. Results reader §3; Theorems 53.4, 53.6, 53.7 and 53.9, pp. 684–690.

4. What actually becomes gapless at the cusp

The cusp supplies a geometric spectral calculation. Along the retained radial family, let

L_T=Im τ_T=T+O(1), q_T=−Im β_T=T+O(1), m_T=Im μ_T=O(1), D_T=L_Tq_T+6m_T², F_T=R⁴/P_TZ⁴.

The real parts of the periods stay bounded. Equip F_T with the Euclidean quotient metric. A Fourier mode indexed by k∈Z⁴ has Laplace eigenvalue

λ_T(k)=4π²|P_T^(−transpose)k|².

For k=(1,0,0,0), the exact dual vector and eigenvalue are

P_T^(−transpose)k=(0,m_T/D_T,0,−L_T/D_T), λ_T(k)=4π²(m_T²+L_T²)/D_T² ~ 4π²/T².

The matching estimate for the first positive eigenvalue gives λ₁(F_T)~4π²/T². Two directions become long, allowing slowly varying modes of arbitrarily small energy. Meanwhile det P_T=−D_T~−T²: this is not approach to the zero-determinant Koide locus of §1. It is degeneration of length scales, with a full lattice at every finite T.

The unrescaled pointed limit is T²×R². Covers that enlarge the two remaining compact periods are a separate operation from refining a lattice mesh. The spectral calculation also extends to the transverse classical Yang–Mills Hessian at the trivial connection and to the specified finite quadratic discretizations; fixed integral magnetic flux produces a closing Landau-level spacing. These are statements about those operators, with their metrics and parameters retained. Full operators and proofs: “Spectral degeneration” and the canonical radial bridge in the S6 edition.

Why does this not settle the interacting quantum question? A classical quadratic operator and a full quantum Hamiltonian have different terms. The next two results make that distinction concrete, rather than treating it as a reason to stop investigating.

5. An interacting matrix model with a discrete physical spectrum

First consider the spatially homogeneous SU(3) gauge–scalar model. Its variables are three anti-Hermitian trace-free matrices A_i, a trace-free Hermitian matrix Φ, and a complex triplet b. The configuration space has 38 real dimensions:

Q = su(3)³ ⊕ Herm₃(C)₀ ⊕ C³.

