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Algebra

92 missions · 41 completed

The study of algebraic structures — groups, rings, and fields — and, through algebraic geometry, the geometry of the solution sets of polynomial equations. Using commutative algebra to describe these varieties, the field provides a common language of symmetry and structure that underlies much of modern mathematics.

Missions

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Captain: Lucas

Fundamental Theorem of Galois Theory I: Galois Extensions and the Galois CorrespondenceTextbook

Motivation

Many questions about polynomial equations — which equations can be solved by radicals, which geometric constructions are possible with ruler and compass, how the roots of a polynomial are related — become questions about the symmetries of a field extension. The fundamental theorem of Galois theory, going back to Évariste Galois, is the dictionary that makes this possible: for a finite Galois extension it matches intermediate fields with subgroups of a finite group, so that questions about fields become questions in finite group theory. The same dictionary underlies Kummer theory and class field theory, and it is the step that turns the unsolvability of the general quintic (Abel–Ruffini) into a statement about solvable groups.

This mission follows the Wikipedia article Fundamental theorem of Galois theory (revision 1345286594): its main statement, its list of properties of the correspondence, three of its worked examples, and its section on the infinite case.

Setting

A field extension E/FE/FE/F is a field EEE with a field FFF inside it; it is finite when EEE is finite-dimensional as an FFF-vector space, of dimension [E:F][E:F][E:F]. An intermediate field is a field KKK with F⊆K⊆EF \subseteq K \subseteq EF⊆K⊆E. The automorphism group G=Aut⁡(E/F)G = \operatorname{Aut}(E/F)G=Aut(E/F) is the group of field automorphisms σ\sigmaσ of EEE with σ(a)=a\sigma(a) = aσ(a)=a for every a∈Fa \in Fa∈F.

The two maps of the correspondence are:

  • for a subgroup H≤GH \le GH≤G, the fixed field EH={x∈E:σ(x)=x for all σ∈H}E^H = \{x \in E : \sigma(x) = x \text{ for all } \sigma \in H\}EH={x∈E:σ(x)=x for all σ∈H};
  • for an intermediate field KKK, the fixing subgroup Aut⁡(E/K)={σ∈G:σ(x)=x for all x∈K}\operatorname{Aut}(E/K) = \{\sigma \in G : \sigma(x) = x \text{ for all } x \in K\}Aut(E/K)={σ∈G:σ(x)=x for all x∈K}.

The extension is Galois when it is normal and separable; for a finite extension this is equivalent to ∣G∣=[E:F]|G| = [E:F]∣G∣=[E:F]. When E/FE/FE/F is Galois, GGG is written Gal⁡(E/F)\operatorname{Gal}(E/F)Gal(E/F).

For an infinite algebraic Galois extension, GGG carries the Krull topology: the coarsest topology for which each restriction map G→Gal⁡(L/F)G \to \operatorname{Gal}(L/F)G→Gal(L/F), with L/FL/FL/F a finite Galois subextension and Gal⁡(L/F)\operatorname{Gal}(L/F)Gal(L/F) discrete, is continuous.

Formalization targets

Goal: Galois if and only if the correspondence is one-to-one

For a finite extension E/FE/FE/F,

E/F is Galois  ⟺  (∀K, EAut⁡(E/K)=K) and (∀H≤G, Aut⁡(E/EH)=H).E/F \text{ is Galois} \iff \Big(\forall K,\ E^{\operatorname{Aut}(E/K)} = K\Big) \text{ and } \Big(\forall H \le G,\ \operatorname{Aut}(E/E^H) = H\Big).E/F is Galois⟺(∀K, EAut(E/K)=K) and (∀H≤G, Aut(E/EH)=H).

Milestones

  1. Basic form (forward direction of the goal, already on the platform): for finite Galois E/FE/FE/F the two maps are mutually inverse.
  2. Non-Galois case: for finite non-Galois E/FE/FE/F, H↦EHH \mapsto E^HH↦EH is injective but not surjective, K↦Aut⁡(E/K)K \mapsto \operatorname{Aut}(E/K)K↦Aut(E/K) is surjective but not injective, and FFF is not the fixed field of any subgroup.
  3. Inclusion reversing: H1≤H2  ⟺  EH2⊆EH1H_1 \le H_2 \iff E^{H_2} \subseteq E^{H_1}H1​≤H2​⟺EH2​⊆EH1​.
  4. Degrees: [E:EH]=∣H∣[E : E^H] = |H|[E:EH]=∣H∣ and [EH:F]=[G:H][E^H : F] = [G : H][EH:F]=[G:H].
  5. Normality: EH/FE^H/FEH/F is normal   ⟺  \iff⟺ HHH is a normal subgroup.
  6. Quotient: if HHH is normal, restriction to EHE^HEH induces an isomorphism G/H≅Gal⁡(EH/F)G/H \cong \operatorname{Gal}(E^H/F)G/H≅Gal(EH/F).
  7. Example 1: K=Q(2,3)K = \mathbb{Q}(\sqrt2, \sqrt3)K=Q(2​,3​) has degree 444, is Galois, its Galois group is a Klein four-group, and it has five subgroups and five intermediate fields.
  8. Example 2: the splitting field of x3−2x^3 - 2x3−2 over Q\mathbb{Q}Q has degree 666, Galois group ≅S3\cong S_3≅S3​, six subgroups and six intermediate fields.
  9. Example 4: Q(23)\mathbb{Q}(\sqrt[3]{2})Q(32​) has degree 333, trivial automorphism group, and is not Galois.
  10. Infinite case, well-definedness: for any Galois extension, Aut⁡(E/K)\operatorname{Aut}(E/K)Aut(E/K) is closed in the Krull topology.
  11. Infinite case (already on the platform): intermediate fields correspond bijectively to closed subgroups.

Significance

The result. The correspondence turns the lattice of intermediate fields of a finite Galois extension into the (reversed) lattice of subgroups of a finite group, with degrees matching indices and normal subextensions matching normal subgroups. This is the tool used to classify subfields, to compute Galois groups of explicit polynomials, and to prove that solvability by radicals corresponds to solvability of the Galois group.

Formalizing it. The theorems are classical, and Mathlib contains formal proofs of the general finite and infinite correspondences (for example IsGalois.intermediateFieldEquivSubgroup and the InfiniteGalois namespace). This mission's contribution is a statement set indexed by the source: the converse direction ("only if Galois") as the goal, the non-Galois behaviour, each listed property, and the concrete examples of the article. The explicit examples require genuine computation: degrees of towers, minimal polynomials, and counting subgroups and subfields.

Difficulty

The general statements reduce to Artin's theorem and a degree count, but the non-Galois milestone asks for four separate claims about injectivity and surjectivity, each needing the correct direction of Artin's theorem. The examples cannot be settled by a general principle: showing that Q(2,3)\mathbb{Q}(\sqrt2,\sqrt3)Q(2​,3​) has exactly five intermediate fields, or that the splitting field of x3−2x^3-2x3−2 has degree 666, requires irreducibility arguments and an explicit transfer through the correspondence. Showing that Q(23)\mathbb{Q}(\sqrt[3]2)Q(32​) has no non-trivial automorphism requires knowing that the other two roots of x3−2x^3-2x3−2 are not real.

Formalization scope

All statements use Mathlib's IntermediateField F E, IntermediateField.fixedField, IntermediateField.fixingSubgroup, the automorphism group E ≃ₐ[F] E, and IsGalois (normal and separable). Finite means FiniteDimensional F E. Subgroups in the finite statements range over all subgroups; in the infinite case the Krull topology is Mathlib's standard topology on E ≃ₐ[F] E. Degrees are Module.finrank, orders are Nat.card, and the index is Subgroup.index. The concrete fields of the examples are taken inside R\mathbb{R}R (for Q(2,3)\mathbb{Q}(\sqrt2,\sqrt3)Q(2​,3​) and Q(23)\mathbb{Q}(\sqrt[3]2)Q(32​), with 23=21/3\sqrt[3]2 = 2^{1/3}32​=21/3 the real cube root) or as the abstract splitting field (for x3−2x^3-2x3−2). The quotient milestone takes the normality of HHH and of EH/FE^H/FEH/F as instance hypotheses; they are equivalent by milestone 5, so neither is vacuous.

The article's Example 3 (the anharmonic group acting on C(λ)\mathbb{C}(\lambda)C(λ)) and the "Applications" section are out of scope for this first mission. No new definitions are needed; contributions of proofs for any milestone are welcome.

Selected references

  • Wikipedia, Fundamental theorem of Galois theory, revision 1345286594. https://en.wikipedia.org/w/index.php?title=Fundamental_theorem_of_Galois_theory&oldid=1345286594
  • J. S. Milne, Fields and Galois Theory, Kea Books, 2022. https://www.jmilne.org/math/CourseNotes/ft.html
  • The Stacks Project, Theorem 9.21.7 (Fundamental theorem of Galois theory). https://stacks.math.columbia.edu/tag/09DW
  • The Stacks Project, Theorem 9.22.4 (Fundamental theorem of infinite Galois theory). https://stacks.math.columbia.edu/tag/0BML
  • L. Ribes, P. Zalesskii, Profinite Groups, Springer, 2010. ISBN 978-3-642-01641-7.
12 thms6 active usersReviewed
🏆Completed
Pure Mathematics·Captain: ShouqiaoWang

Symplectic Modules Free over an Abelian NilradicalResearch Paper

Motivation

Polynomial representations provide a concrete way to study modules over Lie algebras: the underlying vector space is a polynomial ring, while the Lie generators act by explicit multiplication, shift, and differential operators. Chen and Tan classify a family of modules over the symplectic Lie algebra sp2ℓ(C)\mathfrak{sp}_{2\ell}(\mathbb C)sp2ℓ​(C) that are free of rank one over the universal enveloping algebra of an abelian nilradical. Their paper determines the family, its isomorphism classes, its weight and simplicity criteria, its finite-length behavior at exceptional parameters, and an application to Hamiltonian Lie algebras. This mission packages those headline results into one common Lean target, corresponding to Theorems 1.1--1.3 of Chen--Tan.

The common-family formulation matters. The source does not assert three unrelated existence theorems: one explicit two-parameter family τ(C,Φ)\tau(C,\Phi)τ(C,Φ) carries all of the classification, simplicity, finite-length, and Hamiltonian consequences. The Lean goal therefore quantifies that family once and requires all headline properties of the same witness.

Setting

Fix ℓ≥2\ell\ge2ℓ≥2 and the complex symplectic Lie algebra sp2ℓ(C)\mathfrak{sp}_{2\ell}(\mathbb C)sp2ℓ​(C). The relevant maximal parabolic subalgebra has an abelian nilradical n\mathfrak nn. Its enveloping algebra is a polynomial algebra in the root generators, represented formally by a multivariate polynomial ring. A rank-one free U(n)U(\mathfrak n)U(n)-module can consequently be modeled on that polynomial ring.

The definition bundle presents the simple Chevalley generators and their action by explicit operators depending on a scalar C∈CC\in\mathbb CC∈C and a polynomial parameter Φ\PhiΦ. Rather than assuming that these formulas already form a representation, the target asks for a generator presentation satisfying the symplectic Lie relations and for a representation family τ(C,Φ)\tau(C,\Phi)τ(C,Φ) realizing the formulas. It also formalizes module equivalence, weight spaces, simplicity, Noetherian and Artinian conditions, finite composition factors, and the Shen--Larsson construction for a Hamiltonian Lie algebra.

Formalization targets

Common polynomial-module family

Prove that for every ℓ≥2\ell\ge2ℓ≥2 there is one generator presentation and one family

(C,Φ)⟼τ(C,Φ)(C,\Phi)\longmapsto \tau(C,\Phi)(C,Φ)⟼τ(C,Φ)

of sp2ℓ(C)\mathfrak{sp}_{2\ell}(\mathbb C)sp2ℓ​(C)-representations on the polynomial ring, free of rank one over the abelian nilradical, satisfying the explicit generator formulas. Prove the source's classification and isomorphism criteria, including that τ(C,Φ)\tau(C,\Phi)τ(C,Φ) is a weight module exactly when Φ\PhiΦ is constant, and the stated simplicity criterion outside the exceptional arithmetic set

{ℓ+12−n2:n∈Z>0}.\left\{\frac{\ell+1}{2}-\frac{n}{2}:n\in\mathbb Z_{>0}\right\}.{2ℓ+1​−2n​:n∈Z>0​}.

For exceptional CCC, prove the Noetherian/Artinian and finite-composition-series conclusions and the weight/nonweight classification of the composition factors. Finally, prove that the canonical Hamiltonian Shen--Larsson construction has the exact degree-weight spaces and the source's simplicity and weight-module consequences. All clauses must be witnessed by the same family τ\tauτ.

Significance

The result gives a complete algebraic description of a large concrete class of non-highest-weight modules. It separates the generic simple regime from an exceptional finite-length regime and shows how nonweight symplectic modules generate weight modules over an infinite-dimensional Hamiltonian Lie algebra. The explicit formulas make the family suitable for calculation, while the classification prevents duplicate parameter choices from being mistaken for genuinely different modules.

Formalization adds checks that are easy to blur in prose. In particular, the generator formulas cannot be called a Lie representation until the defining relations have been verified, and the same witness must support every later theorem. A completed proof will contribute reusable Lean infrastructure for symplectic root data, polynomial representations, module-theoretic finiteness, exact weight-space descriptions, and Hamiltonian Lie-algebra functors. The paper's proofs are known; the open task is their machine-checked reconstruction.

Difficulty

The first obstacle is structural rather than computational. Checking formulas on individual generators is insufficient: all Chevalley and Serre relations must hold with the correct operator order and signs, after which the action must extend to the full Lie algebra. Classification then requires controlling arbitrary rank-one-free modules, not merely verifying that the displayed examples exist.

The exceptional parameters introduce a second layer. Generic simplicity and exceptional finite length are logically different claims, and the composition-factor statement must be tied to the same parameterized representation. The Hamiltonian application adds another algebra and a tensor construction; exact weight spaces and simplicity cannot be obtained by treating the functor as an opaque interface. The Lean goal deliberately keeps these obligations inside one theorem so that separate convenient witnesses cannot satisfy different portions.

Formalization scope

The mission works over C\mathbb CC with natural rank ℓ≥2\ell\ge2ℓ≥2. The definition bundle uses concrete multivariate polynomials, matrices and linear maps, a presented symplectic Lie algebra, Lie representations, submodules, and tensor products. The exceptional set is expressed with complex coercions, so no accidental natural-number division is involved. The nilradical action, freeness, parameter equivalence, weight-space equalities, simplicity, finite-length properties, and Hamiltonian brackets are transparent propositions in the bundle.