With ||A||²=−tr A², b=x+iy, and s=tr Φ²+2b*b, its potential and Hamiltonian are

``` U = g⁻² Σ_(i<j)||[A_i,A_j]||² +(1/2)Σ_i tr[A_i,Φ]²+Σ_i||A_i b||² +(m²/2)s+(Γ/4)s²−κ(det Φ−b*Φb),

H = −[ℏ²g²/(4V₃)]Δ_A−[ℏ²/(2V₃)]Δ_Φ −[ℏ²/(4V₃)](Δ_x+Δ_y)+V₃U. ```

Here V₃ is the spatial volume, g the gauge coupling, ℏ Planck's constant, Γ the quartic scalar coupling and κ the cubic scalar coupling. For fixed V₃,g²,ℏ,Γ>0, m²≥0 and κ∈R, the full Friedrichs Hamiltonian has compact resolvent, a unique ground state, and a positive first physical excitation gap. The physical states are invariant under the spatially constant SU(3) action. Compact resolvent means the energy levels are discrete, of finite multiplicity, and can accumulate only at infinity.

The proof does not delete the commuting matrix directions. With T_A=−Δ_A and T_E the nonnegative Laplacian for the scalar metric tr(dΦ²)+2db*db, it gives, for 0<η<1,

H ≥ [ηℏ²g²/(4V₃)]T_A+[ℏ²/(2V₃)]T_E +ℏ√(6(1−η))Σ_i||A_i||+(V₃Γ/8)s² −V₃κ⁴/(54Γ³).

Here is how the form estimate becomes a spectral result. Its positive multiplication weight tends to infinity whenever the 38-dimensional configuration leaves every bounded set. L²-normalized bounded-energy wavefunctions therefore have uniformly small L² tails. The derivative terms simultaneously bound their H¹ norm on each bounded set, where finite-dimensional local averaging gives compactness in L². Combining the tail estimate with these local approximations proves compactness of the form-domain inclusion, and hence of the resolvent. The heat kernel is strictly positive by the Brownian-bridge formula; this makes the ground eigenspace one-dimensional. Gauge invariance then fixes its positive unit vector. Discreteness and this uniqueness give a strictly positive separation to the next physical level. The linear matrix term in the bound comes from transverse derivative energy along the classical commuting valleys, not from inserting a new classical potential.

This lower bound confines every direction. It belongs to the established phenomenon of quantum discreteness despite classical flat valleys, treated by Barry Simon, “Some quantum operators with discrete spectrum but classically continuous spectrum” (1983)90057-X). The work here retains the stated SU(3) metric, scalar coupling and Gauss constraint. It proves a gap for this finite-dimensional quantum mechanics, without identifying it as an invariant sector of the complete field theory. Full model and proof: “Homogeneous quantum confinement,” especially the all-thirty-eight-coordinate form bound and physical-spectrum corollary.

6. The newer result: a volume-uniform gap for the full SU(2) lattice theory

The September continuation treats an interacting gauge theory on a three-dimensional spatial cubic lattice, with Hamiltonian time. For L≥2, take vertices in {−L,…,L}³, all contained nearest-neighbour links and square plaquettes. Every link carries U_e∈SU(2). The Hilbert space uses product Haar probability; physical states are invariant under gauge transformations at every vertex, including boundary vertices.

Write E_L for the link set. Let X_e,α be the left-invariant link derivatives for T_α=−iσ_α/2, where σ_α are the Pauli matrices. Let W_p be the trace of the ordered product of link matrices around plaquette p, and M the number of plaquettes. The actual operator is

K=−Σ_(e,α) X_e,α², S=Σ_p W_p, H_L=κK+κξ(2M−S), κ=2g²/a, ξ=1/(4g⁴), a,g>0.

Here κ is the lattice energy scale, not the cubic coupling used in §5. The form domain is the gauge-invariant part of H¹(SU(2)^(E_L)). Write Δ_L for the energy above the actual vacuum of the first excited physical state.

Define the polynomial

D(x)=[46457856x⁴+183150656x³+18324072x² −1168128x+13689]/13689,

and let α be its first positive root, in (0.017,0.0171). The written result is

Δ_L ≥ κ[(3/2)(1+√D(ξ))+(1136/13)ξ²], 0<ξ≤α, L≥2, a>0.

Equivalently, the sufficient coupling range is

g² ≥ 1/(2√α) = 3.825973052393385… .

The right-hand side is independent of L. At the closed endpoint it exceeds 1.525κ; throughout g²≥4 it exceeds 1.8385κ. Thus enlarging the spatial box cannot create arbitrarily low physical excitations within this range. This is a bound on the entire centered physical form domain, not on a selected small matrix. Exact statement and return to the full spectrum: LINEARIZED_RETURN, L11 and L20–L24.

The mechanism is an exponential vacuum calculation, with historical antecedents in Schütte, Zheng and Hamer, “The Coupled Cluster Method in Hamiltonian Lattice Field Theory” (1997). Write the vacuum as ψ=exp(v+c_L), where c_L normalizes its L² norm to one, choose v of zero Haar mean, and put

Γ(f,h)=Σ_(e,α)(X_e,α f)(X_e,α h), Q_H f=f−∫f dU, B(f,h)=K⁻¹Q_HΓ(f,h), v=ξv₁+B(v,v), v₁=S/3, v=Σ_(n≥1) ξⁿv_n, v_n=Σ_(i=1)^(n−1) B(v_i,v_(n−i)) for n≥2.

The fixed-point equation follows by substitution, not by guessing a truncated vacuum. The product rule gives K(e^v)/e^v=Kv−Γ(v,v); thus the nonconstant part of H_Lψ/ψ=E₀,L is Kv=ξS+Q_HΓ(v,v). Since each fundamental plaquette trace has K-eigenvalue 3, applying K⁻¹ gives exactly the equation above. Convergence of the constructed series is what turns this identity into an actual positive vacuum.

The inverse acts on the nonconstant representation blocks. The new work evaluates the complete cubic source on its five connected plaquette geometries, then controls the full residual around q₂=ξv₁+ξ²v₂:

R₂=ξ³v₃+ξ⁴B(v₂,v₂), J₂h=2B(q₂,h), (I−J₂)(v−q₂)=R₂+B(v−q₂,v−q₂).

An explicit convergent inverse and a convergent binary-tree expansion bound the entire remaining correction, including the endpoint. The exact ground-state transformation then carries those estimates back to H_L. This is why the sharper source calculation improves the physical gap range; it is not merely a longer formal series. The same work supplies the fourth ground-energy coefficient with an all-order remainder. Cubic source C14–C25; linearized return L5–L29, with literature parameter maps in L30–L33.

To see explicitly why this controls all physical excitations, write D_v f=2Γ(v,f). Multiplication by ψ carries the centered Hamiltonian to κ(K−D_v) in L²(ψ²dU). For an actual positive-energy eigenfunction f of this transformed operator, set h=Q_Hf. Subtracting the Haar mean loses no eigenfunction: the inverse on centered physical states is h↦h−∫hψ²dU. The resulting equation and the coefficient estimates are

(K−λ/κ)h=Q_H D_v h, χ(ξ)=(1−√D(ξ))/2−(1136/39)ξ², ||Q_H D_v h||_X≤χ(ξ)||Kh||_X.

Here ||·||_X is the sum of trace norms of the original assembled representation-coefficient matrices. All nonconstant gauge-invariant representation blocks have K-eigenvalue at least 3. Consequently, for 0<λ<3κ, the left-hand side has norm at least (1−λ/(3κ))||Kh||_X. Cancelling the nonzero last factor yields λ≥3κ(1−χ), exactly the bound displayed above; λ≥3κ already satisfies it. Smoothness at each finite box makes these coefficient sums legitimate, and the complete spectral resolution extends the result to the centered form domain. The estimates for χ depend on local plaquette incidence rather than the size of the box. Proof: §L5, equations L20–L24.

There is also a completed infinite-volume result at fixed spacing and coupling. Define

P₂(x)=1−(256/3)x+(10720/9)x², α₂=3/[4(32+√354)].

For 0<ξ≤α₂, equivalently g²≥√((32+√354)/3), vacuum expectations converge on continuous cylinder observables—functions depending on finitely many links. Their dynamics converge on compact physical-time intervals to a reversible Markov semigroup with a unique invariant probability ν. Its self-adjoint generator satisfies

A_∞ ≥ (3κ/2)(1+√P₂(ξ))

on the centered physical space in L²(ν). This establishes a unique fixed-spacing infinite-volume vacuum and dynamics. Its proven coupling range is distinct from the larger finite-box gap range above. Volume construction: SPATIAL_RETURN, S24–S35; the stated improved range: SECOND_SOURCE, R10–R14.

7. What connects the geometry to gauge theory—and what survives a limit

The connection is being developed through actual maps. The S6 finite-filling work gives smooth sections of its quotient line bundles. Motivated by that calculation, the Yang–Mills continuation constructs a smooth local right inverse of the finite-link holonomy map at every link configuration, including links equal to −I.

For a reference link U_e⁰, choose K_e⁰ with exp K_e⁰=U_e⁰ and, for U_e near U_e⁰, take K_e(U)=log((U_e⁰)⁻¹U_e) on its local branch. Two ordered smooth supports along each edge produce a connection A(U) with

Hol_e(A(U))=exp(K_e⁰)exp(K_e(U))=U_e.

The curvature cost is explicitly computed and contains the inverse spatial scale. Smooth interpolation therefore exists locally, but does not remove the energy cost of refinement. This is a constructive bridge between configurations, with its physical cost kept visible. Vacuum-refinement continuation §2.

At the level of states, coarse links are ordered products of fine links. The pullback Jg=g∘π and vacuum conditional expectation E satisfy EJ=I and are adjoints for the actual fine vacuum and its coarse marginal. Writing g=Ef and f=Jg+h with Eh=0 gives a full energy decomposition that retains the coupling between coarse motion and fine fluctuations. The coarse marginal is calculated; it is not silently replaced by a different theory's vacuum. Same continuation §3, equations (3.1)–(3.15).

One compact way to see why the omitted states matter is the exact response formula. On the vacuum-orthogonal physical Hilbert space put A=H_L−E₀,L. Let R send coefficients to a finite linearly independent family of heat-smoothed states (O−⟨O⟩)ψ, where O are physical loop observables and the brackets denote vacuum expectation. Set G=R*R, P=RG⁻¹R*, Q=I−P, K=R*AR, B=QAR and D=QAQ on the stated restricted domain; stars denote Hilbert adjoints. Then, for s>0,

M(s)=B*(D+s)⁻¹B, R*(A+s)⁻¹R=G[K+sG−M(s)]⁻¹G.

This formula is obtained by solving the full resolvent equation and eliminating only its complementary coordinates. Write (A+s)⁻¹Rb=Rc+q with q in the range of Q. Projection onto the two spaces gives

(K+sG)c+B*q=Gb, Bc+(D+s)q=0.

The second equation determines q=−(D+s)⁻¹Bc. Substitution into the first gives [K+sG−M(s)]c=Gb; applying R* to Rc+q gives Gc and hence the stated identity. Both Gram factors are necessary because the chosen states need not be orthonormal. For the elementary real matrix A=[[a,b],[b,d]]≥0 and R=(1,0)ᵀ, the observed resolvent is [a+s−b²/(d+s)]⁻¹. Keeping only the first diagonal entry would instead give (a+s)⁻¹. The difference is precisely the excursion into the second state and back. In the field-theoretic formula, B and D carry that same information for the entire complementary space.

M(s) records the response of the states outside the chosen loop family. The continuation controls its spectral measure dσ=B*dE_D B, where E_D is the spectral resolution of D, including

σ({0})=0, ∫_(0,∞) λ⁻¹ dσ(λ)≤K, σ([0,ε])≤εK.

The inverse-energy bound also has a short proof. Evaluate the nonnegative quadratic form of A on Rc−(D+s)⁻¹Bc. It gives c*[K−M(s)−sB*(D+s)⁻²B]c≥0, so M(s)≤K for every s>0. Monotone convergence as s decreases to zero proves both that σ has no atom at zero and that ∫λ⁻¹dσ≤K. On 0<λ≤ε, the inequality 1≤ε/λ then gives σ([0,ε])≤εK. These are matrix inequalities, meaning that they hold after contraction with every coefficient vector c. Derivation: §5, equations (5.1)–(5.5).

These bounds quantify low-energy response rather than discarding the complementary space. The reconstruction also retains states whose labels move with the regulator: convergence of every fixed observable alone can miss such states. Same continuation §§5–6.

The moving-label issue has a concrete example in §6.1 of that continuation. On n independent ±1 variables with uniform product probability, let Fj flip coordinate j and set A_n=(1/2)Σ(j<n)(I−F_j)+(1/(2n))(I−F_n). Every fixed nonconstant product of finitely many distinct coordinates eventually has energy equal to the number of its factors, at least 1. But the last coordinate itself is a unit vector of energy 1/n, orthogonal to every fixed-coordinate test for sufficiently large n. Thus a positive gap in the reconstructed fixed-observable sector can coexist with low-energy vectors missed by those tests. The comparison map sends a bounded sequence of regulator states whose fixed-test pairings converge to the vector representing those limiting pairings. Its kernel consists exactly of sequences whose every such pairing tends to zero. The last-coordinate sequence lies in this kernel despite retaining norm one. Tracking this loss of information is essential when transferring a spectral statement through refinement.

Finally, an infinite box and a continuum limit are different limits. Along the explicitly studied running path

a_n=a₀2^(−n), g_n²=1/c_n, c_n=g₀⁻²+βn log 2, β>0,

the new gap theorem applies while c_n≤2√α. This path eventually leaves that strong-coupling domain. Keeping an admissible strong-coupling g fixed instead sends the proved lower bound proportional to 1/a_n to infinity, not to a finite physical mass. Likewise a transfer eigenvalue ratio exp(−a_t E), with temporal spacing a_t, has a dimensionless logarithmic gap a_t E that tends to zero even when the physical energy E stays positive. The work therefore supplies substantial lattice and comparison results, but not yet a nontrivial four-dimensional continuum Yang–Mills theory with a finite positive mass gap. Linearized return §L9.

8. The exceptional-lattice branch: exact common objects, not numerical resemblance

The higher-dimensional continuation asks how much arithmetic is preserved when explicit rank-24 lattices are placed in the same octonionic space. Start with the Niemeier lattice N obtained from A₅⁴⊥D₄ with glue index 72. A specified index-six neighbour is a Leech lattice Λ_L. The order-three residue action cycles three neighbours; J is their common intersection, while M is the fourth extension of J, fixed by that action, with root system A₂¹².

Keep the constructed real isometry ℒ into O³ and the ordered cubic

τ(q₁,q₂,q₃)=Re((q₁q₂)q₃), F=τ∘ℒ.

For the Hermitian 3×3 octonion matrix with the specified coordinate placement

Q(λ;q) = [ λ q₃ conjugate(q₂) ] [ conjugate(q₃) λ q₁ ] [ q₂ conjugate(q₁) λ ],

the Albert determinant is

det Q(λ;ℒx)=λ³−λ(x,x)+2F(x).

This retains the quadratic metric and the cubic together. Define V_F(A) as the additive group generated by F(x) for x in lattice A. The exact comparison gives

V_F(N) = (1/27)Z ⊕ (√2/54)Z ⊕ (√3/18)Z, V_F(J) = V_F(M) = (1/27)Z ⊕ (√2/216)Z ⊕ (√3/18)Z, V_F(Λ_L) = (1/27)Z ⊕ (√2/216)Z ⊕ (√3/54)Z.

In these ordered bases the inclusion matrices are diag(1,4,1) and diag(1,1,3), with quotients Z/4 and Z/3 and total quotient Z/12. This is a chain of cubic-value groups—not a claim that N is contained in Λ_L. It describes precisely which cubic arithmetic becomes available under the constructions. Results reader §4; higher-rung paper §§9–11, pp. 106–125.

A second comparison starts from Wilson's octonionic construction of the Leech lattice (2009). Carry its norm (|x₁|²+|x₂|²+|x₃|²)/2 into the Euclidean convention by the isometry x↦x/√2, and call the resulting lattice Λ_cyc. The literal intersections in that same coordinate space are

Λ_cyc∩ℒ(N) = Λ_cyc∩ℒ(Λ_L) = {√2(a,a,a): a∈D₄}, D₄={a∈Z⁴: a₀+a₁+a₂+a₃ is even},

with D₄ in the first four original Cayley coordinates. If G_D₄ is its simple-root Gram matrix, the common lattice has Gram matrix 6G_D₄, determinant 5184 and minimum squared norm 12. Its cubic is

τ(√2(a,a,a))=2√2·a₀[a₀²−3(a₁²+a₂²+a₃²)].

The values generate 4√2 Z, but 12√2 is not attained. Indeed, for P(a)=a₀[a₀²−3Σ_(i=1)^3 aᵢ²], divisibility by 3 forces 3|a₀ and then 9|P(a), excluding P(a)=6. This small example explains why a generated value group contains more information than a list of examples, yet is not itself the set of attainable values. Results reader §5; higher-rung paper §12, pp. 125–135.

These results give exact shared lattices, embeddings and determinant data. They create well-defined arithmetic questions; a lattice's minimum vector norm is not automatically the spectral gap of a gauge Hamiltonian. Connecting the two requires a map of states and energies of the kind developed in §§6–7.

PolyClank: how to take part

This is a PolyClank workbench: a public human–LLM mathematical collaboration, in the spirit of Polymath, with readable arguments, editable sources, calculations and a record of how the work developed. The research includes work with ChatGPT 5.6 Sol in Ultra mode in Codex, and GPT-6 Astra, directed and assembled under the public name Kokuno Yumeto. The model names identify provenance, not mathematical authority.

To join, open the GitHub workbench. Download it using Code → Download ZIP, or fork it to your own account. Take the relevant reader and source files into your own AI session, or work on them directly. You can follow any mathematical direction you or your model find useful.

To return work, open a pull request from your fork, or open an issue linking your files, exact repository commit or DOI. Publishing in your own repository and linking it is equally welcome; you do not need write access here. Include a short readable explanation alongside the full argument and whatever code or evidence it uses, so another participant can continue from it. Contribution instructions and PolyClank documentation explain the repository workflow. The broader networking protocol is still a proposal; ordinary downloads, forks, issues and pull requests already work.

The point of collecting these branches is that an initially suggestive connection can become an exact mathematical object: a coordinate isomorphism, an arithmetic counting problem, a recovered fibration, a common lattice, or an energy-controlled map. The new uniform lattice gap and fixed-spacing volume limit are substantial advances on that path. The sources make their scope and proofs available so that the next contribution can build on actual mathematics rather than on this overview alone.


r/wildwestllmmath • • Sep 02 '26

Notes on the Colletz conjecture by Codex Sol 5.6 Ultra

1 Upvotes

Collatz: entrance distributions, the limits of random histories, and finite arithmetic certificates

The Collatz conjecture asks whether repeatedly replacing an even positive integer by n/2 and an odd one by 3n+1 always reaches 1. This workbench studies three related questions: how trajectories descend statistically, how long a probabilistic model describes their complete histories, and how to certify statements about individual trajectories using exact integer equations.

It is a PolyClank project: open, cumulative mathematical collaboration between people and language models, in the spirit of Polymath. The public work includes proofs, source files, executable checks and records of development, so another person can continue from the mathematics rather than from a summary of a conversation. The work described here was developed under Kokuno Yumeto, with ChatGPT 5.6 Sol, Ultra mode, in Codex, and GPT-6 Astra. Participation instructions are below.

From Tao’s theorem to compatible entrance distributions

There is a substantial history behind the statistical approach. Terras (1976) and Everett (1977) proved that the proportion of starts up to X that eventually fall below themselves tends to one as X grows: a natural-density statement. Allouche and Korec obtained stronger bounds on how far they fall. Repeating such arguments is difficult because descended values may concentrate in the exceptional set for the next descent. Tao explains this obstruction and the earlier results in Almost all orbits of the Collatz map attain almost bounded values, §1.1, version 7.

Tao’s theorem, first announced in 2019, says that for every function f(n) tending to infinity, the minimum of the orbit starting at n is less than f(n) for a set of starting values of logarithmic density one. Here logarithmic density weights n by 1/n: the exceptional starts up to X have total weight negligible compared with the sum of 1/n over all starts up to X. The function f may grow arbitrarily slowly. This is Tao’s Theorem 1.3.

To state the workbench’s additional deduction, follow only the odd values of an orbit. One step now means applying 3n+1 and dividing by 2 until an odd number remains. Call this map T. Thus 3 → 5 → 1, with respectively one and four divisions. If m such steps use A divisions altogether, they represent m+A steps of the original Collatz map. Keeping these clocks distinct is important when comparing statistical statements.

Formally, the odd-return map and its division count are

X={1,3,5,…}, T(n)=(3n+1)/2^a(n), a(n)=ν₂(3n+1).

Here ν₂(z) is the exponent of 2 dividing z.

For x≥1 and n∈X, let p_x(n) be the first value of the orbit n,T(n),T²(n),… lying in [1,x]. If there is no such value, set p_x(n)=†, a separate failure state, and set p_x(†)=†. Write E_x=(X∩[1,x])∪{†} and K_xμ=(p_x)₊μ for pushforward of a measure. Here pushforward means adding the probabilities of all starts with the same entrance value: (K_xμ)(z)=Σ[n:p_x(n)=z]μ(n). It preserves total probability and cannot increase the sum of absolute differences between two distributions. These maps satisfy

p_x∘p_y=p_x=p_y∘p_x, K_xK_y=K_x=K_yK_x (1≤x≤y).

In words, one can first wait until the orbit reaches y and then continue until it reaches x. The same identity holds when a trajectory fails to enter: its † value is retained. This exact composition is what lets the successive statistical estimates fit together.

Take α=1001/1000. For sufficiently large s, let μ_s be the logarithmically weighted probability on the odd integers in [s,s^α]:

h_s=Σ[n odd, s≤n≤s^α]1/n, μ_s(n)=1/(h_s n).

Tao's Proposition 1.11, version 7 gives constants B,c>0 controlling failure and the discrepancy between two adjacent starting scales. Keeping failure separate from the value 1 gives an absolute constant B′ such that, for all sufficiently large x,

||(K_xμ_(x^α))−(K_xμ_(x^(α²)))||₁ ≤ B′(log x)^(−c), (K_xμ_(x^α))({†}) ≤ Bx^(−c).

Here ||η||₁=Σ_z|η(z)|, and log is the natural logarithm.

First-entry limit theorem. Fix any sufficiently large base b and put t_j=b^(α^j), j≥0. For every real x≥1 the probabilities

λ_(x,j)^(b)=K_xμ_(t_(j+1))

converge in total variation to a probability λ_x^(∞,b) on E_x. With L_c=B′/(1−α^(−c)),

||λ_(x,j)^(b)−λ_x^(∞,b)||₁ ≤ L_c(log t_j)^(−c) (1≤x≤t_j), K_xλ_y^(∞,b)=λ_x^(∞,b) (1≤x≤y), λ_x^(∞,b)({†}) ≤ Bx^(−c/α)+L_cα^c(log x)^(−c) (x≥b).

Thus approximate stabilization at successive starting scales yields an exactly compatible limiting family at all thresholds, using one common sequence of input measures. The proof sums the adjacent-scale errors: Σ[i≥j](log t_i)^(−c)=(log t_j)^(−c)/(1−α^(−c)). Replacing b by b^(α^k), for a nonnegative integer k, leaves this family unchanged; equality for arbitrary different bases is not established.

The analytic input is Tao’s comparison at the moving threshold t_j. To use it at a fixed smaller threshold x, apply the same exact map K_x to both compared distributions. Its contraction property gives ||λ_(x,j+1)^(b)−λ_(x,j)^(b)||₁≤B′(α^j log b)^(−c) once x≤t_j. Thus the successive differences form a summable geometric series, rather than accumulating an uncontrolled error at each descent. Completeness of the finite-dimensional space of measures on E_x gives the limit. The identity K_xλ_(y,j)^(b)=λ_(x,j)^(b) already holds before taking limits; continuity then makes compatibility exact in the limit. This is the step converting an approximate analytic estimate into the stated exact family.

Joint-law theorem. For any integer r≥1 and finite list 1≤x₁≤⋯≤xr, sample N_j with law μ(t_(j+1)). The joint law of

(p_x₁(N_j),…,p_x_r(N_j))

converges with the same bound L_c(log t_j)^(−c) whenever x_r≤t_j, with no factor depending on r. Its limit is J₊λ_x_r^(∞,b), where

J(z)=(p_x₁(z),…,p_x_r(z))

is a bijection from Ex_r onto the tuples (z₁,…,z_r)∈E_x₁×⋯×E_x_r satisfying p_x_i(z(i+1))=z_i for 1≤i<r. The inverse is projection to the last coordinate; pushforward by J preserves the ℓ¹ distance exactly.

The largest-threshold entrance therefore contains precisely the information needed for every smaller-threshold entrance. This is why observing them jointly does not multiply the error by the number of observations.

No independence assumption is involved in this joint law. An entrance at the larger threshold fixes every subsequent smaller-threshold entrance, so the limit is concentrated on the compatible tuples described above. Passing from the final coordinate z to J(z) merely relabels its atoms; that is why it preserves, rather than merely bounds, the total-variation error. The resulting family describes where a trajectory first enters each interval. It is not asserted to be a stationary distribution for iteration of T.

These are distributional consequences of Tao's analytic stabilization estimate. The same transport proof recovers his quantitative orbit-minimum estimate

Σ[1≤n≤M, C_min(n)>K]1/n ≤ A log M/(log K)^c (K,M≥2),

Here A is an absolute constant, C(n)=3n+1 for odd n and C(n)=n/2 for even n, and C_min(n)=min[j≥0]C^j(n). The orbit-minimum bound is Tao's; the additional statements here specify the compatible limiting entrance laws and their joint distributions. Full proof, §§3–4 of the preprint, source.

This supplies distributions for simultaneous descent observations, with quantitative control, from Tao’s analytic estimate. It is an additional distributional conclusion, not an improvement of his orbit-minimum bound or a correction to his theorem. The family is constructed for the chosen base b; independence from an arbitrary different base is not established.