The final theorem is a single conjunction under one existentially quantified presentation and one existentially quantified family τ\tauτ. Several convenient corollaries can be projected from it, but they are not independent targets and do not permit different witnesses. The bundle contains no custom axioms or opaque semantic assumptions, and the only admitted term is the main theorem's sorry. Contributions may split the proof into source-numbered lemmas about generator relations, classification, exceptional submodules, or the Shen--Larsson application, provided the shared-family quantifier structure is preserved.

Selected references

  • Yang Chen and Haijun Tan, Simple sp2ℓ(C)\mathfrak{sp}_{2\ell}(\mathbb C)sp2ℓ​(C)-modules which are free over an abelian nilradical, Journal of Algebra 697 (2026), 341--372, Theorems 1.1--1.3 (formal Theorems 3.7, 3.8, 4.7, 4.9, and 5.2). DOI
  • G. Shen, foundational work on mixed-product constructions for modules over Lie algebras of Cartan type, cited in the source paper for the Shen--Larsson functor.
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Number Theory·Captain: mikedeng1

On Ideal Lattices and Learning with Errors over Rings: Multiplication by t ∈ I with tI⁻¹ Coprime to J Induces an R-Module Isomorphism M/JM ≅ IM/IJMResearch Paper

Background and motivation

Ring learning with errors (ring-LWE) is the algebraic variant of the learning-with-errors problem on which most practical lattice-based cryptography is built, including the key-encapsulation scheme ML-KEM standardized by NIST in 2024. Its hardness rests on the paper of Lyubashevsky, Peikert and Regev, On ideal lattices and learning with errors over rings (J. ACM 60(6), 2013, doi:10.1145/2535925; conference version at EUROCRYPT 2010). The paper's main theorem (Theorem 3.6, p. 19) is a polynomial-time quantum reduction from worst-case approximate shortest-vector problems on ideal lattices to the ring-LWE decision problem. Statements about reductions, running times and negligible probabilities are outside the scope of this mission.

What this mission formalizes is the algebraic tool both of the paper's reductions rest on, which the authors list among their main technical contributions (p. 7): a Chinese-remainder technique for clearing an ideal. An arbitrary ideal I\mathcal{I}I of the ring of integers RRR need not be principal, so a reduction that receives samples from a lattice I\mathcal{I}I cannot simply divide by a generator. Lemmas 2.14 and 2.15 show that, modulo an ideal J\mathcal{J}J such as ⟨q⟩\langle q\rangle⟨q⟩, multiplication by a well-chosen t∈It\in\mathcal{I}t∈I identifies R/qRR/qRR/qR with I/qI\mathcal{I}/q\mathcal{I}I/qI, and more generally M/JM\mathcal{M}/\mathcal{J}\mathcal{M}M/JM with IM/IJM\mathcal{I}\mathcal{M}/\mathcal{I}\mathcal{J}\mathcal{M}IM/IJM for every fractional ideal M\mathcal{M}M. Steps 1–3 of the BDD-to-LWE reduction of §4.2 consist of exactly these identifications. The authors note that the lemmas are "probably standard for experts in computational number theory" (p. 16); the formulation used in lattice cryptography is theirs, and it is reused throughout the later literature on algebraic lattices.

Setting

Let KKK be a number field of degree nnn and R=OKR = \mathcal{O}_KR=OK​ its ring of integers. An integral ideal is a nonzero ideal I⊆R\mathcal{I}\subseteq RI⊆R (the paper excludes {0}\{0\}{0}, footnote 2, p. 13). A fractional ideal is a set I⊂K\mathcal{I}\subset KI⊂K such that dId\mathcal{I}dI is an integral ideal for some nonzero d∈Rd\in Rd∈R; the nonzero fractional ideals form a group under multiplication, and I−1\mathcal{I}^{-1}I−1 denotes the inverse. Two integral ideals are coprime when I+J=R\mathcal{I}+\mathcal{J} = RI+J=R.

For t∈Rt\in Rt∈R the cleared ideal is t⋅I−1=⟨t⟩ I−1t\cdot\mathcal{I}^{-1} = \langle t\rangle\,\mathcal{I}^{-1}t⋅I−1=⟨t⟩I−1. When t∈It\in\mathcal{I}t∈I it is an integral ideal, and "t⋅I−1t\cdot\mathcal{I}^{-1}t⋅I−1 is coprime to J\mathcal{J}J" means

t⋅I−1⊆Randt⋅I−1+J=R.t\cdot\mathcal{I}^{-1}\subseteq R \quad\text{and}\quad t\cdot\mathcal{I}^{-1}+\mathcal{J}=R .t⋅I−1⊆Randt⋅I−1+J=R.

For a fractional ideal M\mathcal{M}M and t∈It\in\mathcal{I}t∈I, the map θt(u)=t⋅u\theta_t(u) = t\cdot uθt​(u)=t⋅u sends M\mathcal{M}M into IM\mathcal{I}\mathcal{M}IM, and therefore induces an RRR-linear map

θt: M⟶IM/IJM,u↦tu mod IJM.\theta_t:\ \mathcal{M}\longrightarrow \mathcal{I}\mathcal{M}/\mathcal{I}\mathcal{J}\mathcal{M},\qquad u\mapsto t u \bmod \mathcal{I}\mathcal{J}\mathcal{M}.θt​: M⟶IM/IJM,u↦tumodIJM.

The dual of a fractional ideal L\mathcal{L}L is L∨={x∈K:Tr⁡(xL)⊆Z}\mathcal{L}^\vee = \{x\in K:\operatorname{Tr}(x\mathcal{L})\subseteq\mathbb{Z}\}L∨={x∈K:Tr(xL)⊆Z}; R∨R^\veeR∨ is the codifferent, and I∨=I−1R∨\mathcal{I}^\vee = \mathcal{I}^{-1}R^\veeI∨=I−1R∨. For the cyclotomic field K=Q(ζ)K=\mathbb{Q}(\zeta)K=Q(ζ), ζ\zetaζ a primitive mmm-th root of unity, τk\tau_kτk​ (k∈Zm∗k\in\mathbb{Z}_m^*k∈Zm∗​) is the automorphism with τk(ζ)=ζk\tau_k(\zeta)=\zeta^kτk​(ζ)=ζk, and for a prime q≡1(modm)q\equiv 1\pmod mq≡1(modm) with a primitive mmm-th root of unity ω∈Zq\omega\in\mathbb{Z}_qω∈Zq​ the primes above qqq are qi=⟨q,ζ−ωi⟩\mathfrak{q}_i = \langle q,\zeta-\omega^i\rangleqi​=⟨q,ζ−ωi⟩, i∈Zm∗i\in\mathbb{Z}_m^*i∈Zm∗​. Calligraphic I,J,M\mathcal{I},\mathcal{J},\mathcal{M}I,J,M of the paper are written I, J, M in the milestone texts.

Formalization targets

Goal: Lemma 2.15 (p. 17)

For nonzero ideals I,J⊆R\mathcal{I},\mathcal{J}\subseteq RI,J⊆R, t∈It\in\mathcal{I}t∈I with t⋅I−1t\cdot\mathcal{I}^{-1}t⋅I−1 coprime to J\mathcal{J}J, and a nonzero fractional ideal M\mathcal{M}M,

θt: M→IM/IJM is surjective with kernel JM,soM/JM  ≅  IM/IJM\theta_t:\ \mathcal{M}\to\mathcal{I}\mathcal{M}/\mathcal{I}\mathcal{J}\mathcal{M}\ \text{is surjective with kernel}\ \mathcal{J}\mathcal{M},\quad\text{so}\quad \mathcal{M}/\mathcal{J}\mathcal{M}\;\cong\;\mathcal{I}\mathcal{M}/\mathcal{I}\mathcal{J}\mathcal{M}θt​: M→IM/IJM is surjective with kernel JM,soM/JM≅IM/IJM

as RRR-modules, via u mod JM↦tu mod IJMu\bmod\mathcal{J}\mathcal{M}\mapsto tu\bmod\mathcal{I}\mathcal{J}\mathcal{M}umodJM↦tumodIJM.

Milestones

  1. The existence content of Lemma 2.13 (a coprime pair has c∈Jc\in\mathcal{J}c∈J with c≡1 mod Ic\equiv 1\bmod\mathcal{I}c≡1modI), already proved on the platform and entered as a reference. Lemma 2.12 (Chinese Remainder Theorem) is also included as a reference item, without being a milestone.
  2. Lemma 2.14 (p. 16): for nonzero I,J\mathcal{I},\mathcal{J}I,J there exists a nonzero t∈It\in\mathcal{I}t∈I with t⋅I−1t\cdot\mathcal{I}^{-1}t⋅I−1 coprime to J\mathcal{J}J.
  3. The kernel claim of the proof of Lemma 2.15: u∈Mu\in\mathcal{M}u∈M and tu∈IJMtu\in\mathcal{I}\mathcal{J}\mathcal{M}tu∈IJM imply u∈JMu\in\mathcal{J}\mathcal{M}u∈JM.
  4. The surjectivity claim of the proof: if c∈t⋅I−1c\in t\cdot\mathcal{I}^{-1}c∈t⋅I−1 and c≡1 mod Jc\equiv1\bmod\mathcal{J}c≡1modJ, then for v∈IMv\in\mathcal{I}\mathcal{M}v∈IM, cv∈tMcv\in t\mathcal{M}cv∈tM and cv−v∈IJMcv-v\in\mathcal{I}\mathcal{J}\mathcal{M}cv−v∈IJM.

Companion statements

  • §4.2 step 2 (p. 23) and step 3 (p. 24): multiplication by ttt is a bijection R/qR→I/qIR/qR\to\mathcal{I}/q\mathcal{I}R/qR→I/qI and I∨/qI∨→R∨/qR∨\mathcal{I}^\vee/q\mathcal{I}^\vee\to R^\vee/qR^\veeI∨/qI∨→R∨/qR∨ for every integer q≥2q\ge2q≥2, the two instances of Lemma 2.15 the reduction uses.
  • Lemma 2.16 (p. 17): τj(qi)=qi/j\tau_j(\mathfrak{q}_i)=\mathfrak{q}_{i/j}τj​(qi​)=qi/j​ for all i,j∈Zm∗i,j\in\mathbb{Z}_m^*i,j∈Zm∗​.
  • Lemma 2.9 (p. 14): n1/pN(I)1/n≤λ1(I)≤n1/pN(I)1/nΔK1/nn^{1/p}N(\mathcal{I})^{1/n}\le\lambda_1(\mathcal{I})\le n^{1/p}N(\mathcal{I})^{1/n}\sqrt{\Delta_K^{1/n}}n1/pN(I)1/n≤λ1​(I)≤n1/pN(I)1/nΔK1/n​​ in every ℓp\ell_pℓp​ norm, p∈[1,∞]p\in[1,\infty]p∈[1,∞], stated as two items.

Significance

The isomorphism of Lemma 2.15 is what makes ideal lattices usable in worst-case to average-case reductions: it turns a discrete Gaussian sample from an arbitrary ideal I\mathcal{I}I into a uniform element of the fixed ring RqR_qRq​, and turns the ring-LWE secret in Rq∨R^\vee_qRq∨​ back into a coset of qI∨q\mathcal{I}^\veeqI∨. Lemma 2.16 is the corresponding tool for the search-to-decision reductions of §5, which move between the CRT components R/qiR/\mathfrak{q}_iR/qi​ of a completely split qqq. Lemma 2.9 gives the scale of the lattices involved.

On the formal side, none of Lemmas 2.14–2.16 is stated on the platform or in Mathlib in this form. Mathlib has the Chinese remainder theorem for ideals, inverses of fractional ideals in Dedekind domains, trace duals with I∨=I−1R∨\mathcal{I}^\vee=\mathcal{I}^{-1}R^\veeI∨=I−1R∨, and the isomorphism Gal(Q(ζm)/Q)≅(Z/mZ)∗\mathrm{Gal}(\mathbb{Q}(\zeta_m)/\mathbb{Q})\cong(\mathbb{Z}/m\mathbb{Z})^*Gal(Q(ζm​)/Q)≅(Z/mZ)∗; the mission connects these to the quotient modules and explicit primes that lattice cryptography works with. All statements are proved in the paper; what remains is the formal proof.

Difficulty

The obvious argument for Lemma 2.15 — both quotients have cardinality N(J)N(\mathcal{J})N(J), so an injective map is bijective — needs the multiplicativity of the norm on fractional ideals and finiteness of the quotients, and still needs the kernel computation, which uses unique factorization: from tu∈IJMtu\in\mathcal{I}\mathcal{J}\mathcal{M}tu∈IJM one has to cancel I\mathcal{I}I and M\mathcal{M}M inside the group of fractional ideals and then use coprimality of tI−1t\mathcal{I}^{-1}tI−1 and J\mathcal{J}J. Lemma 2.14 needs the factorization of I\mathcal{I}I along the primes of J\mathcal{J}J and a CRT choice of ttt; for J=0\mathcal{J}=0J=0 it would assert that I\mathcal{I}I is principal, which is why the nonzero convention matters. In Lemma 2.16 the delicate point is the direction of the action: τj\tau_jτj​ sends qi\mathfrak{q}_iqi​ to qi/j\mathfrak{q}_{i/j}qi/j​, not qij\mathfrak{q}_{ij}qij​.

Formalization scope

  • KKK is a NumberField, RRR is 𝓞 K, fractional ideals are FractionalIdeal (𝓞 K)⁰ K, and integral ideals are coerced into them. Ideals are nonzero, per footnote 2: every statement carries I ≠ ⊥ (and J ≠ ⊥, M ≠ 0 where the paper's convention applies); I ≠ ⊥ is essential because Lean defines 0−1=00^{-1}=00−1=0. Two kernel/surjectivity milestones drop the nonzero hypotheses on J\mathcal{J}J and M\mathcal{M}M, which only strengthens them.
  • "tI−1t\mathcal{I}^{-1}tI−1 coprime to J\mathcal{J}J" is the predicate ClearedCoprime: tI−1≤1t\mathcal{I}^{-1}\le 1tI−1≤1 and tI−1+J=1t\mathcal{I}^{-1}+\mathcal{J}=1tI−1+J=1 in the semiring of fractional ideals.
  • M/N\mathcal{M}/\mathcal{N}M/N is the quotient of the RRR-module M\mathcal{M}M by N∩M\mathcal{N}\cap\mathcal{M}N∩M; θt\theta_tθt​ is the given RRR-linear map M→IM/IJM\mathcal{M}\to\mathcal{I}\mathcal{M}/\mathcal{I}\mathcal{J}\mathcal{M}M→IM/IJM. The goal states surjectivity and the kernel of this map. A bare statement that some isomorphism M/JM≅IM/IJM\mathcal{M}/\mathcal{J}\mathcal{M}\cong\mathcal{I}\mathcal{M}/\mathcal{I}\mathcal{J}\mathcal{M}M/JM≅IM/IJM exists would be true for unrelated reasons and is not the lemma.
  • Duals are Mathlib's FractionalIdeal.dual ℤ ℚ. τj\tau_jτj​ is the inverse image of jjj under IsCyclotomicExtension.Rat.galEquivZMod, acting on ideals by images; ωi\omega^iωi uses the representative of iii in {0,…,m−1}\{0,\dots,m-1\}{0,…,m−1}. ℓp\ell_pℓp​ norms sum over all nnn complex embeddings; λ1\lambda_1λ1​ bounds are phrased through nonzero elements of I\mathcal{I}I.
  • Dropped algorithmic clauses: "such ttt can be found efficiently" (Lemma 2.14), "this isomorphism may be efficiently inverted" (Lemma 2.15), the "deterministic polynomial-time algorithm" of Lemma 2.13 (only the existence of ccc is referenced), and "which can be efficiently inverted" in §4.2. No complexity notion is encoded.
  • Contributions welcome: proofs of the milestones, of the goal from them, and of the companion statements; general lemmas on quotients M/JM\mathcal{M}/\mathcal{J}\mathcal{M}M/JM of fractional ideals are reusable beyond this mission.

Selected references

  • V. Lyubashevsky, C. Peikert, O. Regev, On ideal lattices and learning with errors over rings, J. ACM 60(6), Article 43, 2013. https://doi.org/10.1145/2535925
  • V. Lyubashevsky, C. Peikert, O. Regev, On ideal lattices and learning with errors over rings, EUROCRYPT 2010, LNCS 6110, pp. 1–23. https://doi.org/10.1007/978-3-642-13190-5_1
  • O. Regev, On lattices, learning with errors, random linear codes, and cryptography, J. ACM 56(6), 2009. https://doi.org/10.1145/1568318.1568324
  • NIST, FIPS 203: Module-Lattice-Based Key-Encapsulation Mechanism Standard, 2024. https://doi.org/10.6028/NIST.FIPS.203
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Algebraic Geometry·Captain: Lucas

Hilbert's Nullstellensatz (Wikipedia) I: Formulations over Algebraically Closed FieldsTextbook

Motivation

Hilbert's Nullstellensatz ("theorem of zeros") is the basic link between algebra and geometry. It was proved by David Hilbert in his second major paper on invariant theory in 1893, after his 1890 paper that proved the basis theorem, and it is a foundational result of algebraic geometry. It gives an algebraic criterion for when a system of polynomial equations over an algebraically closed field has a solution, and an algebraic criterion for when one polynomial vanishes wherever a given family does. Every dictionary between affine varieties and ideals — points and maximal ideals, algebraic sets and radical ideals, irreducible sets and prime ideals — is a consequence.

This mission follows the Wikipedia article Hilbert's Nullstellensatz (snapshot of 27 September 2026): its introduction, its section Formulations, the statement of Zariski's lemma from Proofs, and the first theorem of Generalizations (finitely generated algebras over Jacobson rings).

Setting

Let kkk be a field and KKK an algebraically closed field extension of kkk (every non-constant polynomial over KKK has a root in KKK). Write k[X1,…,Xn]k[X_1,\dots,X_n]k[X1​,…,Xn​] for the polynomial ring in nnn variables. A point is an nnn-tuple a=(a1,…,an)∈Kna = (a_1,\dots,a_n) \in K^na=(a1​,…,an​)∈Kn, and f(a)f(a)f(a) is the value of a polynomial fff at aaa.

  • For an ideal JJJ, the algebraic set (zero locus) is V(J)={a∈Kn:f(a)=0 for all f∈J}\mathrm V(J) = \{a \in K^n : f(a) = 0 \text{ for all } f \in J\}V(J)={a∈Kn:f(a)=0 for all f∈J}.
  • For U⊆KnU \subseteq K^nU⊆Kn, the vanishing ideal is I(U)={p:p(a)=0 for all a∈U}\mathrm I(U) = \{p : p(a) = 0 \text{ for all } a \in U\}I(U)={p:p(a)=0 for all a∈U}.
  • The radical of JJJ is J={p:pr∈J for some r∈N}\sqrt J = \{p : p^r \in J \text{ for some } r \in \mathbb N\}J​={p:pr∈J for some r∈N}.
  • For a∈Kna \in K^na∈Kn, ma=(X1−a1,…,Xn−an)\mathfrak m_a = (X_1 - a_1, \dots, X_n - a_n)ma​=(X1​−a1​,…,Xn​−an​) is the ideal of the point.
  • A subset W⊆KnW \subseteq K^nW⊆Kn is irreducible (Zariski topology) if it is nonempty and is not covered by two algebraic sets without lying in one of them.
  • A commutative ring is Jacobson if every radical ideal is an intersection of maximal ideals.

Formalization targets

Goal: the Nullstellensatz

If p∈k[X1,…,Xn]p \in k[X_1,\dots,X_n]p∈k[X1​,…,Xn​] vanishes on V(J)⊆Kn\mathrm V(J) \subseteq K^nV(J)⊆Kn, then

∃ r∈N,pr∈J.\exists\, r \in \mathbb N,\qquad p^r \in J.∃r∈N,pr∈J.

This is the statement of the article's section Formulations, with the coefficient field kkk and the algebraically closed field KKK allowed to differ.

Milestones

  1. Systems of equations. Over algebraically closed KKK: a system f1=⋯=fm=0f_1 = \dots = f_m = 0f1​=⋯=fm​=0 has no solution in KnK^nKn iff g1f1+⋯+gmfm=1g_1 f_1 + \dots + g_m f_m = 1g1​f1​+⋯+gm​fm​=1 for some gig_igi​; and fff vanishes on all solutions iff fr=g1f1+⋯+gmfmf^r = g_1 f_1 + \dots + g_m f_mfr=g1​f1​+⋯+gm​fm​ for some rrr and gig_igi​.
  2. Geometric form. I(V(J))=J\mathrm I(\mathrm V(J)) = \sqrt JI(V(J))=J​.
  3. Weak Nullstellensatz. A proper ideal of k[X1,…,Xn]k[X_1,\dots,X_n]k[X1​,…,Xn​] has a common zero in KnK^nKn; algebraic closedness is needed, as (X2+1)⊆R[X](X^2+1) \subseteq \mathbb R[X](X2+1)⊆R[X] shows; for K=CK = \mathbb CK=C, n=1n = 1n=1 this is the fundamental theorem of algebra: PPP has a complex root iff deg⁡P≠0\deg P \ne 0degP=0.
  4. Correspondences. V\mathrm VV is an order-reversing bijection from radical ideals onto algebraic sets, with inverse I\mathrm II; I({a})=ma\mathrm I(\{a\}) = \mathfrak m_aI({a})=ma​ is maximal; every maximal ideal of K[X1,…,Xn]K[X_1,\dots,X_n]K[X1​,…,Xn​] is some ma\mathfrak m_ama​; an algebraic set WWW is irreducible iff I(W)\mathrm I(W)I(W) is prime.
  5. Intersections. J=⋂m⊇Jm=⋂a∈V(J)ma\sqrt J = \bigcap_{\mathfrak m \supseteq J} \mathfrak m = \bigcap_{a \in \mathrm V(J)} \mathfrak m_aJ​=⋂m⊇J​m=⋂a∈V(J)​ma​.
  6. Zariski's lemma. A field finitely generated as an algebra over a field KKK is a finite extension of KKK.
  7. Jacobson rings. A finitely generated algebra SSS over a Jacobson ring RRR is Jacobson, and for a maximal ideal n⊆S\mathfrak n \subseteq Sn⊆S, n∩R\mathfrak n \cap Rn∩R is maximal and S/nS/\mathfrak nS/n is finite over R/(n∩R)R/(\mathfrak n \cap R)R/(n∩R).

Significance

The Nullstellensatz makes the zero sets of polynomial systems accessible through ideals: solvability of a system becomes the ideal-membership question 1∈J1 \in J1∈J, and the geometry of algebraic sets becomes the algebra of radical ideals. Consequences include the identification of the points of KnK^nKn with the maximal ideals of K[X1,…,Xn]K[X_1,\dots,X_n]K[X1​,…,Xn​], the description of irreducible algebraic sets by prime ideals, and the reduction of the fundamental theorem of algebra to the case n=1n=1n=1. The Jacobson-ring version extends the first equality of the intersection formula to every finitely generated algebra over a field.

All statements here are classical and proved. Mathlib already contains versions of several of them in its own vocabulary (Jacobson rings, Zariski's lemma, and a Nullstellensatz over an algebraically closed coefficient field). What this mission adds is a single set of statements matching the article's formulations: the version with separate fields k⊆Kk \subseteq Kk⊆K, the explicit systems-of-equations form, the point-ideal and irreducibility correspondences over KnK^nKn, and the intersection formula — and, for solvers, the bridges from these concrete statements to Mathlib's abstract ones.

Difficulty

The inclusion J⊆I(V(J))\sqrt J \subseteq \mathrm I(\mathrm V(J))J​⊆I(V(J)) is immediate; the content is the reverse inclusion, which requires producing a point of KnK^nKn from purely algebraic data. When k≠Kk \ne Kk=K the ideal JJJ lives over kkk while the points live over KKK, so a result stated only for K[X1,…,Xn]K[X_1,\dots,X_n]K[X1​,…,Xn​] does not apply directly: an ideal of k[X]k[X]k[X] must be related to the ideal it generates in K[X]K[X]K[X] without losing membership information. For the correspondences, the explicit ideals ma\mathfrak m_ama​ and the closed-set definition of irreducibility must be matched with the abstract notions (maximal spectrum, irreducible closed subsets) used in the library.

Formalization scope

  • Points of KnK^nKn are functions Fin n→K\mathrm{Fin}\,n \to KFinn→K; polynomials are MvPolynomial (Fin n) k. When k≠Kk \ne Kk=K, KKK is a kkk-algebra and evaluation of a polynomial over kkk at a point of KnK^nKn goes through k→Kk \to Kk→K.
  • n=0n = 0n=0 is allowed throughout; so is the unit ideal J=k[X]J = k[X]J=k[X], where V(J)=∅\mathrm V(J) = \emptysetV(J)=∅ and empty intersections of ideals are the whole ring.
  • Irreducibility is stated through closed sets (algebraic sets) without putting a topology on KnK^nKn. The degree in the n=1n=1n=1 statement is Mathlib's Polynomial.degree, with deg⁡0=−∞\deg 0 = -\inftydeg0=−∞.
  • In the goal, the exponent rrr may be 000; that witness only works when JJJ is the unit ideal, so it does not trivialize the statement.
  • Out of scope: the proofs via resultants and Gröbner bases, the effective Nullstellensatz, Lang's infinite-variable version, the scheme-theoretic generalizations, and the projective and analytic Nullstellensätze.
  • Reusable output: the definitions V\mathrm VV, I\mathrm II, algebraic set, irreducible set and ma\mathfrak m_ama​, and bridges to Mathlib's MvPolynomial.zeroLocus, MvPolynomial.vanishingIdeal, and IsJacobsonRing.

Selected references

  • D. Hilbert, Ueber die vollen Invariantensysteme, Mathematische Annalen 42 (1893).
  • Wikipedia contributors, Hilbert's Nullstellensatz. https://en.wikipedia.org/wiki/Hilbert%27s_Nullstellensatz
  • M. F. Atiyah, I. G. Macdonald, Introduction to Commutative Algebra, Addison-Wesley, 1969, Chapters 5 and 7.
  • D. Eisenbud, Commutative Algebra with a View Toward Algebraic Geometry, Springer GTM 150, 1995, Chapter 4.
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Representation Theory·Captain: lisamegawatts

Clifford Casimir I: Odd-Sector Adjoint Spectrum on Cl(6,0)Research Paper

Motivation

The real Clifford algebra Cl(6,0)\mathrm{Cl}(6,0)Cl(6,0) is the smallest Euclidean Clifford algebra whose full structure carries a nontrivial multiplicity-eight representation-theoretic decomposition, and it has become a recurring object in programs that build internal gauge and family structure from Clifford generators rather than imposing it by hand. Within such programs, the single most basic representation-theoretic question one can ask about the algebra is: how does a distinguished su(2)\mathfrak{su}(2)su(2) subalgebra, acting by the adjoint action, decompose the odd part of the algebra as a representation?

This mission answers that question exactly, for the specific triple of bivectors built on the index set {0,2,5}\{0,2,5\}{0,2,5}. The computation was carried out structurally (by splitting active indices from spectator indices) in the LeanProofs research program in 2026 and recorded with exact multiplicities; no machine-checked proof exists yet. The purpose here is to close that gap: the result is finite-dimensional linear algebra, completely within reach of a Lean 4 + Mathlib development, and every constant in it is explicit.

Setting

Fix R6\mathbb{R}^6R6 with its standard inner product and the associated quadratic form Q60=diag(1,1,1,1,1,1)Q_{60} = \mathrm{diag}(1,1,1,1,1,1)Q60​=diag(1,1,1,1,1,1), and let Cl(6,0)=CliffordAlgebra(Q60)\mathrm{Cl}(6,0) = \mathrm{CliffordAlgebra}(Q_{60})Cl(6,0)=CliffordAlgebra(Q60​) be the real Clifford algebra generated by symbols e0,…,e5e_0,\dots,e_5e0​,…,e5​ with

ei2=1,eiej=−ejei  (i≠j).e_i^2 = 1, \qquad e_i e_j = -e_j e_i \ \ (i \neq j).ei2​=1,ei​ej​=−ej​ei​  (i=j).

The algebra is Z\mathbb{Z}Z-graded in the usual sense: it is the direct sum of its grade-kkk subspaces, spanned by products of kkk distinct generators, of dimension (6k)\binom{6}{k}(k6​). The odd sector is the linear span of the odd grades,

Cl−(6,0)  =  grade1⊕grade3⊕grade5,dim⁡RCl−(6,0)=6+20+6=32.\mathrm{Cl}^-(6,0) \;=\; \mathrm{grade}_1 \oplus \mathrm{grade}_3 \oplus \mathrm{grade}_5, \qquad \dim_{\mathbb{R}} \mathrm{Cl}^-(6,0) = 6 + 20 + 6 = 32.Cl−(6,0)=grade1​⊕grade3​⊕grade5​,dimR​Cl−(6,0)=6+20+6=32.