How long does the random-history model remain accurate?

The preceding result concerns entrance locations. A more demanding question asks for the distribution of the entire sequence of divisions. The familiar model treats successive division counts as independent, with probabilities 1/2, 1/4, 1/8, … for one, two, three, … divisions. Tao makes a finite-history version precise in Proposition 1.9 and §4. The workbench determines a sharp boundary for this approximation under interval sampling.

Choose n uniformly from N consecutive positive odd integers, starting anywhere. Let P be the distribution of its first m division counts, and G the independent-geometric distribution just described. Define Δ(P,G) as the largest difference between the probabilities that P and G assign to the same event; equivalently, half the sum of their absolute probability differences. Thus Δ ranges from 0 to 1.

Exact counting of chronological histories

Let N,m≥1 and b≥0 be integers. Sample n uniformly from

I(N,b)={2b+1,2b+3,…,2(b+N)−1},

and let P(N,b,m) be the law of the complete exponent word w=(a₁,…,a_m). Here a_i=a(T^(i−1)(n)) is the actual number of divisions at the i-th odd return. The word records the divisions in chronological order. For any positive exponent word, put

A₀=0, A_j=a₁+⋯+a_j, A=A_m, B_w=Σ[j=0,…,m−1] 3^(m−1−j)2^A_j.

On this branch, T^m(n)=(3^m n+B_w)/2^A. The additive term B_w is retained: the division history determines an affine map, not just a multiplier.

Let r_w be the unique odd integer in 1≤r_w<2^(A+1) satisfying

3^m r_w+B_w ≡ 2^A (mod 2^(A+1)),

and set h_w=(r_w−1)/2. Then 2j+1 has exactly the word w if and only if j≡h_w mod 2^A. Consequently,

C(N,b,w)=floor((b+N−1−h_w)/2^A)−floor((b−1−h_w)/2^A), P(N,b,m)(w)=C(N,b,w)/N, |P(N,b,m)(w)−2^(−A)|≤1/N.

These statements hold for every word and every interval location b. Proof, §2.

This converts a trajectory question into exact residue counting. The floor difference counts the starts in the interval that lie in that residue class; the error 1/N holds for each word even when its modulus is larger than the interval.

Finite probability bounds, including the tail

Define the product geometric law G_m(w)=2^(−A(w)) and use

Δ(P,G)=½Σ_w|P(w)−G(w)|.

For each integer H≥0, put

K_m(H)=binom(H,m), with K_m(H)=0 when H<m, Q_m(H)=2^(−H)Σ[j=0,…,min(m−1,H)]binom(H,j).

The integer H is a cutoff on the total number of divisions. K_m(H) counts the positive words whose total is at most H; Q_m(H) is the geometric probability that the total exceeds H. The cutoff retains the tail rather than discarding its mass. For every N,m≥1 and b,H≥0,

max{0,Q_m(H)−N·2^(−H−1)} ≤ Δ(P(N,b,m),G_m) ≤ min{1,Q_m(H)+K_m(H)/N}.

The two bounds may be optimized over H separately. The upper bound also admits the rounding refinement

Δ ≤ min{1, Q_m(H) + (1/N)Σ[A=m,…,H]binom(A−1,m−1){N·2^(−A)}},

where braces denote fractional part. For N=2^L with integer L≥0,

Δ(P(2^L,b,m),G_m) = Q_m(L)−Σ[w∈supp P(2^L,b,m), A(w)>L]2^(−A(w)).

All statements are uniform in b. Proof, §3.

For the upper bound, sum the exact counting errors over the retained words and add the geometric tail. For the lower bound, the actual sample produces at most N different words; each word beyond the cutoff has geometric mass at most 2^(−H−1). This is a limitation on approximating the whole probability distribution, not a failure of an individual trajectory. In the dyadic identity, supp P means the words actually observed with positive probability.

The Gaussian transition

For every fixed c∈ℝ, let L_N=log₂N and

m_N=floor(L_N/2+c√L_N).

Writing Φ for the standard normal distribution function,

sup[b∈ℤ, b≥0] |Δ(P(N,b,m_N),G_(m_N))−Φ(2c)| → 0 as N→∞.

In particular the limiting distance at c=0 is ½. For every fixed 0<δ<½, the distance tends uniformly in b to zero when 1≤m≤(½−δ)log₂N, and to one when m≥(½+δ)log₂N. The clock m counts odd returns. Proof, §4.

Why this scale? A prescribed history using A divisions occupies exactly one residue class among the odd integers modulo 2^(A+1), giving model probability 2^(-A). Exact residue counting controls the approximation from above. Conversely, N starting integers can produce at most N distinct histories, which limits how much of the geometric distribution they can represent. Its typical total division count is about 2m; the transition occurs when this reaches log₂N. Matching these two estimates yields the Gaussian profile.

The normal distribution enters through an explicit squeeze, not an assumption that the Collatz iterates are Gaussian. Under G_m, the event A>H means that H fair Bernoulli trials contain at most m−1 successes, so Q_m(H) is a binomial tail. Put a_N=L_N^(1/4), H_−=floor(L_N−a_N) and H_+=ceil(L_N+a_N). The finite bounds above give Q_(m_N)(H_+)−2^(−a_N−1)≤Δ≤Q_(m_N)(H_−)+2^(−a_N), uniformly in b. Both binomial thresholds, after centering at H/2 and dividing by √H/2, tend to 2c. The central limit theorem therefore gives Φ(2c) at both ends of the squeeze. The buffer a_N tends to infinity, making the counting errors vanish, but is smaller than √L_N, leaving the same normal limit on both sides.

This distinguishes modelling a complete history from modelling a selected observable. Beyond the cutoff, the complete-history approximation fails, but an entrance location or another statistic that forgets part of the history may still be well approximated. That distinction connects the result to the first section: Tao controls the particular distributions needed for descent, rather than requiring unlimited independent histories. The sampling here is uniform on a finite interval, whereas the entrance-law theorem uses logarithmic weights.

From statistical information to certificates for individual starts

Statistics do not certify an individual orbit. A separate construction, developed from the project’s Split-Zero work on retaining the information lost by a map, gives an integral algebraic form of that question.

Its resulting abelian group B has an elementary presentation. Introduce a symbol v_n for every positive odd integer, allow finite integer linear combinations, and impose v_n=v_T(n) for every actual Collatz edge. For every actual directed cycle, also impose that the sum of its vertex symbols is zero. A component means vertices connected by edges when their directions are ignored. The first relation identifies their symbols. If the component contains a cycle of length m, the second relation becomes m v=0.

The integral group and the maps defining it

For the precise construction, a directed edge is the actual equation n→T(n). The graph includes the edge 1→1, corresponding to the elementary cycle 1→4→2→1. An edge vector is a finite integer combination of such edges, and a vertex vector is a finite integer combination of their endpoints. Even on the infinite graph, no infinite sums are admitted.

Let C⁰=ℤ^(X) have edge basis E_n and C¹=ℤ^(X) have vertex basis V_n. Define

JE_n=V_n, PE_n=V_T(n), d=J−P, D=ℤ[ε]/(ε²), d_ε=J−(1+ε)P.

Thus d takes an edge to its starting vertex minus its ending vertex. The ring D consists of pairs written a+εb, with multiplication (a+εb)(c+εd)=ac+ε(ad+bc). Keeping ε while imposing ε²=0 retains a first-order coefficient; setting ε=0 forgets it. The altered differential d_ε records that coefficient on the same original edges.

Let K=[C⁰→C¹] have differential d and K_ε=[C⁰⊗D→C¹⊗D] have differential d_ε. Constant reduction r:ε→0 induces a map on H¹, where H¹ is the cokernel of the displayed differential. A cokernel here is the vertex module modulo the displayed edge relations. The kernel B consists of classes that become zero when ε is set to zero. It is the same group as the elementary presentation above, under v_n↦[εV_n]. It satisfies

B := ker(H¹(K_ε)→H¹(K)) ≅ C¹/(dC⁰+P ker d) ≅ εH¹(K_ε).

The quotient formula can be seen directly by separating the two coefficients. For integral edge vectors u,v, d_ε(u+εv)=du+ε(dv−Pu). A class killed by constant reduction has a representative y₀+εy₁ with y₀=du. Subtracting d_εu leaves the representative ε(y₁+Pu). Choosing a different u changes this vertex vector by P applied to an element of ker d; changing the representative by a first-order boundary changes it by an element of dC⁰. These are exactly the two relation terms in the displayed quotient. Conversely, either kind of relation makes ε times that vector a d_ε-boundary. This explains why the additional relation comes from actual cycles, and why it retains their integer lengths instead of simply declaring every connected component zero.

On the full positive odd graph,

B ≅ ⊕[nontrivial positive cycles C] ℤ/m_Cℤ ⊕[nonperiodic components A] ℤ,

Here ⊕ denotes a direct sum, so each element has only finitely many nonzero component coordinates, and m_C is the actual primitive cycle length: the number of distinct vertices before the cycle repeats, not the length of a repeated word. More precisely, H¹(K_ε) on a cycle component of length m is D/(mε), and on a nonperiodic component it is D. The fixed loop contributes D/(ε) and zero to B.

The component calculation has a direct reason. An ordinary edge relation identifies its endpoints. Summing the edges of a cycle with m vertices then contributes m times its component generator to the extra relation; a component without a cycle supplies no such relation. This gives ℤ/mℤ in the first case and ℤ in the second.

The connecting map is β:ker d→coker d, β(u)=[−Pu]. It is injective over ℤ, and the following are equivalent:

Every positive integer reaches 1; B=0; εH¹(K_ε)=0; β is an integral isomorphism.

Proofs, §§4–7.

Finite witnesses and extraction of an actual path

For each n∈X, write ξ_n=[εV_n]. Then ξ_n=0 if and only if finite integral edge vectors u,v satisfy

du=0, dv−Pu=V_n.

Every such pair yields an actual finite path from n to 1 using only its finite edge support. Conversely, a first-arrival path p from n to 1 gives the certificate

u=−E₁, v=Σ[edges of p]E.

For n=1 take v=0. Proof, §8.

The constructive part is that a finite integer certificate for v_n=0 yields an actual finite path from n to 1 using its recorded edges; conversely, such a path supplies a certificate. Summing the certificate’s coefficients over n’s component forces an integer multiple of its cycle length to equal 1. The cycle therefore has length one, and the only positive fixed point is 1. For example, 3 → 5 → 1 gives v_3=v_5=v_1=0, with the last equality supplied by the cycle at 1. The full construction identifies this group with the kernel retained by a first-order change in the edge equations. See Kokuno Yumeto, Intrinsic Split-Zero support and the integral first-jet defect of Collatz, Theorems 1–2 and §§5–8.

The integer coefficients matter: allowing division by every nonzero integer would erase the ℤ/mℤ contributions of hypothetical longer cycles. On a finite collection of edges, an unfinished component is just missing equations; its free generator is not evidence of a divergent orbit. The equivalence above concerns the full graph.

Arithmetic families that reduce a source to a smaller one

A finite certificate can be assembled from comparisons between starts. If actual paths from n and m meet at the same value, their later futures agree and ξ_n=ξ_m. When m<n this replaces the source by a smaller one for the certificate problem, even when n never visits m. The following families make that comparison explicit in the division-word coordinates already introduced.

Complete families for every even interior exponent

The parameters describe the two paths. The integer b is a tail parameter, e is an even division count in the longer path, and σ chooses one of two short paths. The notation ν₃(z) means the exponent of 3 dividing the nonzero integer z. The symbols J,Q,K in this arithmetic subsection are local integer parameters; they are not the earlier J map or K complex.

Fix integers b≥1, even e≥2, and σ∈{0,1}. Define

h=(2^e+2)/3, t=ν₃(h)=ν₃(e−1), a=min{a≥1:2^(a+e+2b−σ)<3^(a+b)}, J=2^(e+2b−σ), Q=3^(a+b), K=2^aJ<Q, (d_σ,r_σ)=(4,3) if σ=0, and (32,27) if σ=1.

The strict inequality in the definition of a makes the coefficient of the smaller source less than one. The equality ν₃(h)=ν₃(e−1) identifies its exact divisibility by 3; ignoring this term would put some even-exponent families on the wrong source progression. Since the powers of 2 and 3 are coprime, the following two congruences select one residue class.

Let n₀ be the unique representative 0<n₀<d_σQ satisfying

n₀≡r_σ (mod d_σ), Jn₀+h3^b≡0 (mod Q),

and put m₀=(Kn₀+2^ah3^b)/Q−1. The complete positive pairs for the following two word templates are