On it, register three bivectors and their halved adjoint actions:

E1=e0e2,E2=e2e5,E3=e0e5,Ti=12 adEi,E_1 = e_0 e_2, \quad E_2 = e_2 e_5, \quad E_3 = e_0 e_5, \qquad T_i = \tfrac{1}{2}\,\mathrm{ad}_{E_i},E1​=e0​e2​,E2​=e2​e5​,E3​=e0​e5​,Ti​=21​adEi​​,

where adX(Y)=XY−YX\mathrm{ad}_{X}(Y) = XY - YXadX​(Y)=XY−YX. The triple satisfies the su(2)\mathfrak{su}(2)su(2) relations [E1,E2]=2E3[E_1,E_2]=2E_3[E1​,E2​]=2E3​ and cyclic permutations, so the TiT_iTi​ generate a copy of su(2)\mathfrak{su}(2)su(2) with [T1,T2]=T3[T_1,T_2]=T_3[T1​,T2​]=T3​ cyclically. The associated quadratic Casimir is the endomorphism

C  =  −(T12+T22+T32).C \;=\; -(T_1^2 + T_2^2 + T_3^2).C=−(T12​+T22​+T32​).

Because each EiE_iEi​ is even, every TiT_iTi​ preserves the odd sector, and so does CCC.

Formalization targets

Goal — the Casimir spectrum with exact multiplicities

C∣Cl−(6,0) has eigenvalue 2 with multiplicity 24 and eigenvalue 0 with multiplicity 8,C\big|_{\mathrm{Cl}^-(6,0)} \ \text{has eigenvalue } 2 \text{ with multiplicity } 24 \ \text{and eigenvalue } 0 \text{ with multiplicity } 8,C​Cl−(6,0)​ has eigenvalue 2 with multiplicity 24 and eigenvalue 0 with multiplicity 8,

the two eigenspaces spanning the whole odd sector. Equivalently, as a representation of the generated Spin(3)≅SU(2)\mathrm{Spin}(3) \cong \mathrm{SU}(2)Spin(3)≅SU(2),

Cl−(6,0)  ≅  8 Vj=1  ⊕  8 Vj=0,\mathrm{Cl}^-(6,0) \;\cong\; 8\,V_{j=1} \;\oplus\; 8\,V_{j=0},Cl−(6,0)≅8Vj=1​⊕8Vj=0​,

eight copies of the spin-1 module and eight copies of the trivial module. The goal deliberately asserts only the eigenspace dimensions and their spanning property — the decomposition shape — not any particular basis or pairing.

Stronger — the Cartan weight decomposition

T3-weights on Cl−(6,0):0 (multiplicity 16),+1 and −1 (multiplicity 8 each),T_3\text{-weights on } \mathrm{Cl}^-(6,0): \quad 0 \ \text{(multiplicity } 16\text{)}, \qquad +1 \ \text{and} \ -1 \ \text{(multiplicity } 8 \text{ each)},T3​-weights on Cl−(6,0):0 (multiplicity 16),+1 and −1 (multiplicity 8 each),

the three weight spaces spanning the sector. This refines the goal: each j=1j=1j=1 copy contributes weights −1,0,+1-1,0,+1−1,0,+1 and each j=0j=0j=0 copy contributes weight 000.

Significance

The result itself. The spectrum pins down exactly how an su(2)\mathfrak{su}(2)su(2) acting from inside the algebra sees the odd sector: not irreducibly, but as a clean 8⊕88 \oplus 88⊕8 multiplicity split between spin-1 and spin-0. In the LeanProofs program this decomposition is load-bearing for everything downstream that distinguishes "active" indices from "spectator" indices — the multiplicity 888 is the number of spectator degrees of freedom, and its appearance in the spectrum is what makes the split structural rather than coincidental. The weight decomposition further identifies the Cartan grading and is the natural first test case for any technology that must eventually handle larger Clifford algebras or other subalgebras.

Formalizing it. The computation is proved (structurally, by hand, in the research record) but not machine-checked. Everything needed lives in Mathlib: CliffordAlgebra, its Z2\mathbb{Z}_2Z2​ grading CliffordAlgebra.evenOdd, Submodule, LinearMap, Module.finrank. What the mission produces is a fully verified finite spectral computation inside Clifford algebra — a reusable certificate that the platform's Clifford and grading infrastructure supports exact representation-theoretic bookkeeping, not just algebraic identities.

Difficulty

The obstruction is bookkeeping, not ideas. The natural attack — split indices into active {0,2,5}\{0,2,5\}{0,2,5} and spectator {1,3,4}\{1,3,4\}{1,3,4}, decompose Cl(active)⊗Cl(spectator)\mathrm{Cl}(\text{active}) \otimes \mathrm{Cl}(\text{spectator})Cl(active)⊗Cl(spectator) as a tensor product of graded pieces, and read off the 8=238 = 2^38=23 multiplicity from the spectator sector — requires transferring the su(2)\mathfrak{su}(2)su(2) action across such a tensor decomposition, which Mathlib does not provide ready-made for Clifford algebras. A purely computational route (fix the 64-element blade basis, build the 32×3232 \times 3232×32 matrices of the TiT_iTi​ explicitly, compute kernels) is straightforwardly correct but laborious; making it readable is the real work. The statement is stated through arbitrary endomorphisms bound pointwise to the halved adjoint actions precisely so that solvers may choose either route.

Formalization scope

The mission commits to: the quadratic form Q60 as QuadraticMap.weightedSumSquares ℝ (fun _ : Fin 6 => 1); generators e6 i = CliffordAlgebra.ι Q60 (Pi.single i 1); the odd sector as the Mathlib-native CliffordAlgebra.evenOdd Q60 1; and the registered triple as products of two generators. All theorems quantify over endomorphism witnesses bound pointwise to 12 adEi\tfrac12\,\mathrm{ad}_{E_i}21​adEi​​, so no particular matrix realization is privileged. Spectra are stated as eigenspace decompositions with exact Module.finrank multiplicities — never as pointwise eigenvalue claims, which would be false for mixed vectors. No trivializing formalization exists: the multiplicities are hard constants, and the dimension gate (32) rules out statements about degenerate sector choices. The definition file is reusable for any future mission on Cl(6,0)\mathrm{Cl}(6,0)Cl(6,0); the su(2) relations and dimension gate are self-contained milestones. Contributions of either a structural (active/spectator split) or computational (explicit blade basis) proof are equally welcome.

Selected references

  • Lawson & Michelsohn, Spin Geometry, Princeton University Press, 1989 (Clifford algebra grading and structure).
  • MonumentalSystems, LeanProofs research record #2561 (2026): exact full-sector SU(2) decomposition of Cl−(6,0)\mathrm{Cl}^-(6,0)Cl−(6,0) with multiplicities, https://github.com/MonumentalSystems/LeanProofs
  • Mathlib, Mathlib.LinearAlgebra.CliffordAlgebra.Grading (the evenOdd grading used as the odd sector).
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Number Theory·Captain: Lucas

Grothendieck-Teichmüller: the graded Lie algebra grt_1 and the Deligne-Drinfeld-Ihara conjectureOpen Problem

Motivation

The Grothendieck-Teichmüller group organises a family of symmetries that act on braided monoidal categories, on quantised universal enveloping algebras, on the little-discs operad, and on the ring of periods of the projective line minus three points. Three versions exist: a profinite one GT^\widehat{GT}GT, introduced by Grothendieck and Drinfeld and containing the absolute Galois group Gal(Q‾/Q)\mathrm{Gal}(\overline{\mathbb Q}/\mathbb Q)Gal(Q​/Q); a pro-ℓ\ellℓ one; and a pro-unipotent one GTGTGT, together with its graded companion GRTGRTGRT. This mission is about the graded, pro-unipotent side, which is the version that governs the homological-algebra and deformation-quantisation applications, and which is closest to a concrete, computable object: a Lie algebra of Lie polynomials in two variables, cut out by three explicit equations.

Its Lie algebra grt1\mathfrak{grt}_1grt1​ carries a distinguished family of elements σ3,σ5,σ7,…\sigma_3, \sigma_5, \sigma_7, \dotsσ3​,σ5​,σ7​,…, one in each odd degree at least 333, produced from the Knizhnik-Zamolodchikov associator. Deligne, Drinfeld and Ihara conjectured that grt1\mathfrak{grt}_1grt1​ is the free Lie algebra on such a family. A timeline of what is actually known:

  • 1990 - V. Drinfeld, On quasitriangular quasi-Hopf algebras and a group closely connected with Gal(Q‾/Q)\mathrm{Gal}(\overline{\mathbb Q}/\mathbb Q)Gal(Q​/Q), introduces GTGTGT, GRTGRTGRT, associators, and the defining equations of grt1\mathfrak{grt}_1grt1​; the Knizhnik-Zamolodchikov associator shows the set of associators is non-empty, hence σ3,σ5,…\sigma_3, \sigma_5, \dotsσ3​,σ5​,… exist and are non-zero.
  • 2012 - F. Brown, Mixed Tate motives over Z\mathbb ZZ (Annals of Mathematics 175, 949-976, doi:10.4007/annals.2012.175.2.10), proves that the ζf(r1,…,rn)\zeta^{\mathfrak f}(r_1,\dots,r_n)ζf(r1​,…,rn​) with rj∈{2,3}r_j \in \{2,3\}rj​∈{2,3} form a basis of the algebra of motivic multiple zeta values. One half of the conjecture follows: the Lie subalgebra of grt1\mathfrak{grt}_1grt1​ generated by the σ2p+1\sigma_{2p+1}σ2p+1​ is free on them.
  • The converse half - that these elements generate all of grt1\mathfrak{grt}_1grt1​ - is open.

Setting

Let F(x,y)\mathbb{F}(x,y)F(x,y) be the free Lie algebra over Q\mathbb QQ on two generators xxx and yyy, graded by total word length. For a Lie algebra AAA over Q\mathbb QQ and a,b∈Aa, b \in Aa,b∈A, write ψ(a,b)\psi(a,b)ψ(a,b) for the image of ψ∈F(x,y)\psi \in \mathbb{F}(x,y)ψ∈F(x,y) under the unique Lie algebra morphism sending x↦ax \mapsto ax↦a and y↦by \mapsto by↦b.

For n≥1n \ge 1n≥1, the Drinfeld-Kohno Lie algebra tn\mathfrak t_ntn​ is generated over Q\mathbb QQ by symbols tijt_{ij}tij​, 1≤i,j≤n1 \le i, j \le n1≤i,j≤n, subject to

tii=0,tij=tji,[tij,tkl]=0,[tij,tik+tjk]=0,t_{ii} = 0, \qquad t_{ij} = t_{ji}, \qquad [t_{ij}, t_{kl}] = 0, \qquad [t_{ij}, t_{ik} + t_{jk}] = 0,tii​=0,tij​=tji​,[tij​,tkl​]=0,[tij​,tik​+tjk​]=0,

the third relation for i,j,k,li,j,k,li,j,k,l pairwise distinct and the fourth for i,j,ki,j,ki,j,k pairwise distinct. It is the Lie algebra of infinitesimal braid relations: the associated graded of the pure braid Lie algebra, and the coefficient algebra of the Knizhnik-Zamolodchikov connection.

The graded Grothendieck-Teichmüller Lie algebra grt1\mathfrak{grt}_1grt1​ is the set of ψ∈F(x,y)\psi \in \mathbb{F}(x,y)ψ∈F(x,y) satisfying three equations:

ψ(x,y)=−ψ(y,x),\psi(x,y) = -\psi(y,x),ψ(x,y)=−ψ(y,x), ψ(x,y)+ψ(y,z)+ψ(z,x)=0where x+y+z=0,\psi(x,y) + \psi(y,z) + \psi(z,x) = 0 \quad \text{where } x + y + z = 0,ψ(x,y)+ψ(y,z)+ψ(z,x)=0where x+y+z=0, ψ(t12,t23)−ψ(t12,t23+t24)+ψ(t12+t13,t24+t34)−ψ(t13+t23,t34)+ψ(t23,t34)=0  in t4.\psi(t_{12},t_{23}) - \psi(t_{12},t_{23}+t_{24}) + \psi(t_{12}+t_{13},t_{24}+t_{34}) - \psi(t_{13}+t_{23},t_{34}) + \psi(t_{23},t_{34}) = 0 \ \text{ in } \mathfrak t_4 .ψ(t12​,t23​)−ψ(t12​,t23​+t24​)+ψ(t12​+t13​,t24​+t34​)−ψ(t13​+t23​,t34​)+ψ(t23​,t34​)=0  in t4​.

All three are linear in ψ\psiψ and degree preserving, so grt1\mathfrak{grt}_1grt1​ is a graded Q\mathbb QQ-subspace.

grt1\mathfrak{grt}_1grt1​ is not closed under the bracket of F(x,y)\mathbb{F}(x,y)F(x,y); it is closed under the Ihara (Poisson) bracket

{f,g}=[f,g]+Dfg−Dgf,\{f,g\} = [f,g] + D_f g - D_g f,{f,g}=[f,g]+Df​g−Dg​f,

where DfD_fDf​ is the derivation of F(x,y)\mathbb{F}(x,y)F(x,y) determined by Dfx=0D_f x = 0Df​x=0 and Dfy=[y,f]D_f y = [y,f]Df​y=[y,f]. Writing Der\mathrm{Der}Der for the Lie algebra of derivations of F(x,y)\mathbb{F}(x,y)F(x,y) under the commutator, the assignment f↦Dff \mapsto D_ff↦Df​ satisfies [Df,Dg]=D{f,g}[D_f, D_g] = D_{\{f,g\}}[Df​,Dg​]=D{f,g}​, and it is injective on grt1\mathfrak{grt}_1grt1​; this is the form in which the Lie structure of grt1\mathfrak{grt}_1grt1​ is expressed in the formal statements below.

Finally, for n1≥2n_1 \ge 2n1​≥2 and n2,…,nk≥1n_2,\dots,n_k \ge 1n2​,…,nk​≥1 the multiple zeta value is

ζ(n1,…,nk)=∑j1>j2>⋯>jk≥11j1n1j2n2⋯jknk.\zeta(n_1,\dots,n_k) = \sum_{j_1 > j_2 > \cdots > j_k \ge 1} \frac{1}{j_1^{n_1} j_2^{n_2} \cdots j_k^{n_k}} .ζ(n1​,…,nk​)=j1​>j2​>⋯>jk​≥1∑​j1n1​​j2n2​​⋯jknk​​1​.

These numbers are the coefficients of the Knizhnik-Zamolodchikov associator, which is why they enter a mission about grt1\mathfrak{grt}_1grt1​; they satisfy the stuffle and shuffle relations, whose common refinement (the double shuffle relations) is the arithmetic side of the same story.

Formalization targets

Goal - Deligne-Drinfeld-Ihara

∃ σ0,σ1,σ2,⋯∈grt1,deg⁡σp=2p+3,such that grt1 is the free Lie algebra on (σp)p≥0 for { ,}.\exists\, \sigma_0, \sigma_1, \sigma_2, \dots \in \mathfrak{grt}_1, \quad \deg \sigma_p = 2p+3, \quad \text{such that } \mathfrak{grt}_1 \text{ is the free Lie algebra} \text{ on } (\sigma_p)_{p \ge 0} \text{ for } \{\,,\}.∃σ0​,σ1​,σ2​,⋯∈grt1​,degσp​=2p+3,such that grt1​ is the free Lie algebra on (σp​)p≥0​ for {,}.

Concretely: the Lie algebra morphism from the free Lie algebra on countably many generators to Der\mathrm{Der}Der sending the ppp-th generator to DσpD_{\sigma_p}Dσp​​ is injective, and its image is exactly D(grt1)D(\mathfrak{grt}_1)D(grt1​). The statement fixes the degrees of the generators but not the generators themselves, which is the weakest form that still carries the content of the conjecture.

Milestone level - Brown's half

The same family exists with the morphism merely injective: the σ2p+1\sigma_{2p+1}σ2p+1​ generate a free Lie subalgebra. This is a theorem (Brown 2012); the open part of the goal is surjectivity.

Supporting levels

The Ihara bracket is a Lie bracket; grt1\mathfrak{grt}_1grt1​ is closed under it; the degree-333 element [x+y,[x,y]][x+y,[x,y]][x+y,[x,y]] lies in grt1\mathfrak{grt}_1grt1​; every odd degree ≥3\ge 3≥3 contains a non-zero element of grt1\mathfrak{grt}_1grt1​; multiple zeta values satisfy the stuffle and shuffle relations; and ζ(2,1)=ζ(3)\zeta(2,1) = \zeta(3)ζ(2,1)=ζ(3).

Significance

A positive answer would determine grt1\mathfrak{grt}_1grt1​ completely and, through the GTGTGT-GRTGRTGRT-associator torsor, describe the pro-unipotent Grothendieck-Teichmüller group by generators without relations. Downstream it would pin down the homotopy automorphisms of the rationalised little-discs operad and the Lie algebra of the motivic Galois group of mixed Tate motives over Z\mathbb ZZ up to the same freeness statement. Without it, even the dimension of grt1\mathfrak{grt}_1grt1​ in a given degree is only known to be bounded above by the Broadhurst-Kreimer style count, with equality unproved.

Formalizing this mission produces a machine-checked definition of tn\mathfrak t_ntn​, grt1\mathfrak{grt}_1grt1​ and the Ihara bracket - objects that have no Mathlib counterpart at present - and machine-checked proofs of the Lie-theoretic facts around them. Brown's theorem itself is proved in the literature but not formalized; the goal statement is genuinely open, and no part of this mission is closed by an existing Lean development known to the proposal.

Difficulty

The obvious approach to the goal - exhibit the generators and count dimensions degree by degree - fails in both directions. Upwards, no closed formula for σ2p+1\sigma_{2p+1}σ2p+1​ is known: they are extracted from the Knizhnik-Zamolodchikov associator, whose coefficients are regularised iterated integrals, and only their leading coefficients are controlled. Downwards, freeness of the subalgebra they generate is not an algebraic manipulation of the three defining equations: Brown derives it from the motivic theory of multiple zeta values, where the missing input is a basis theorem for a period algebra, not an identity in F(x,y)\mathbb{F}(x,y)F(x,y). Even the milestone "grt1\mathfrak{grt}_1grt1​ is closed under the Ihara bracket" is not a formality: the pentagon equation lives in t4\mathfrak t_4t4​ and must be transported through substitutions into a quotient Lie algebra.

Formalization scope

The formalization commits to the following conventions, all visible in the definition files.

  1. The base field is Q\mathbb QQ. The source works over a field KKK of characteristic zero; every statement here is over Q\mathbb QQ.
  2. grt1\mathfrak{grt}_1grt1​ is modelled inside the free Lie algebra FreeLieAlgebra ℚ (Fin 2), i.e. by Lie polynomials, not the completed Lie algebra F^(x,y)\widehat{\mathbb{F}}(x,y)F(x,y) of the source. The three defining equations are homogeneous, so the graded object determines the completed one; solvers should be aware that no topology or completion appears anywhere.
  3. tn\mathfrak t_ntn​ is the quotient of the free Lie algebra on ordered pairs of indices in Fin n by the Lie ideal generated by the four relation families above, so dkGen i j is ti+1,j+1t_{i+1,j+1}ti+1,j+1​ under the shift Fin 4 = {0,1,2,3} versus indices 1,2,3,41,2,3,41,2,3,4.
  4. Homogeneity is expressed by the rescaling characterisation: ψ\psiψ has degree nnn if ψ(cx,cy)=cnψ(x,y)\psi(cx,cy) = c^n \psi(x,y)ψ(cx,cy)=cnψ(x,y) for all c∈Qc \in \mathbb Qc∈Q. Over an infinite field this is equivalent to homogeneity for the word-length grading.
  5. The Ihara derivation uses Dfx=0D_f x = 0Df​x=0. The source writes Dfx=xD_f x = xDf​x=x in Remark 4.4 and in Section 7.3, but that convention contradicts Lemma 7.2 of the same notes and the computation {x,y}=[x,y]+[y,x]=0\{x,y\} = [x,y] + [y,x] = 0{x,y}=[x,y]+[y,x]=0 in Remark 7.2; Dfx=0D_f x = 0Df​x=0 is the convention under which both hold, and is the standard one.
  6. The Lie structure on grt1\mathfrak{grt}_1grt1​ is carried by the injection f↦Dff \mapsto D_ff↦Df​ into LieDerivation ℚ (FreeLieAlgebra ℚ (Fin 2)) (FreeLieAlgebra ℚ (Fin 2)), so that freeness can be stated as injectivity of a morphism out of a free Lie algebra without first installing a new Lie algebra structure. Note f↦Dff \mapsto D_ff↦Df​ is injective on grt1\mathfrak{grt}_1grt1​ but not on all of F(x,y)\mathbb{F}(x,y)F(x,y), where Dy=0D_y = 0Dy​=0; a supporting item records the injectivity actually used.
  7. Multiple zeta values are real numbers defined by an iterated tsum; for non-admissible words the series diverges and the definition returns Mathlib's junk value. Every statement about them therefore carries an admissibility hypothesis: all letters ≥1\ge 1≥1 and first letter ≥2\ge 2≥2. The stuffle and shuffle products are multisets of words, so no free module on words is needed.
  8. Nothing here is vacuous by construction: the defining equations of grt1\mathfrak{grt}_1grt1​ are linear conditions on a non-zero graded space, t4≠0\mathfrak t_4 \ne 0t4​=0, and the milestone [x+y,[x,y]]∈grt1[x+y,[x,y]] \in \mathfrak{grt}_1[x+y,[x,y]]∈grt1​, [x+y,[x,y]]≠0[x+y,[x,y]] \ne 0[x+y,[x,y]]=0 exhibits a non-zero element.

Contributions welcome: the Lie-theoretic milestones (Lemma 7.2, Corollary 7.1, closure of grt1\mathfrak{grt}_1grt1​, the degree-333 element) are self-contained and need no motivic input; the multiple zeta milestones need summability infrastructure for iterated series; Brown's theorem and the goal need a substantial development that does not yet exist in Lean.

Selected references

  • V. G. Drinfeld, On quasitriangular quasi-Hopf algebras and a group closely connected with Gal(Q‾/Q)\mathrm{Gal}(\overline{\mathbb Q}/\mathbb Q)Gal(Q​/Q), Leningrad Math. J. 2 (1991), 829-860.
  • F. Brown, Mixed Tate motives over Z\mathbb ZZ, Annals of Mathematics 175 (2012), 949-976, doi:10.4007/annals.2012.175.2.10.
  • T. Willwacher, The Grothendieck-Teichmüller Group, ETH Zürich lecture notes, 27 February 2014 (the source text for this mission).
  • T. Willwacher, M. Kontsevich's graph complex and the Grothendieck-Teichmüller Lie algebra, Invent. Math. 200 (2015), 671-760, doi:10.1007/s00222-014-0528-x.
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Number TheoryRepresentation Theory·Captain: Lucas

Ngo's Fundamental Lemma II: Isogenies of Root Data and Paired GroupsResearch Paper

Motivation

Waldspurger's non-standard fundamental lemma is an identity between stable orbital integrals on the Lie algebras of two reductive groups that are not isomorphic, and not even isogenous as algebraic groups, but whose root data become identified after tensoring with Q\mathbb{Q}Q. The basic example is the pair (Sp2n,SO2n+1)(\mathrm{Sp}_{2n}, \mathrm{SO}_{2n+1})(Sp2n​,SO2n+1​), whose root systems CnC_nCn​ and BnB_nBn​ are exchanged by Langlands duality; the identity is what allows the twisted fundamental lemma to be deduced from the ordinary one. Waldspurger formulated the conjecture in L'endoscopie tordue n'est pas si tordue (2008); it is Theorem 1.12.7 of Bao Chau Ngo, Le lemme fondamental pour les algebres de Lie, Publ. Math. IHES 111 (2010), 1-169 (DOI), proved there in equal characteristic by the same Hitchin-fibration argument that gives the ordinary fundamental lemma.

Before any of that geometry can start, the two sides have to be compared: one needs a single Cartan subalgebra, a single Weyl group and a single space of characteristic polynomials serving both groups at once. Producing that comparison is a self-contained piece of linear algebra over the root data, carried out in Ngo's §1.12, and it is what this mission asks for.

Setting

Let G1G_1G1​ and G2G_2G2​ be split reductive groups over a field, pinned, with maximal tori T1T_1T1​ and T2T_2T2​. Each is determined by its root datum (X∗(Ti),X∗(Ti),Φi,Φi∨,Δi)(X^*(T_i), X_*(T_i), \Phi_i, \Phi_i^\vee, \Delta_i)(X∗(Ti​),X∗​(Ti​),Φi​,Φi∨​,Δi​), where Φi\Phi_iΦi​ is the set of roots, Φi∨\Phi_i^\veeΦi∨​ the set of coroots and Δi\Delta_iΔi​ the set of simple roots singled out by the pinning.

An isogeny of root data between G1G_1G1​ and G2G_2G2​ (Ngo, Definition 1.12.1) is a pair of isomorphisms of Q\mathbb{Q}Q-vector spaces

ψ∗:X∗(T2)⊗Q⟶X∗(T1)⊗Q,ψ∗:X∗(T1)⊗Q⟶X∗(T2)⊗Q\psi^* : X^*(T_2)\otimes\mathbb{Q} \longrightarrow X^*(T_1)\otimes\mathbb{Q}, \qquad \psi_* : X_*(T_1)\otimes\mathbb{Q} \longrightarrow X_*(T_2)\otimes\mathbb{Q}ψ∗:X∗(T2​)⊗Q⟶X∗(T1​)⊗Q,ψ∗​:X∗​(T1​)⊗Q⟶X∗​(T2​)⊗Q

which are transposes of one another, such that ψ∗\psi^*ψ∗ carries the set of lines Qα2\mathbb{Q}\alpha_2Qα2​ (α2∈Φ2\alpha_2 \in \Phi_2α2​∈Φ2​) bijectively onto the set of lines Qα1\mathbb{Q}\alpha_1Qα1​ (α1∈Φ1\alpha_1\in\Phi_1α1​∈Φ1​), matching lines of simple roots with lines of simple roots, and such that ψ∗\psi_*ψ∗​ has the same property for the lines spanned by coroots. Two semisimple groups with the same adjoint group are isogenous in this sense; so are a group and its Langlands dual, the interesting cases being Bn↔CnB_n \leftrightarrow C_nBn​↔Cn​, F4F_4F4​ and G2G_2G2​, where a short root α\alphaα is sent to αˇ\check\alphaαˇ and a long root to nαˇn\check\alphanαˇ with n=∣αlong∣2/∣αshort∣2n = |\alpha_{\mathrm{long}}|^2/|\alpha_{\mathrm{short}}|^2n=∣αlong​∣2/∣αshort​∣2. Groups obtained by twisting a pair of isogenous pinned groups by a common torsor are called paired.

A prime ppp is good with respect to ψ∗\psi^*ψ∗ when it divides neither of the indices

∣X∗(T1)/(X∗(T1)∩X∗(T2))∣and∣X∗(T2)/(X∗(T1)∩X∗(T2))∣,\bigl|X_*(T_1)/(X_*(T_1)\cap X_*(T_2))\bigr| \quad\text{and}\quad \bigl|X_*(T_2)/(X_*(T_1)\cap X_*(T_2))\bigr|,​X∗​(T1​)/(X∗​(T1​)∩X∗​(T2​))​and​X∗​(T2​)/(X∗​(T1​)∩X∗​(T2​))​,

the two lattices being compared inside the single Q\mathbb{Q}Q-vector space identified by ψ∗\psi_*ψ∗​.

Formalization targets

Goal (1.12.4 and 1.12.6): the Weyl groups are identified compatibly

ψ∗ w ψ∗−1∈W2for all w∈W1,and conversely,\psi_* \, w \, \psi_*^{-1} \in W_2 \quad \text{for all } w \in W_1, \qquad\text{and conversely,}ψ∗​wψ∗−1​∈W2​for all w∈W1​,and conversely,

i.e. conjugation by ψ∗\psi_*ψ∗​ carries the Weyl group W1W_1W1​ acting on X∗(T1)⊗QX_*(T_1)\otimes\mathbb{Q}X∗​(T1​)⊗Q onto the Weyl group W2W_2W2​ acting on X∗(T2)⊗QX_*(T_2)\otimes\mathbb{Q}X∗​(T2​)⊗Q. Ngo's reason is that the reflection attached to a root depends only on the line through that root, so the bijection of root lines transports reflections to reflections. This equivariance is what makes the induced isomorphism t1→t2\mathfrak{t}_1 \to \mathfrak{t}_2t1​→t2​ descend to an isomorphism ν:cG1→cG2\nu : \mathfrak{c}_{G_1} \to \mathfrak{c}_{G_2}ν:cG1​​→cG2​​ of the spaces of characteristic polynomials, which is Lemme 1.12.6 and which is what allows two points a1a_1a1​ and a2a_2a2​ with ν(a1)=a2\nu(a_1) = a_2ν(a1​)=a2​ to be compared at all.

Milestones

Two steps lead there: the reflection computation that makes a matched pair of root lines give a matched pair of reflections, and the integral statement behind Ngo's good-characteristic hypothesis — that when the two indices above are invertible in the base ring, the two lattices become identified after base change.