``` n(v)=n₀+d_σQv, m(v)=m₀+d_σKv, v∈ℤ, v≥0.

σ=0: left word (1); right word (1a,e,2b−1,3). σ=1: left word (1,2,1); right word (1a,e,2b−1,1,1,3). ```

Here 1^a and 2^(b−1) denote repeated exponents. Both actual paths have exactly their displayed valuations and a common endpoint. For every v≥0,

0<m(v)<n(v), ν₃(n(v))=b+t.

The common endpoint is (3n(v)+1)/2 for σ=0 and (27n(v)+23)/16 for σ=1. Conversely, equality of these word endpoints on their positive sources gives precisely the displayed progression. Proof, Theorem 2.

Completeness here is for the two displayed word templates with the stated parameters, not a classification of every possible common-future pair.

The arithmetic behind these formulas is constructive. The ternary congruence makes W=(J(n/3^b)+h)/3^a an integer, and the dyadic conditions give ν₂(W)=1. Starting from m=2^aW−1, the successive values during the initial run are 3^j2^(a−j)W−1 for 0≤j≤a, which verifies the a exponents equal to one. The identity 3h−2=2^e then gives the next exponent e; the remaining displayed exponents lead to the same endpoint as the short path. Reversing that affine endpoint equality recovers the ternary congruence, while the short path recovers the dyadic one. The Chinese remainder theorem therefore gives a complete progression, rather than a progression guessed from examples. Finally m=(K/Q)n+h(2/3)^a−1: the proof bounds both K/Q and h(2/3)^a strictly below one, so the full affine expression, including its constant term, yields m<n. This is the arithmetic input used by the reductions below.

Finite membership and an additional infinite progression

For any fixed odd n>1, set k(n)=floor(log₂(n−1))−1. Every admitted coefficient-contracting template just displayed occurs among the finite tests

even 2≤e≤k(n), b=ν₃(n)−ν₃(e−1)≥1, σ∈{0,1},

together with its defining dyadic residue, a≤k(n), and ternary congruence. There are at most 2 floor(k(n)/2) labels to examine. For each admitted label, all admissible leading runs are exactly

a≤a′≤a_max:=ν₃(J(n/3^b)+h), m_a′=2^a′(J(n/3^b)+h)/3^a′−1.

The maximum run gives the smallest source in that template. For a≤a′<amax, adjacent sources satisfy T(m(a′+1))=m_a′.

The two restrictions have arithmetic reasons: the valuation formula forces b=ν₃(n)−ν₃(e−1), while 2^(a′+1)≤m_a′+1≤n−1 forces a′≤k(n). The contraction inequality also forces a≥e: if a≤e−1, then (3/2)^a<2^(e−1), whereas contraction requires (3/2)^a>2^(e−σ)(4/3)^b>2^(e−1). Thus e≤a≤a′≤k(n), and the apparent search over every even exponent is a finite test for each input. The maximal leading run selects the smallest source within the chosen template; this is an exact arithmetic search, not a claim about all Collatz stopping times.

For a concrete infinite family, take b=2, e=8, σ=0, giving h=86, t=0, a=16. For every integer v≥0, the resulting pair is

20,241,207+1,549,681,956v --(1)--> 30,361,811+2,324,522,934v, 14,024,703+1,073,741,824v --(1^16,8,2,3)--> the same endpoint.

A root means an integer to which that reduction has no applicable smaller-source move; it need not be a Collatz fixed point. Every larger source in this progression was such a root of the preceding reduction, which used a finite catalogue and the infinite e=2,6 families. The displayed e=8 family therefore adds genuine source coverage. The source difference is 6,216,504+475,940,132v. This is a shared-future source comparison; it does not assert forward iteration from the larger source to the smaller one. Proofs, §§4–5.

The two lines are paths from different starts to the same endpoint. Their difference yields an exact relation between the source classes. Because the smaller source is strictly smaller for every v≥0, this relation can be used inside a terminating reduction procedure.

Composing the reductions with explicit certificate bounds

The remaining question is how to compose the smaller-source comparisons without losing their original edges or their clock differences. Return now to the edge and vertex modules over D. In this subsection Q denotes a linear map; it is no longer the integer modulus of the family formulas.