Significance

Theorem 1.12.7, the non-standard fundamental lemma, asserts that for two paired groups over Ov=k[[ϖ]]O_v = k[[\varpi]]Ov​=k[[ϖ]] with residue characteristic exceeding twice the Coxeter numbers, and for points a1a_1a1​ and a2a_2a2​ corresponding under ν\nuν, the stable orbital integrals of the characteristic functions of g1(Ov)\mathfrak{g}_1(O_v)g1​(Ov​) and g2(Ov)\mathfrak{g}_2(O_v)g2​(Ov​) agree. Waldspurger showed that this identity, together with the ordinary fundamental lemma, implies the twisted fundamental lemma. None of the objects in that statement — reductive group schemes over a discrete valuation ring, orbital integrals, Haar measures on the centralizer tori — exists in Mathlib today. The comparison of §1.12 does not need any of them: it is a statement about lattices, root systems and Weyl groups, and it is a strict prerequisite, since without the isomorphism ν\nuν the two sides of Theorem 1.12.7 cannot even be matched up.

Beyond this paper, the notion of an isogeny of root data and the good-characteristic base change of a pair of lattices are reusable: they are the standard bookkeeping behind Langlands duality for split groups, and neither is currently available.

Difficulty

The reflection step looks like a one-line computation and is one — but only once the two proportionality constants are known to agree. If ψ∗(α2)=c α1\psi^*(\alpha_2) = c\,\alpha_1ψ∗(α2​)=cα1​ and ψ∗(α1∨)=c′ α2∨\psi_*(\alpha_1^\vee) = c'\,\alpha_2^\veeψ∗​(α1∨​)=c′α2∨​, the conjugate of sα1s_{\alpha_1}sα1​​ is sα2s_{\alpha_2}sα2​​ exactly when c=c′c = c'c=c′, and that is forced by transposition together with ⟨α,α∨⟩=2\langle\alpha,\alpha^\vee\rangle = 2⟨α,α∨⟩=2. The genuine difficulty in the goal is different: the definition only says that ψ∗\psi^*ψ∗ and ψ∗\psi_*ψ∗​ permute lines, so one has to show that the bijection induced on root lines and the bijection induced on coroot lines are the same bijection. A solver who assumes this without proof has assumed the substance of 1.12.4.

The lattice milestone has its own trap: the quotient Λ1/(Λ1∩Λ2)\Lambda_1/(\Lambda_1\cap\Lambda_2)Λ1​/(Λ1​∩Λ2​) must be shown to have vanishing Tor\mathrm{Tor}Tor after base change, not merely to vanish, or the inclusion becomes only surjective.

Formalization scope

Root data are modelled by Mathlib's RootPairing ι ℚ M N, with MMM the character space, NNN the cocharacter space, and rational coefficients throughout, so that "tensoring with Q\mathbb{Q}Q" is built into the ambient objects rather than performed explicitly. A choice of simple roots is recorded as a subset of the index type rather than as a RootPairing.Base; nothing in the statements depends on that subset beyond its role in the definition of an isogeny. The Weyl group is the subgroup of linear automorphisms of the cocharacter space generated by the coreflections, which is the form in which it acts on the Cartan.

The goal is stated as a two-sided intertwining property rather than as an equality of subgroups: every element of W1W_1W1​ is intertwined by ψ∗\psi_*ψ∗​ with some element of W2W_2W2​ and conversely. This avoids introducing a conjugation homomorphism, and it is the form in which the statement is used. Both root pairings in the goal are required to be finite, reduced root systems, matching Ngo's hypothesis that G1G_1G1​ and G2G_2G2​ are reductive groups.

The good-characteristic condition is formalized exactly as Ngo writes it, by the invertibility in the base ring of the two indices, each expressed as the cardinality of an explicit quotient group; the conclusion is the bijectivity of the map induced on the tensor product by the inclusion of the intersection. If a quotient were infinite its cardinality is reported as 000, and invertibility of 000 then forces the base ring to be trivial, so no false statement hides in that corner.

No statement here is vacuous: any pair consisting of a root system and itself, with ψ∗\psi^*ψ∗ and ψ∗\psi_*ψ∗​ the identity, satisfies every hypothesis, and the pair (Bn,Cn)(B_n, C_n)(Bn​,Cn​) gives the intended non-trivial instances.

Selected references

  • Bao Chau Ngo, Le lemme fondamental pour les algebres de Lie, Publ. Math. IHES 111 (2010), 1-169. https://doi.org/10.1007/s10240-010-0026-7
  • J.-L. Waldspurger, L'endoscopie tordue n'est pas si tordue, Mem. Amer. Math. Soc. 908 (2008). https://doi.org/10.1090/memo/0908
  • J.-L. Waldspurger, Le lemme fondamental implique le transfert, Compositio Math. 105 (1997), 153-236. https://doi.org/10.1023/A:1000103112268
  • T. A. Springer, Reductive groups, in Automorphic Forms, Representations and L-functions, Proc. Sympos. Pure Math. 33 (1979), 3-27. https://doi.org/10.1090/pspum/033.1
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Liouville's theorem (differential algebra)Textbook

Motivation

Some elementary functions, such as e−x2e^{-x^2}e−x2, sin⁡(x)/x\sin(x)/xsin(x)/x and xxx^xxx, have antiderivatives that cannot be written as elementary functions. Liouville's theorem, formulated by Joseph Liouville between 1833 and 1841, is the algebraic statement that explains when an elementary antiderivative can exist: if a function has an elementary antiderivative at all, then that antiderivative lies in the differential field of the function, plus finitely many logarithms. The theorem underlies the Risch algorithm for symbolic integration, which relies on it to find any elementary antiderivative.

Setting

A differential field is a field FFF together with a derivation D:F→FD : F \to FD:F→F, i.e. an additive map satisfying D(ab)=a Db+b DaD(ab) = a\,Db + b\,DaD(ab)=aDb+bDa. Its constants form the subfield

Con⁡(F)={f∈F:Df=0}.\operatorname{Con}(F) = \{ f \in F : Df = 0 \}.Con(F)={f∈F:Df=0}.

Let G⊇FG \supseteq FG⊇F be a differential field extension (the derivation of GGG restricts to that of FFF).

  • GGG is a logarithmic extension of FFF if G=F(t)G = F(t)G=F(t) with ttt transcendental over FFF and Dt=Ds/sDt = Ds/sDt=Ds/s for some nonzero s∈Fs \in Fs∈F (so ttt behaves like log⁡s\log slogs).
  • GGG is an exponential extension of FFF if G=F(t)G = F(t)G=F(t) with ttt transcendental over FFF and Dt/t=DsDt/t = DsDt/t=Ds for some s∈Fs \in Fs∈F (so ttt behaves like ese^{s}es).
  • GGG is an elementary differential extension of FFF if there is a finite chain of subfields F=K0⊆K1⊆⋯⊆Km=GF = K_0 \subseteq K_1 \subseteq \cdots \subseteq K_m = GF=K0​⊆K1​⊆⋯⊆Km​=G in which every step Ki+1=Ki(ti)K_{i+1} = K_i(t_i)Ki+1​=Ki​(ti​) is algebraic, logarithmic or exponential.

The running example is C(x)\mathbb{C}(x)C(x), the field of rational functions in one variable with the standard derivative d/dxd/dxd/dx.

Formalization targets

Goal: Liouville's theorem

Let F⊆GF \subseteq GF⊆G be differential fields of characteristic zero with Con⁡(F)=Con⁡(G)\operatorname{Con}(F) = \operatorname{Con}(G)Con(F)=Con(G), and let GGG be an elementary differential extension of FFF. If f∈Ff \in Ff∈F and g∈Gg \in Gg∈G satisfy Dg=fDg = fDg=f, then there are n≥0n \ge 0n≥0, constants c1,…,cn∈Con⁡(F)c_1, \dots, c_n \in \operatorname{Con}(F)c1​,…,cn​∈Con(F) and nonzero f1,…,fn∈Ff_1, \dots, f_n \in Ff1​,…,fn​∈F, and s∈Fs \in Fs∈F with

f=c1Df1f1+⋯+cnDfnfn+Ds.f = c_1 \frac{Df_1}{f_1} + \cdots + c_n \frac{Df_n}{f_n} + Ds.f=c1​f1​Df1​​+⋯+cn​fn​Dfn​​+Ds.

Milestones from the article

  1. The constants Con⁡(F)\operatorname{Con}(F)Con(F) form a subfield of FFF.
  2. C(x)\mathbb{C}(x)C(x) carries a (unique) derivation extending the formal derivative of polynomials.
  3. Con⁡(C(x))=C\operatorname{Con}(\mathbb{C}(x)) = \mathbb{C}Con(C(x))=C.
  4. 1/x1/x1/x has no antiderivative in C(x)\mathbb{C}(x)C(x).
  5. The antiderivatives ln⁡x+C\ln x + Clnx+C of 1/x1/x1/x exist in the logarithmic extension C(x,ln⁡x)\mathbb{C}(x, \ln x)C(x,lnx).
  6. 1/(x2+1)1/(x^2+1)1/(x2+1) has no antiderivative in C(x)\mathbb{C}(x)C(x).
  7. 1x2+1=12i Duu\displaystyle \frac{1}{x^2+1} = \frac{1}{2i}\,\frac{Du}{u}x2+11​=2i1​uDu​ with u=1+ix1−ixu = \frac{1+ix}{1-ix}u=1−ix1+ix​, i.e. tan⁡−1x=12iln⁡1+ix1−ix\tan^{-1} x = \frac{1}{2i}\ln\frac{1+ix}{1-ix}tan−1x=2i1​ln1−ix1+ix​ has the form required by the theorem.

Significance

The theorem reduces the question of whether an integral is elementary to a question about the base differential field. That reduction is what makes decision procedures for integration in finite terms (the Risch algorithm) possible, and it is the standard route to proving that e−x2e^{-x^2}e−x2, sin⁡(x)/x\sin(x)/xsin(x)/x or xxx^xxx have no elementary antiderivative.

The result is classical and proved (Liouville; modern algebraic proof by Rosenlicht; textbook proof in Geddes–Czapor–Labahn, §12.4). Mathlib contains a formalization of the algebraic-extension part of the argument (IsLiouville, isLiouville_of_finiteDimensional in Mathlib/FieldTheory/Differential/Liouville.lean); the logarithmic and exponential steps and the full theorem for elementary extensions are the remaining work.

Difficulty

The algebraic steps can be handled by taking traces. The central difficulty is the transcendental steps: for a logarithmic or exponential generator ttt one must show, by comparing partial-fraction expansions in ttt and degrees in ttt, that an expression of the Liouville form over K(t)K(t)K(t) can be pushed down to one over KKK. This needs the hypothesis that no new constants appear. The induction must also track how constants and logarithmic derivatives behave along the whole chain.

Formalization scope

A differential field is a Mathlib Field with a Differential instance (a derivation over Z\mathbb{Z}Z, written a′a'a′); the extension F⊆GF \subseteq GF⊆G is an Algebra F G with DifferentialAlgebra F G, i.e. DDD commutes with the embedding. The chain of the elementary extension is a sequence of IntermediateField F G, starting at ⊥\bot⊥ and ending at ⊤\top⊤. Each step adjoins a single element, which is algebraic, logarithmic, or exponential over the previous field, and every derivative is computed in GGG. Characteristic zero is assumed (CharZero F). The article does not state it, but it is the standing convention of the theorem in its standard sources. Con⁡(F)=Con⁡(G)\operatorname{Con}(F) = \operatorname{Con}(G)Con(F)=Con(G) is stated as the equality of the image of Con⁡(F)\operatorname{Con}(F)Con(F) with Con⁡(G)\operatorname{Con}(G)Con(G). In the conclusion, the fif_ifi​ are required to be nonzero, so the quotients Dfi/fiDf_i/f_iDfi​/fi​ carry no division-by-zero junk.

For the C(x)\mathbb{C}(x)C(x) examples, C(x)\mathbb{C}(x)C(x) is Mathlib's RatFunc ℂ. Mathlib does not provide its derivative, so the examples take an arbitrary derivation satisfying IsStandardDerivation (it agrees with the formal derivative on polynomials). Milestone 2 asserts that exactly one such derivation exists, so the examples are not vacuous.

Selected references

  • J. Liouville, Premier / Second mémoire sur la détermination des intégrales dont la valeur est algébrique, J. École Polytechnique XIV (1833), 124–193.
  • M. Rosenlicht, Integration in finite terms, Amer. Math. Monthly 79 (1972), 963–972. https://doi.org/10.2307/2318066
  • K. O. Geddes, S. R. Czapor, G. Labahn, Algorithms for Computer Algebra, Kluwer, 1992, §12.4.
  • Wikipedia, Liouville's theorem (differential algebra), oldid 1349223559.
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Numerical Analysis·Captain: Lucas

Métodos Numéricos (Freitas) III: Sistemas Lineares e a Convergência de Gauss-SeidelTextbook

Motivation

Linear systems are the inner loop of scientific computing: discretized differential equations, least-squares fitting, network flow balances and equilibrium models all end in Ax=bAx = bAx=b. Direct elimination solves the system exactly in O(n3)O(n^3)O(n3) operations, but for the large sparse systems produced by discretization the cost and the round-off growth make iterative methods preferable: start from an arbitrary vector and apply a cheap update until the residual is small. The question such a method raises is when the iteration converges, and to that the chapter gives a clean sufficient answer: diagonal dominance.

This mission is the third in a series formalizing the lecture notes Métodos Numéricos by Sergio Roberto de Freitas (UFMS, 2000). It covers the iterative part of Chapter 5, Solução de Sistemas Lineares.

Setting

Let A=(aij)A = (a_{ij})A=(aij​) be a real ntimesnn \\times nntimesn matrix and binmathbbRnb \\in \\mathbb{R}^nbinmathbbRn. Assume aiineq0a_{ii} \\neq 0aii​neq0 for all iii.

The Jacobi method computes every coordinate of the new iterate from the old one:

xi(k+1)=frac1aiileft(bi−sumjneqiaijxj(k)right).x_i^{(k+1)} = \\frac{1}{a_{ii}}\\left(b_i - \\sum_{j \\neq i} a_{ij} x_j^{(k)}\\right).xi(k+1)​=frac1aii​left(bi​−sumjneqi​aij​xj(k)​right).

The Gauss-Seidel method updates the coordinates in order i=1,dots,ni = 1, \\dots, ni=1,dots,n and uses the values already updated in the same sweep:

xi(k+1)=frac1aiileft(bi−sumj<iaijxj(k+1)−sumj>iaijxj(k)right).x_i^{(k+1)} = \\frac{1}{a_{ii}}\\left(b_i - \\sum_{j < i} a_{ij}x_j^{(k+1)} - \\sum_{j > i} a_{ij}x_j^{(k)}\\right).xi(k+1)​=frac1aii​left(bi​−sumj<i​aij​xj(k+1)​−sumj>i​aij​xj(k)​right).