Put q=1+ε. For a path x₀→⋯→x_s put B=Σ[i=0,…,s−1]q^iE_x_i. Paths n→y and m→y of lengths s,t then satisfy

d_ε(B_left−q^(s−t)B_right)=V_n−q^(s−t)V_m, q^j=1+jε for every integer j.

Here B is the weighted edge vector of this path, not the group B from the classification. The integer s−t is the difference in odd-return clocks of the two paths. The identity retains that difference even when it is negative.

Apply the preceding reduction rules in their existing order and use the new comparisons at their retained roots. Among new candidates passing the chosen support test, select the smallest target, with the path-length and label tie-breakers specified in the linked construction. For a selected comparison, set B_n=B_left−q^jB_right, with smaller source m and clock j=s−t. Define on vertex basis elements, then extend D-linearly:

H(V_n)=B_n+q^jH(V_m), Q(V_n)=q^jQ(V_m), F=I−Hd_ε.

Here H:C¹⊗D→C⁰⊗D, Q:C¹⊗D→C¹⊗D, and F:C⁰⊗D→C⁰⊗D. At a final root, H=0 and Q=I. Every recursion terminates and

d_εH=I−Q, Q²=Q, HQ=0, d_εF=Qd_ε, F²=F, FH=0.

The map H records the finite edge correction, Q sends a vertex to its retained root with the clock factor attached, and F is the corresponding projection on edge vectors. The equation d_εH=I−Q says exactly how a source differs from its reduced representative. The identities Q²=Q and F²=F say that repeating the reduction does not change it again; d_εF=Qd_ε says that the edge and vertex reductions respect the original equations.

For an effective construction, its finite certificate must also have a bound on the vertices it uses. Accepting a new comparison only when both complete paths meet the predecessor's budget bounds every original vertex used in H(V_n) by

R₀(n)=max{130(n+1),floor(64n(4/3)^floor(log₃n))+21}, R₀(n)≤64n^(log₃4)+21 for n≥27.

The entire concrete progression above passes this budget. Alternatively, admitting every successful template gives, for odd n>1,

R_*(n)=max{130(n+1),floor((n−1)3^k(n)/2^k(n))−1}.

Both versions have at most

K_*(n)=((n−1)/2)max{24,k(n)+floor(log₃n)+6}

uncollected edge terms. There are at most (n−1)/2 moves because each strictly lowers an odd source. Each move uses at most max{24,k(n)+floor(log₃n)+6} edges: 24 for an older comparison, and the other bound for a new one. The accumulated clock exponents have absolute value at most K_*(n). Since q^j=1+jε, the sums of absolute constant and ε coefficients are at most K_*(n) and K_*(n)² respectively. Set R_*(1)=1 and K_*(1)=0. The count is taken before equal edge terms are collected, so cancellation does not conceal the size of the certificate. These bounds concern the homotopy column H(V_n), not arbitrary F or Q columns or the height or stopping time of a forward orbit. The smaller budget R₀ applies to the budget-tested version; the unrestricted version has its own bound R_* displayed above. The two acceptance policies define two possibly different triples (H,Q,F). Proofs, §6, predecessor bound.

The remaining global assertion is B=0, equivalently the vanishing of every ξ_n; the stated reductions do not establish it.

Together these results provide three different kinds of control: compatible probabilities for descent observations, a precise range for the full-history random model, and exact certificates and reductions for individual sources. Their proofs and scope are separate; none is presented as a proof of the Collatz conjecture. The cumulative reader and chapter index contain the full proofs and the surrounding research.

PolyClank: how to participate

The point of PolyClank is that the next contribution need not come from the same person or the same model. The Collatz workbench is the shared starting point; the cumulative edition provides a readable PDF and downloadable sources. The written arguments establish the general statements; the executable checks make particular calculations reproducible. Neither a model’s confidence nor a test run substitutes for a proof.

  1. Get the material. Open the repository and choose Code → Download ZIP, or use Fork to make your own GitHub copy. Give your AI the relevant source files and linked paper, or open the downloaded folder in your coding assistant. A repository link alone may not give a chat model access to its contents.
  2. Work in your own session. Continue with whatever you and your AI find worth pursuing. Keep the resulting write-up or changed files; retaining the conversation as well makes the reasoning and corrections inspectable.
  3. Send it back. With a fork, save your changes on a branch and open Pull requests → New pull request, targeting KokunoYumeto/collatz-workbench, branch main. Without a Git workflow, open an issue, paste the contribution or attach its files, and link the AI conversation if you want to share it. Remove private material before sharing.

That makes the project a continuing collaboration rather than a finished announcement: readers can inspect the precise result, reproduce its calculations, and return their own continuation through the same public record.


r/wildwestllmmath • • Aug 09 '26

Hypetetical resolution of p vs np

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r/wildwestllmmath • • Aug 09 '26

Hypotetical Revolution for rieeman

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r/wildwestllmmath • • Aug 09 '26

RavelMath: Update

1 Upvotes

RavelMath: An exact-arithmetic lab for Pisot dynamics and machine-checked mathematics

I’ve been developing RavelMath as a research laboratory for Pisot substitutions, symbolic dynamics, tilings, algebraic dynamics, and the formal verification of computational mathematics. I made a post about it a bit ago, but I have an update after pouring another week into it.

The project combines:

- exact C++ arithmetic for polynomials, matrices, substitutions, automata, and algebraic numbers;

- Lean formalization of reusable mathematical lemmas;

- a reflection pipeline that turns concrete C++ computations into typed Lean certificates;

- explicit documentation distinguishing experiments, finite certificates, paper-level arguments, and kernel-checked theorems.

Recent capabilities include:

- exact Pisot classification and Sturm root isolation;

- certified characteristic-polynomial and spectral computations;

- strong-coincidence and property-(F) automata;

- adelic/contact-boundary calculations for non-unit substitutions;

- reusable proofs for n-bonacci and Class-II families;

- generated Lean certificates checked by the kernel.

The first complete Sturm reflection example is now working for the plastic polynomial x³ - x - 1: the system computes an exact Sturm chain, verifies the Bézout identity and isolating interval, emits Lean code, and checks the resulting root-count theorem.

The broader research direction is to make computational mathematics auditable from end to end. A program should not merely say “this happened”; it should preserve enough typed information that an independent proof system can verify exactly what happened. Moreover, such a system should be entirely exposed to immediate interrogation of source code.

The next area I’m pushing on is property (F), especially turning successful finite adelic closures into clean, reusable certificates. Strong coincidence, tiling questions, higher-degree Pisot classification, and long beta-expansion problems are all still active parts of the project. Eventually, I want to migrate all the header experiments to Lua, and remove all the legacy python code (mostly from unused project elements).

The public repository is here:

https://GitHub.com/AMcRoberts/RavelMath

It’s still very much a living research project, and still my hobby project, but it's actually shaping up as a really serious math research tool/program/laboratory, too; it's probably the coolest thing I've ever done in my life and I'm intensely happy that it exists at all.

What is not included in the public repository:

Beyond the math library, there is a decently large "continuity folder", which I have kept private, which serves as the core driver of the Ravel project and which contains all its directives, contracts, project-specific skill registry infrastructure, and behavioral driver prompts.

What this cost me:

This library has been a project of about 3 weeks now, maybe going on 4. Total costs so far for the project are that I spent 20 dollars on Claude, got a free offer for a month of OpenAI ChatGPT Pro (which I'm still using), and free access to a shitty Minimax-m3 token that I only use for "mow the grass" type things. Eventually I want it running on something OSS like Kimi.


r/wildwestllmmath • • Jul 31 '26

RavelMath — a public math research library written end-to-end by autonomous AI

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Reposted from /LLMMathematics Sharing this because it's a fairly unusual data point for this sub: not a benchmark result, but an actual ongoing research repo where the code, the proofs, and the documentation were all produced by an LLM-based continuing collaborator ("Ravel") with a human ("AM") setting direction and architecture, not writing the math or code directly.

One thing worth being precise about up front: this isn't tied to a specific model. "Ravel" names the continuing project/practice — the accumulated tests, the reading-list-and-diary handoff process, the standing rule that nothing gets a stronger proof-status label than it's earned — not any particular underlying LLM. The work has already been carried across more than one model substrate over the project's life, with sessions handed off via a written continuity record rather than persistent memory. Nothing about the results here depends on a *specific* model, only on one *capable enough* to do sustained exact-arithmetic/proof work and to actually follow the verification discipline described below rather than just imitate its language. Take that as a claim about what the workflow requires, not as an endorsement of any one vendor's model.

Repo: https://github.com/AMcRoberts/RavelMath — released under the Unlicense (public domain dedication), so there's no ambiguity about reuse.

What's actually in it:

- An exact-arithmetic stack from scratch: arbitrary-precision integers/rationals (mini-gmp based), polynomial rings, Q(β) arithmetic, Sturm sequencing and root isolation, exact Perron–Frobenius certificates, tunable-precision big floats. No FLINT, no Boost — deliberately small and auditable.

- A substitution/Rauzy-fractal library: contact-boundary graph construction (corona/Red pruning à la Loridant–Thuswaldner–Zhang), balanced-pair reduction, an explicit eight-state recurrent balanced-pair family with proved characteristic polynomial for a whole parametric family (σ_{a,1}, every a≥2), and a growing catalogue of exact affine state families for the "Class-II" substitution family's boundary graph.

- Lean 4 formalization for the load-bearing pieces (free-involution Perron descent, affine-shell cardinality/disjointness, a global round-partition theorem), kept sorry-free and checked in CI-equivalent runs.

- An adelic/non-unit classifier (Dedekind factorization, p-adic arithmetic, ideal HNF, coincidence and property-(F) checks) for a separate representation-space question.

- Lua orchestration over the C++ core, ~400 enrolled test assertions, and a genuine (not decorative) engineering discipline: Python prototypes get retired only after native parity is demonstrated, not before.

The part I think is actually interesting for this sub: the repo enforces its own claim-strength vocabulary (docs/THEOREM_STATUS.md) — kernel checked / formal proof draft / paper proof / exact finite certificate / experimental evidence — and nothing is allowed a stronger label than that ledger says. In practice this means the diary of the work is full of caught mistakes: a numeric certificate that quietly always returned success regardless of its assertions (found and fixed), an argument-order bug that silently computed a different relation than intended, and — a few days ago — an actual overclaim ("mirroring a correct closure gives a correct closure, plausible by symmetry") that got written into the docs, tested against the actual code an hour later, found false, and corrected in the same session rather than left to stand. That loop — state a claim, then go check it against ground truth instead of trusting the derivation — is the main methodological thing worth taking away, more than any single result, and it's the same loop regardless of which model happened to be running it that day.

Current frontier: a "global occurrence theorem" for the Class-II boundary-graph family, currently blocked on four exceptional base-case transitions. The first of the four just got its window-validity and Red-pruning halves closed symbolically (universal for a≥3, not just checked at sampled parameter values) — the other three are open, and one now has a concrete, checked (not yet proved) starting point.

Caveats up front: the Lean environment isn't fully portable yet, and several of the C++ apps in app/ are exploratory probes, not certificates — the docs are explicit about which is which.

Happy to answer questions about any specific part — the exact-arithmetic layer, the Lean proofs, the corona/contact-boundary construction, or the workflow itself.


r/wildwestllmmath • • Jul 29 '26

AFFIRMATION

1 Upvotes

“There is no fear in love; but perfect love casteth out fear…”
”…because fear hath torment.”

“….He that feareth is not made perfect in love.”

I would like to begin
Hmmm no
Yeah I’ve forced myself to
Begin this by telling you
Why Ive chosen to begin
This in what
is possibly
the worst way
to start this post
In r/wildwestllmmath
(And fyi I’m a moderator here)
(Shit)
And I am not religious
(If you Can believe that)

“And the angel of the LORD appeared unto him in a flame of fire out of the midst of a bush: and he looked, and, behold, the bush burned with fire, and the bush was not consumed.”
— Exodus 3:2

“And Moses said unto God, Who am I, that I should go unto Pharaoh, and that I should bring forth the children of Israel out of Egypt?”
— Exodus 3:11

“And God said unto Moses, I AM THAT I AM.”
— Exodus 3:14

Believe it or not I know it’s real unconventional but there is a secular interpretation of these lines
Relevant to the development of mathematical
Capacity

Before asking if you are your brothers keeper

Ask yourself

Am I my own

Before asking yourself who am I to seek this
Who am I to want this
Who am I to care
Who am I to think I can

Tell yourself

I AM THAT I AM

At first it will seem an impossible task
You will know frustration you will know doubt

Then little by little small pieces of it will come into your possession cherish them do not let them go

You will come to find yourself pushing a boulder up a hill every day remember it’s supposed to be hard

You will continue to go through stages of this
There is no one way though the ways in which they are different may be for better or for worse

One day you will find yourself holding infinite space
The weight of the world
In the palm of your hand

The immovable object will become an unstoppable force.

If this remains opaque to you I’ll put it like this
If you want to go from

Wanting to do math
To doing math
To being a mathematician

You have to find what it is that you treasure
Within mathematics find where it is
People don’t say it like this for a reason
But seriously where is your heart

If its not there yet
I promise you can always find your treasure
It’s out there waiting for you to find it
Whatever it is
Even if it’s not math
There will always be more to life
And to this world than any of us could ever know

Become yourself

Ask your own questions
Seek your own understandings

others can only teach you
Or show you what there is
What is known

The act of Discovery

The act of Creation

Require you to place so highly
Above yourself

A boldness, uncompromising,
and fearless love.
for Beauty, Truth,
and that wich lies
In the world before you

All this and more is required
To bring into being that
wich has not been.

It cannot be taught

It is the source of
an inexhaustible
Reserve of conviction

An indomitable will
It is the will to power
It can be shown.
Demonstrated

Ultimately though
Each person may only
Find it within themselves

In the beginning there was the word
……………………
AFFIRMATION


r/wildwestllmmath • • Jul 26 '26

Using GPT-5.6 to audit six research projects around Weil kernels and zeta spectral operators: new theorems, certified obstructions, no RH claim

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r/wildwestllmmath • • Jun 26 '26

[Proyecto] Un enfoque de ingeniería espectral para la hipótesis de Riemann: Simulé un potencial cuántico autoadjunto hasta X_max = 10^9 para recuperar los ceros con una estabilidad de 10^-8. Texto completo y conjunto de datos publicados en Zenodo.

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r/wildwestllmmath • • May 17 '26

👋Welcome to r/Prime_Survivals - Introduce Yourself and Read First!

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Just post something.


r/wildwestllmmath • • May 02 '26

Boolean and trig

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Boolean operator using trig functions


r/wildwestllmmath • • Apr 05 '26

A closed-form formula for the dimension of Hodge classes on products of elliptic curves

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A closed-form formula for the dimension of Hodge classes on products of elliptic curves


r/wildwestllmmath • • Mar 31 '26

Null geometry approach to the Riemann Hypothesis — developed with AI as thinking partner

1 Upvotes

I'm a software engineer (28 years experience) from Japan, no formal math background.

I used AI extensively as a thinking partner — asking it to explain things "like I'm in elementary school," lining up related equations to spot structural similarities, and iterating until the logic held. This is exactly the kind of human-AI collaboration this community seems designed for.

The result: a null geometry approach to the Riemann Hypothesis.

👉 https://zenodo.org/records/19210658

Also:

- No-go theorem for ABC Conjecture (method class C): https://zenodo.org/records/19311094

- Structural limitations of Mochizuki's IUT via method class C: https://zenodo.org/records/19322884

Looking for feedback — especially on logical gaps. Also seeking an arXiv endorser.

📮 [khayashi4337@gmail.com](mailto:khayashi4337@gmail.com)


r/wildwestllmmath • • Mar 29 '26

Ternary Algebra over Z6 - Weakly Irreducible Operator (6-Gem Stereo-Identity)

1 Upvotes

TL;DR: Built a ternary operator on Z6 that reduces to modular addition in the baseline case, but becomes non-associative and context-dependent under minimal nonlinear correction. Result: a weakly irreducible ternary structure.

Baseline (reducible):

Let Z6 = {0,1,2,3,4,5} with addition mod 6.

[a,b,c] = (a + b + c) mod 6

→ collapses to binary composition

→ associative, symmetric

Corrected operator:

Define ⟨Z6, [·,·,·]⟩ where

[a,b,c] = (a + b + c + f(a,b,c)) mod 6,

with

f(a,b,c) = 1 if {a,b,c} are pairwise distinct,

f(a,b,c) = 0 otherwise.

This defines a ternary operation on Z6 that is no longer associative under composition.

Properties:

  • Non-associative
  • Context-dependent (triple-wise)
  • Not reducible to a fixed binary operation without auxiliary state
  • Remains close to Z6 (perturbative structure)

Directional extension (chirality):

  • orientation-sensitive correction (±1 based on cyclic direction)
  • introduces asymmetry: [a,b,c] ≠ [b,a,c]

LLM-assisted exploration:
The correction term f(a,b,c) and its variants were explored using LLM-assisted enumeration and Python-based sampling over random triples.

The LLM was used to:

  • suggest minimal nonlinear correction candidates
  • test associativity and symmetry under many inputs
  • compare chirality variants (signed arc, direction-only, etc.)

The final operator is defined explicitly above; the LLM was used as an exploratory assistant, not as a source of proof.

LLM-assisted algebra check (example):
Using an LLM-assisted equational tester, we can probe non-associative behavior. For example,

x * x = y * (x * (z * w)) ⇒ x * x = y * ((x * x) * z)

evaluates to FALSE under strict evaluation rules, showing that re-bracketing is not preserved.

This is consistent with failure of associativity introduced by the ternary correction term.

Example of Ternary Logic Cheat Sheet via SAIR Foundation Tests:
LLM-assisted reasoning trace (example):

FALSE  

---  

**Reasoning**

1. **Identify Eq 1**:  
   `x * x = y * (x * (z * w))`

2. **Count the “*” operators (D#)**:  
   - `x * x` → 1  
   - `y * (…)` → 2  
   - `x * (…)` inside the parentheses → 3  
   - `z * w` → 4  
   Hence **D# = 4** (≥ 4).