Both are instances of an affine iteration x(k+1)=Bx(k)+dx^{(k+1)} = Bx^{(k)} + dx(k+1)=Bx(k)+d associated with an equivalent rewriting Ax=biffx=Bx+dAx = b \\iff x = Bx + dAx=biffx=Bx+d.

The matrix AAA is diagonally dominant when each diagonal entry dominates its row:

∣aii∣>sumjneqi∣aij∣qquad(i=1,dots,n).|a_{ii}| > \\sum_{j \\neq i} |a_{ij}| \\qquad (i = 1, \\dots, n).∣aii​∣>sumjneqi​∣aij​∣qquad(i=1,dots,n).

Target

The goal theorem is Proposição 5.10.1: if AAA is diagonally dominant and x^\\star solves Ax^\\star = b, then the Gauss-Seidel iterates converge to x^\\star from any starting vector.

The milestones are the general facts the source uses to get there: that the limit of a convergent affine iteration is a fixed point of it and hence a solution of the system (Proposição 5.5.1), that a contraction condition lVertBvrVertleclVertvrVert\\lVert Bv \\rVert \\le c\\lVert v \\rVertlVertBvrVertleclVertvrVert with c<1c < 1c<1 forces convergence to the solution (Proposição 5.5.3), and that the Jacobi sweep has exactly the solutions of Ax=bAx = bAx=b as its fixed points (Proposição 5.5.2).

Significance

Diagonal dominance is the hypothesis a practitioner can check by inspection, and it is satisfied by the matrices that come from standard finite-difference stencils, from strictly diagonally dominant collocation systems and from many equilibrium models. The theorem says that for those systems Gauss-Seidel needs no spectral analysis and no preconditioner to be safe: convergence holds from any starting vector. The supporting milestones isolate the two halves of the argument — a fixed-point identification and a contraction estimate — in a form reusable for other splittings (Jacobi, SOR, block variants).

Mathlib has Banach's fixed point theorem and the theory of matrix norms, but not the Gauss-Seidel sweep, the notion of diagonal dominance as used here, or the convergence statement, which is what this mission adds.

Difficulty

Gauss-Seidel is not a plain affine map applied coordinatewise: within one sweep the coordinates are updated sequentially, so the new value of coordinate iii depends on the new values of coordinates j<ij < ij<i. Formalizing the sweep therefore requires a recursion over the coordinate index before the recursion over the iteration counter, and the contraction estimate has to be propagated along that inner recursion. The classical proof compares \\max_i |x_i^{(k+1)} - x_i^\\star| with \\max_i |x_i^{(k)} - x_i^\\star| and needs, for each iii, a bound that already uses the improved bounds for j<ij < ij<i; getting that induction right is the substance of the mission.

Formalization scope

Vectors are functions from a finite index type with nnn elements to mathbbR\\mathbb{R}mathbbR, and convergence is convergence in that finite product space (equivalently, coordinatewise). The Gauss-Seidel sweep is defined through an auxiliary partial sweep: after kkk inner steps the first kkk coordinates carry their new values and the remaining ones their old values, and the full sweep is the partial sweep after nnn steps. The Jacobi sweep is defined directly. Diagonal dominance is the strict inequality above, with the sum taken over the row with the diagonal index removed; for n=0n = 0n=0 every statement is vacuous, and the goal theorem is then trivially true because the space has a single point. Division by the diagonal entry is total division, so the definitions make sense even when aii=0a_{ii} = 0aii​=0; diagonal dominance rules that out, because the right-hand side of the dominance inequality is nonnegative. The goal theorem assumes a solution x^\\star is given rather than asserting its existence, and it asserts convergence for every starting vector, generalizing the source's choice x(0)=0x^{(0)} = 0x(0)=0. The contraction milestone states the consistency of the norms as the hypothesis lVertBvrVertleclVertvrVert\\lVert Bv \\rVert \\le c \\lVert v \\rVertlVertBvrVertleclVertvrVert in the supremum norm rather than fixing a particular matrix norm.

Selected references

  • S. R. Freitas, Métodos Numéricos, Departamento de Computação e Estatística, Universidade Federal de Mato Grosso do Sul, 2000. Chapter 5, Solução de Sistemas Lineares, pp. 85–118. (Course notes supplied with this mission.)
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Picard groups of semi-local or finite semiringsOpen Problem

Motivation

Invertible modules over a commutative semiring are Zariski-locally free, so local semirings have trivial Picard group. The source asks whether the ring-theoretic semilocal conclusion survives without subtraction: must every invertible module over a semiring with finitely many maximal ideals be free? If not, is the conclusion at least true for finite semirings?

This mission turns CUHK-Shenzhen AI Math Problem 19, Picard groups of semi-local or finite semirings, into an auditable Lean campaign. The objective is not merely to transcribe notation: it is to expose the mathematical model, the capstone, and a smaller attack surface as separate artifacts that other formalizers can inspect and reuse.

Setting

The main theorem asserts freeness for every invertible module over a commutative semiring with finite maximal spectrum. A separate milestone states the finite-semiring fallback. Both are positive formulations; a concrete counterexample to either resolves that target negatively and should motivate a corrected classification.

Significance

Solving this target would settle the precise finite or analytic core represented by the Lean statement and would create reusable infrastructure in semirings, Picard groups, invertible modules, finite semirings. Even a rigorous disproof is valuable: several entries in this collection deliberately ask whether an attractive extrapolation is true, and Lean forces a counterexample to satisfy every side condition. The mission therefore treats theorem proving and model criticism as equally legitimate research outcomes.

Difficulty

Ring proofs use subtraction-sensitive k-ideal properties and decompositions into local factors that can fail for semirings. Finite indecomposable semirings need not be local and may have positive Krull dimension. Invertible modules are projective with strong duality, but familiar rank and determinant arguments may not survive additive noncancellation.

Suggested attack route

Formalize the known local-freeness proof from the evaluation isomorphism and study patching over finitely many principal opens. Identify exactly where partitions of unity require k-ideals. For finite semirings, enumerate idempotent matrices representing projective modules, impose the invertibility constraints, and seek either a reduction to principal rank-one modules or a minimal counterexample. Product decompositions and faithful-action lemmas should be reusable.

Formalization scope

The Lean targets use Mathlib's commutative semiring, maximal spectrum, module, invertible-module, and free-module notions. 'Semilocal' is encoded only as finiteness of MaximalSpectrum; no unproved decomposition theorem is assumed. The finite fallback assumes the underlying semiring type is finite but does not assume the module itself finite separately. Cardinality-only variants from the source are not the capstone.

The natural-language source remains authoritative for motivation, while the Lean declaration is authoritative for what Prove2Me will verify. The mission description calls out restrictions where the current formal target is a finite-dimensional core, a fixed interpretation of informal terminology, or one sharpened subquestion from a broader classification problem. Those restrictions should not be silently generalized in a proof claim.

Milestones

Resolve the finite-semiring statement, computationally or structurally, while developing the local-to-semilocal patching lemmas needed by the main theorem.

The capstone is marked as the mission's main item and is never duplicated as a milestone. Definitions precede theorem statements in the proposal order. A milestone is considered complete only when its own exact statement is proved; proving a nearby theorem with stronger-looking prose but mismatched quantifiers, signs, supports, dimensions, or asymptotic constants does not complete it.

Timeline and literature status

The CUHK-Shenzhen AI Math Problems page added this problem on June 24, 2026. At the drafting date, August 31, 2026, the status and target corrections described above were checked against the source page and the cited primary material.

Acceptance criteria

A contribution may prove the displayed theorem or refute it by constructing data satisfying every Lean hypothesis while negating the conclusion. Informal changes of model do not count: any proposed correction must be submitted as a separately reviewed statement with an explanation of which source ambiguity or false implication it repairs. Definitions must remain computational or mathematically constrained; fields that simply assume the desired conclusion are not acceptable. Every proof must compile against the mission's pinned Mathlib revision, use no sorry, and expose a top-level theorem solution when submitted to Prove2Me.

The main theorem is intentionally separated from a smaller milestone. Contributors should preserve that dependency order, publish reusable lemmas rather than monolithic tactics, and report whether a lemma is analytic, algebraic, combinatorial, or infrastructure-only. Numerical evidence, external computer algebra, and exhaustive search are welcome for discovery, but a final certificate must be replayable by Lean. If an external result is invoked, its hypotheses must be represented in the formal statement or proved in the dependency tree.

Formal verification policy

The files were built locally with Lean 4.30.0 and Mathlib revision c5ea00351c28e24afc9f0f84379aa41082b1188f, the supported Prove2Me environment at drafting time. The mission definition file is ordered before all theorem files, and each theorem imports exactly that public definition module or Mathlib. Independent blind read-backs accompany the draft items so reviewers can compare what the Lean code literally says with this mathematical description. Human confirmation remains required before the public proposal can be submitted for moderation.

Selected references

  • Original problem
  • Facets of Module Theory over Semirings
  • MathOverflow discussion
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Captain: Henry Yuen

Fundamental Theorem of AlgebraTextbook

Show that every nonconstant complex polynomial has a complex root.

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Mathematical Physics·Captain: Lucas

Celestial w_{1+∞} wedge algebra and gluon S-algebra (Zhu review, §7.1)Research Paper

Motivation

In celestial holography, scattering amplitudes of massless particles in four-dimensional flat spacetime are rewritten, by a Mellin transform in the particle energies, as correlation functions of operators on the two-dimensional celestial sphere. Soft theorems then become Ward identities of two-dimensional currents. Guevara, Himwich, Pate and Strominger (arXiv:2103.03961) found that the conformally soft graviton modes obtained this way close under the collinear OPE into an infinite-dimensional algebra, and Strominger (arXiv:2105.14346) identified it, after a rescaling, with the wedge subalgebra of w1+∞w_{1+\infty}w1+∞​, the Lie algebra of polynomial area-preserving (Hamiltonian) vector fields on a two-plane. The review of B. Zhu (arXiv:2606.24285, Section 7.1) summarises this derivation, together with its gauge-theory counterpart, the gluon SSS-algebra, and the action of w1+∞w_{1+\infty}w1+∞​ on it. The review describes the celestial www-algebra as a consistency test for any proposed flat-space hologram.

Setting

The wedge range is the set of labels (p,m)(p,m)(p,m) with

p∈{1,32,2,52,… },1−p≤m≤p−1,p−1−m∈Z,p\in\{1,\tfrac32,2,\tfrac52,\dots\},\qquad 1-p\le m\le p-1,\qquad p-1-m\in\mathbb Z,p∈{1,23​,2,25​,…},1−p≤m≤p−1,p−1−m∈Z,

equivalently: p+m−1p+m-1p+m−1 and p−m−1p-m-1p−m−1 are both natural numbers. Let WWW be the complex vector space with basis {wmp}\{w^p_m\}{wmp​} indexed by the wedge range, and define a bilinear bracket on WWW by Eq. (7.8),

[wmp,wnq]=(m(q−1)−n(p−1)) wm+np+q−2,[w^p_m,w^q_n]=\bigl(m(q-1)-n(p-1)\bigr)\,w^{p+q-2}_{m+n},[wmp​,wnq​]=(m(q−1)−n(p−1))wm+np+q−2​,

where the right-hand side is 000 whenever (p+q−2,m+n)(p+q-2,m+n)(p+q−2,m+n) falls outside the wedge.

Eq. (7.9) realises wmpw^p_mwmp​ as the monomial up+m−1vp−m−1u^{p+m-1}v^{p-m-1}up+m−1vp−m−1 in the polynomial ring C[u,v]\mathbb C[u,v]C[u,v], equipped with the Poisson bracket {f,g}=∂uf ∂vg−∂vf ∂ug\{f,g\}=\partial_uf\,\partial_vg-\partial_vf\,\partial_ug{f,g}=∂u​f∂v​g−∂v​f∂u​g.

The conformally soft graviton modes HmkH^k_mHmk​ (k=2,1,0,−1,…k=2,1,0,-1,\dotsk=2,1,0,−1,…, k−22≤m≤2−k2\tfrac{k-2}{2}\le m\le\tfrac{2-k}{2}2k−2​≤m≤22−k​) obey the commutator (7.5) with factorial coefficients and the gravitational coupling κ\kappaκ. The rescaling (7.6), wmp=1κ(p−m−1)!(p+m−1)! Hm−2p+4w^p_m=\tfrac1\kappa(p-m-1)!(p+m-1)!\,H^{-2p+4}_mwmp​=κ1​(p−m−1)!(p+m−1)!Hm−2p+4​, turns (7.5) into (7.8).

On the gauge-theory side, with colour index aaa and Lie-algebra structure constants fabcf^{ab}{}_cfabc​, the conformally soft gluon modes Rnk,aR^{k,a}_nRnk,a​ obey (7.14). The rescaling (7.15), Smq,a=(q−m−1)!(q+m−1)! Rm3−2q,aS^{q,a}_m=(q-m-1)!(q+m-1)!\,R^{3-2q,a}_mSmq,a​=(q−m−1)!(q+m−1)!Rm3−2q,a​, gives the SSS-algebra (7.16), [Smp,a,Snq,b]=−ifabcSm+np+q−1,c[S^{p,a}_m,S^{q,b}_n]=-if^{ab}{}_cS^{p+q-1,c}_{m+n}[Smp,a​,Snq,b​]=−ifabc​Sm+np+q−1,c​. The wedge algebra acts on it by (7.17), [wmp,Snq,a]=(m(q−1)−n(p−1))Sm+np+q−2,a[w^p_m,S^{q,a}_n]=\bigl(m(q-1)-n(p-1)\bigr)S^{p+q-2,a}_{m+n}[wmp​,Snq,a​]=(m(q−1)−n(p−1))Sm+np+q−2,a​.

Formalization targets

Goal: (7.8) is a Lie bracket

[X,X]=0,[X,[Y,Z]]=[[X,Y],Z]+[Y,[X,Z]]for all X,Y,Z∈W.[X,X]=0,\qquad [X,[Y,Z]]=[[X,Y],Z]+[Y,[X,Z]]\qquad\text{for all }X,Y,Z\in W.[X,X]=0,[X,[Y,Z]]=[[X,Y],Z]+[Y,[X,Z]]for all X,Y,Z∈W.