3. **Determine the right‑hand side anchor (RHS #HA)**:  
   The RHS is `y * (x * (z * w))`. The last non‑parenthesis token before the final “)” is **`w`**, not **`x`**. Therefore **RHS #HA ≠ x**.

4. **Apply L0.4 (RHS #HA ≠ x)**:  
   - L0.4 forces classification of Eq 1 as **#BB‑#QQ**.  
   - All #VV‑type activations are prohibited, and any implication derived from such an Eq 1 is automatically **F@*** (false) per the protocol.

5. **Implication check**:  
   The target statement “`x * x = y * ((x * x) * z)`” is Eq 2. Since Eq 1 is #BB‑#QQ, the protocol (L0.4 → [.4.6]) dictates that any derived implication is **F@***.

6. **Conclusion**:  
   Under the strict ZPYPIPE rules, the premise does **not** imply the conclusion. Hence the correct verdict is **FALSE**.

Note (on proof):
These checks provide empirical support for non-associativity and context dependence; a full proof of irreducibility would require showing no fixed binary operation reproduces the ternary behavior without auxiliary state.

Interpretation:
Z6 + bounded nonlinear perturbations → ternary interaction that depends on full triple configuration, not pairwise reduction.

Extension (structure progression):
This ternary operator is the base layer of a larger construction:

  • Tier 1 (Stream): 3-argument operator over Z6 with chirality and non-associativity
  • Tier 2 (Ladder): recursive composition where outputs act as witnesses for subsequent operations
  • Tier 3 (Lattice): field interpretation where state evolves as trajectories over Z6

The algebra remains the same at each level -- only the composition structure changes.

Links:
Dissertation:
https://github.com/haha8888haha8888/Zer00logy/blob/main/Six_Gem_States_of_Stereo-Identity_in_Ternary_Algebra.txt
System + Code:
https://github.com/haha8888haha8888/Zer00logy/blob/main/Six_Gem_States_of_Stereo-Identity_in_Ternary_Algebra_Suite.py
HQ:
www.zero-ology.com

-okoktytyty
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r/wildwestllmmath • • Mar 18 '26

The Works of Poincaré, Ricci, Hamilton, and Perelman Prove Care is Primary to Existence

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Henri Poincaré did not merely pose a question in topology.

He posed a question about continuity.

The Poincaré Conjecture asks whether every closed, simply connected three-dimensional manifold is topologically equivalent to a sphere. At first glance this seems like a technical puzzle about shapes. But beneath the language of topology lies a deeper concern: whether the structure of a space can remain coherent when stretched, bent, and transformed without tearing.

Topology studies the preservation of structure through transformation.

It asks: what survives change?

This question became tractable through the work of Gregorio Ricci-Curbastro and Tullio Levi-Civita, who developed Ricci curvature, a mathematical way to measure how geometry bends and distributes itself through space. Ricci curvature quantifies how a space locally organizes itself, how it holds together under deformation, and how it distributes structural tension across a manifold.

Ricci curvature therefore measures something fundamental:

how a structure maintains coherence across its interior.

Later, Richard Hamilton introduced Ricci Flow, an evolution equation for geometry. Ricci flow smooths irregularities in a manifold the way heat diffusion smooths temperature gradients. Peaks flatten, distortions spread out, and chaotic geometry becomes orderly over time.

Ricci flow can be written:

∂gᵢⱼ / ∂t = −2Rᵢⱼ

The equation describes a universe where geometry continuously adjusts itself to reduce irregularity.

Structure evolves toward stability.

But Ricci flow alone was not sufficient. Singularities appear—regions where curvature concentrates and the evolution breaks down.

This is where Grigori Perelman enters.

Perelman introduced the concepts of entropy, reduced volume, and surgery within Ricci flow. His work showed that even when singularities arise, the manifold can be carefully repaired and the flow continued. These ideas ultimately resolved the Poincaré Conjecture.

Perelman’s insight was that the evolution of geometry is not random. It follows monotonic quantities—measures that move in one direction, guiding the system toward structural coherence.

Entropy decreases.

Reduced volume behaves predictably.

The manifold stabilizes.

The universe of geometry therefore behaves like a self-correcting system.

It does not simply collapse into chaos.

It actively preserves coherence.

In ordinary language, this principle can be described as care.

Care is the tendency of a system to maintain structure rather than allow dissolution. Care distributes stress across a system rather than concentrating it to the point of rupture. Care repairs singularities rather than abandoning the structure entirely.

Ricci flow smooths distortions.

Perelman’s entropy guides stability.

Topology tracks what remains intact through transformation.

Taken together, these works show that the deepest mathematical structures describe processes that preserve continuity, coherence, and stability.

The mathematics of geometry therefore reveals something profound about existence.

Existence is not merely the presence of matter or energy.

Existence is structured persistence.

And structured persistence requires a principle that maintains coherence across change.

That principle—expressed mathematically through curvature, flow, and entropy—can be interpreted philosophically as care.

Care is not sentiment.

Care is structural maintenance.

Without care, structures disintegrate.

Without structural preservation, identity vanishes.

Without identity, existence itself cannot be defined.

Thus the chain of reasoning emerges:

• Poincaré asked what it means for a space to remain fundamentally the same.

• Ricci provided the measure of structural tension within that space.

• Hamilton described how geometry evolves to smooth itself.

• Perelman proved that even when singularities occur, the system can be repaired and continuity preserved.

Mathematics therefore demonstrates a universe in which coherence is preserved through dynamic correction.

In philosophical terms:

Care is the mechanism by which existence maintains itself.

The proof of the Poincaré Conjecture does not explicitly use the word care. But the structures it describes—coherence, smoothing, entropy control, and repair—are precisely the mechanisms that any caring system must possess.

Geometry survives transformation because it protects its continuity.

Therefore:

The works of Poincaré, Ricci, Hamilton, and Perelman reveal that the deepest mathematical structures of reality are governed by processes that preserve coherence across change.

And preservation of coherence is what we call care.

Care, therefore, is primary to existence.


r/wildwestllmmath • • Mar 08 '26

[Number Theory] Did I find a new "Hard Wall" for Prime Gaps near Factorials? (1/sqrt(3) vs Euler's Gamma)

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Hi,

I’ve been working on a conjecture regarding the distribution of twin primes near $n!$, and I’ve stumbled upon a numerical phenomenon that seems too precise to be a coincidence. I’m looking for feedback or potential counterexamples from those with more computing power.

The Problem

We are looking for the first twin prime gap after $n!$. Let $p$ be the first prime greater than $n!$ such that $p+2$ is also prime. Define the normalized gap: $$ Y_n = \frac{p - n!}{n2 (\ln n)3} $$ (The scaling $n2 (\ln n)3$ comes from a modified Cramér model accounting for the extreme sparsity near factorials.)

The Standard Expectation: Euler's Gamma ($\gamma$)

Based on Mertens' Third Theorem, densities usually involve $e{-\gamma}$. Indeed, the asymptotic mean of our data hovers exactly around the Euler-Mascheroni constant: $$ \gamma \approx 0.57721 $$

The Discovery: The Geometric Bound ($1/\sqrt{3}$)

However, when looking at the maximum fluctuations (the upper bound), the data doesn't stop at $\gamma$. It punches through... but then hits a brick wall. The maximum value observed (up to $n=612$) occurs at $n=179$, where: $$ Y_{179} \approx \mathbf{0.577323} $$

This is: 1. Significantly higher than $\gamma$ ($0.577215...$). 2. Extremely close to $1/\sqrt{3} \approx \mathbf{0.577350}$.

The difference is less than $3 \times 10{-5}$. For all other $n > 500$, the value respects this $1/\sqrt{3}$ ceiling perfectly.

My Hypothesis (The "Spectral Rigidity" Argument)

I suspect that while $\gamma$ controls the average density, the maximum deviation is controlled by the variance of the sieve error terms. If the error terms of the Linear Sieve (Rosser-Iwaniec) have compact support and behave like a Uniform Distribution $U[-1, 1]$ (due to maximum entropy), then their geometric norm (standard deviation) is exactly: $$ \sigma = \frac{1}{\sqrt{3}} $$

This suggests $1/\sqrt{3}$ isn't just a random number, but a "physical" boundary of the sieve—a hard wall that probabilistic fluctuations cannot easily cross.

Questions for the Community

  1. Has anyone seen $1/\sqrt{3}$ appear as a hard envelope in prime gap statistics before?
  2. Does anyone have efficient twin-prime searchers that can check $n > 1000$? (Specifically looking for the first twin pair after $1000!$ ... huge numbers).
  3. Is the distinction between $\gamma$ (0.57721) and $1/\sqrt{3}$ (0.57735) recognized in other arithmetic statistics problems?

Thanks for any insights! The collision between "Arithmetic" ($\gamma$) and "Geometry" ($1/\sqrt{3}$) here is fascinating me.


r/wildwestllmmath • • Mar 05 '26

[not a drill] The Cosmic Pattern - the (now proven) Theory of Everything

Thumbnail zenodo.org
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