Milestones

  1. Closure of the wedge (7.7)–(7.8): if (p,m)(p,m)(p,m) and (q,n)(q,n)(q,n) are in the wedge and m(q−1)−n(p−1)≠0m(q-1)-n(p-1)\ne0m(q−1)−n(p−1)=0, then (p+q−2,m+n)(p+q-2,m+n)(p+q−2,m+n) is in the wedge.
  2. Rescaling (7.5) ⇒\Rightarrow⇒ (7.8): any family HmkH^k_mHmk​ satisfying (7.5) in a complex vector space with a bilinear bracket, rescaled by (7.6), satisfies (7.8) (for κ≠0\kappa\neq 0κ=0).
  3. Poisson realisation on generators (7.9): {up+m−1vp−m−1,uq+n−1vq−n−1}=2(m(q−1)−n(p−1))up+q+m+n−3vp+q−m−n−3\{u^{p+m-1}v^{p-m-1},u^{q+n-1}v^{q-n-1}\}=2\bigl(m(q-1)-n(p-1)\bigr)u^{p+q+m+n-3}v^{p+q-m-n-3}{up+m−1vp−m−1,uq+n−1vq−n−1}=2(m(q−1)−n(p−1))up+q+m+n−3vp+q−m−n−3. The review's "convention-dependent overall factor" is pinned to 222.
  4. Poisson realisation, linear form (7.9): the linear map wmp↦up+m−1vp−m−1w^p_m\mapsto u^{p+m-1}v^{p-m-1}wmp​↦up+m−1vp−m−1 intertwines (7.8) with 12{⋅,⋅}\tfrac12\{\cdot,\cdot\}21​{⋅,⋅}.
  5. Gluon rescaling (7.14) ⇒\Rightarrow⇒ (7.16).
  6. The SSS-algebra is a Lie algebra (7.16), given that fabcf^{ab}{}_cfabc​ are Lie structure constants.
  7. SSS is a w1+∞w_{1+\infty}w1+∞​-module (7.17): [[X,Y],s]=[X,[Y,s]]−[Y,[X,s]][[X,Y],s]=[X,[Y,s]]-[Y,[X,s]][[X,Y],s]=[X,[Y,s]]−[Y,[X,s]].

Significance

The statements fix, in a machine-checked form, the precise normalisations used in the celestial literature: the wedge range, the rescalings (7.6) and (7.15), and the overall factor in the Poisson realisation, which the review leaves convention-dependent. They form the algebraic base layer for later formalisations of deformations of w1+∞w_{1+\infty}w1+∞​, its loop algebra Lw1+∞Lw_{1+\infty}Lw1+∞​, and the gluon–graviton soft algebras. The results themselves are established in the physics literature. The formal work that remains is the combinatorics of the factorial coefficients, the closure of the finite wedge range, and the Jacobi identities.

Difficulty

None of the statements is deep, but each carries bookkeeping that is easy to get wrong. The factorial coefficients of (7.5) and (7.14) must cancel exactly against the rescalings. At the corners of the wedge (m=p−1m=p-1m=p−1, n=q−1n=q-1n=q−1, or p+q−2<1p+q-2<1p+q−2<1) the target label leaves the wedge, and the structure constant must be shown to vanish there. The Jacobi identity for (7.8) does not follow term by term from the formula; the natural route is through the Poisson realisation, which must first be shown to be faithful.

Formalization scope

All objects are over C\mathbb CC. Labels p,m,q,n,k,lp,m,q,n,k,lp,m,q,n,k,l are rationals, and every label set is carved out by the predicate "p+m−1p+m-1p+m−1 and p−m−1p-m-1p−m−1 are natural numbers". Vector spaces with a given basis are finitely supported functions on the index set, and brackets are the bilinear extensions of the basis formulas. When the target label of a bracket falls outside the wedge, the bracket is defined to be 000 (milestone 1 shows this only happens when the structure constant already vanishes). Factorials of rational arguments are taken of the truncation ⌊⋅⌋+\lfloor\cdot\rfloor_+⌊⋅⌋+​ to a natural number; on the relevant ranges the arguments are natural numbers, and at the single corner where (7.5) has argument −1-1−1 its prefactor vanishes. The operator-level identities (milestones 2 and 5) are stated for an arbitrary complex vector space with an arbitrary bilinear bracket, taking (7.5) resp. (7.14) as hypotheses on the given modes. The colour algebra is given by structure constants f:ι3→Cf:\iota^3\to\mathbb Cf:ι3→C on a finite index set ι\iotaι, with antisymmetry and the Jacobi identity as the definition of Lie structure constants. The factor κ−1\kappa^{-1}κ−1 uses the convention 0−1=00^{-1}=00−1=0, and milestone 2 assumes κ≠0\kappa\ne0κ=0.

Selected references

  • B. Zhu, Topics in Celestial holography: A bottom-up perspective, invited review for Physics Reports, arXiv:2606.24285v3, 2026. https://arxiv.org/abs/2606.24285 (Section 7.1, Eqs. (7.1)–(7.17)).
  • A. Guevara, E. Himwich, M. Pate, A. Strominger, Holographic symmetry algebras for gauge theory and gravity, JHEP 2021. https://arxiv.org/abs/2103.03961
  • A. Strominger, w1+∞w_{1+\infty}w1+∞​ and the celestial sphere, Phys. Rev. Lett. 2021. https://arxiv.org/abs/2105.14346
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Complexity TheoryLinear algebraTheoretical Computer Science·Captain: mikedeng1

Most Tensor Problems Are NP-Hard 4: A Rational 2×2×2 Tensor Has Smaller Rank over the Reals Than over the RationalsResearch Paper

Motivation

The rank of a matrix does not depend on the field in which its entries are read: a rational matrix has the same rank over Q\mathbb QQ, R\mathbb RR and C\mathbb CC, because rank is computed by Gaussian elimination, which never leaves the field of the entries. For 3-tensors, arrays A=[ ⁣[aijk] ⁣]\mathcal A = [\![a_{ijk}]\!]A=[[aijk​]] with three indices, this fails. Tensor rank governs the complexity of bilinear maps (the exponent of matrix multiplication is a statement about the rank of one tensor), the uniqueness of the CANDECOMP/PARAFAC decompositions used in psychometrics and signal processing, and the identifiability of latent-variable models. In each application the field matters: algorithms are run over R\mathbb RR or C\mathbb CC, while complexity results are often proved over Q\mathbb QQ or finite fields.

Håstad (1990) proved that deciding rank⁡(A)≤r\operatorname{rank}(\mathcal A) \le rrank(A)≤r is NP-complete over finite fields and NP-hard over Q\mathbb QQ. De Silva and Lim (2008) gave real tensors whose rank over C\mathbb CC is strictly smaller than their rank over R\mathbb RR. Hillar and Lim (2013, Theorem 1.14) showed that the same phenomenon already occurs between Q\mathbb QQ and R\mathbb RR, for a 2×2×22\times2\times22×2×2 tensor with integer entries, so that Håstad's result over Q\mathbb QQ does not by itself say anything about rank over R\mathbb RR.

Setting

Let EEE be a field. The outer product of x∈El\mathbf x \in E^lx∈El, y∈Em\mathbf y \in E^my∈Em, z∈En\mathbf z \in E^nz∈En is the tensor x⊗y⊗z∈El×m×n\mathbf x\otimes\mathbf y\otimes\mathbf z \in E^{l\times m\times n}x⊗y⊗z∈El×m×n with entries xiyjzkx_iy_jz_kxi​yj​zk​. The rank of A\mathcal AA over EEE is

rank⁡E(A)=min⁡{r:A=∑s=1rλs xs⊗ys⊗zs,  λs∈E, xs∈El, ys∈Em, zs∈En}.\operatorname{rank}_E(\mathcal A) = \min\Big\{ r : \mathcal A = \sum_{s=1}^{r} \lambda_s\,\mathbf x_s\otimes\mathbf y_s\otimes\mathbf z_s,\ \ \lambda_s\in E,\ \mathbf x_s\in E^l,\ \mathbf y_s\in E^m,\ \mathbf z_s\in E^n\Big\}.rankE​(A)=min{r:A=s=1∑r​λs​xs​⊗ys​⊗zs​,  λs​∈E, xs​∈El, ys​∈Em, zs​∈En}.

If A\mathcal AA has entries in a subfield F⊆EF \subseteq EF⊆E, both rank⁡F(A)\operatorname{rank}_F(\mathcal A)rankF​(A) and rank⁡E(A)\operatorname{rank}_E(\mathcal A)rankE​(A) are defined, and rank⁡E(A)≤rank⁡F(A)\operatorname{rank}_E(\mathcal A) \le \operatorname{rank}_F(\mathcal A)rankE​(A)≤rankF​(A).

The paper's example uses x=[1,0]⊤\mathbf x = [1,0]^\topx=[1,0]⊤, y=[0,1]⊤\mathbf y = [0,1]^\topy=[0,1]⊤ and

A=2 x⊗x⊗x−4 y⊗y⊗x+4 y⊗x⊗y−4 x⊗y⊗y∈Q2×2×2.\mathcal A = 2\,\mathbf x\otimes\mathbf x\otimes\mathbf x - 4\,\mathbf y\otimes\mathbf y\otimes\mathbf x + 4\,\mathbf y\otimes\mathbf x\otimes\mathbf y - 4\,\mathbf x\otimes\mathbf y\otimes\mathbf y \in \mathbb Q^{2\times2\times2}.A=2x⊗x⊗x−4y⊗y⊗x+4y⊗x⊗y−4x⊗y⊗y∈Q2×2×2.

A decomposition A=u1⊗u2⊗u3+v1⊗v2⊗v3\mathcal A = \mathbf u_1\otimes\mathbf u_2\otimes\mathbf u_3 + \mathbf v_1\otimes\mathbf v_2\otimes\mathbf v_3A=u1​⊗u2​⊗u3​+v1​⊗v2​⊗v3​ with ui=[ai,bi]⊤\mathbf u_i = [a_i,b_i]^\topui​=[ai​,bi​]⊤, vi=[ci,di]⊤\mathbf v_i = [c_i,d_i]^\topvi​=[ci​,di​]⊤ is equivalent to the eight cubic equations (30) in the twelve unknowns a1,…,d3a_1,\dots,d_3a1​,…,d3​, one for each entry of A\mathcal AA.

In Lean, outer x y z and rankOver E A implement the two definitions, tensorA is A\mathcal AA, and System30 is (30).

Formalization targets

Goal: Theorem 1.14

∃ A∈Q2×2×2:rank⁡R(A)<rank⁡Q(A).\exists\, \mathcal A \in \mathbb Q^{2\times2\times2}:\quad \operatorname{rank}_{\mathbb R}(\mathcal A) < \operatorname{rank}_{\mathbb Q}(\mathcal A).∃A∈Q2×2×2:rankR​(A)<rankQ​(A).

Milestones (proof of Theorem 1.14, p. 0:26)

  1. With z=x+2 y\mathbf z = \mathbf x + \sqrt2\,\mathbf yz=x+2​y and zˉ=x−2 y\bar{\mathbf z} = \mathbf x - \sqrt2\,\mathbf yzˉ=x−2​y:
zˉ⊗z⊗zˉ+z⊗zˉ⊗z=A,so rank⁡R(A)≤2.\bar{\mathbf z}\otimes\mathbf z\otimes\bar{\mathbf z} + \mathbf z\otimes\bar{\mathbf z}\otimes\mathbf z = \mathcal A,\qquad\text{so } \operatorname{rank}_{\mathbb R}(\mathcal A)\le 2.zˉ⊗z⊗zˉ+z⊗zˉ⊗z=A,so rankR​(A)≤2.
  1. A tensor of rank at most 2 over a field is a sum of two outer products, and for A\mathcal AA the identity (29) A=u1⊗u2⊗u3+v1⊗v2⊗v3\mathcal A = \mathbf u_1\otimes\mathbf u_2\otimes\mathbf u_3 + \mathbf v_1\otimes\mathbf v_2\otimes\mathbf v_3A=u1​⊗u2​⊗u3​+v1​⊗v2​⊗v3​ holds exactly when the coordinates of ui,vi\mathbf u_i, \mathbf v_iui​,vi​ satisfy (30).
  2. Every solution of (30) in a field of characteristic zero satisfies 2c22−d22=02c_2^2 - d_2^2 = 02c22​−d22​=0 and c1d2d3+2=0c_1d_2d_3 + 2 = 0c1​d2​d3​+2=0.
  3. Lemma 8.1: (30) has no rational solution.
  4. rank⁡Q(A)>2\operatorname{rank}_{\mathbb Q}(\mathcal A) > 2rankQ​(A)>2.

Significance

The theorem shows that tensor rank, unlike matrix rank, is not invariant under field extension even between Q\mathbb QQ and R\mathbb RR, and even for the smallest nontrivial format 2×2×22\times2\times22×2×2. Its consequence for complexity is that a hardness result for rank over Q\mathbb QQ cannot be transferred to R\mathbb RR by reading the same instance in a larger field; the paper accordingly re-examines Håstad's construction to obtain hardness over R\mathbb RR and C\mathbb CC (Theorem 8.2), which is outside this mission.

The result is proved in the paper, with the decisive algebraic step delegated to a computer-algebra computation (Appendix). A machine-checked proof replaces that computation by a certificate verified in Lean, and it settles a printed error: one of the two consequences of (30) in the proof of Lemma 8.1 is printed with the wrong sign (see Formalization scope). No formalization of array tensor rank over a field, or of its field dependence, is known to exist in Mathlib or on this platform.

Difficulty

The upper bound is an identity among explicit 2×2×22\times2\times22×2×2 arrays. The lower bound is the substance: one must show that the cubic system (30), which has real solutions, has no rational one. Since (30) is solvable over R\mathbb RR, no argument by signs, inequalities or real geometry can work; the obstruction is arithmetic, coming from the irrationality of 2\sqrt22​. The step that fails in a naive attempt is the elimination: eliminating ten of the twelve unknowns from eight cubic equations by hand is impractical. A second, smaller difficulty is the reduction from "rank⁡Q(A)≤2\operatorname{rank}_{\mathbb Q}(\mathcal A) \le 2rankQ​(A)≤2" to two terms of the special form (29), which requires absorbing the scalars and padding a decomposition with fewer than two terms.

Formalization scope

  • Tensors are functions Fin l → Fin m → Fin n → E, with 0-based indices: the paper's aijka_{ijk}aijk​ is A (i-1) (j-1) (k-1). Vectors are Fin n → E.
  • rankOver E A is the sInf over N\mathbb NN of the lengths rrr of decompositions ∑sλs xs⊗ys⊗zs\sum_s \lambda_s\, \mathbf x_s\otimes\mathbf y_s\otimes\mathbf z_s∑s​λs​xs​⊗ys​⊗zs​. The set is nonempty (one term per entry), so this is the paper's minimum. Zero summands are allowed; this gives the same minimum as the paper's sum of nonzero rank-1 tensors.
  • rank⁡R\operatorname{rank}_{\mathbb R}rankR​ of a rational tensor is rankOver ℝ of its entrywise cast to R\mathbb RR; rank⁡Q\operatorname{rank}_{\mathbb Q}rankQ​ is rankOver ℚ, whose witnesses are rational. A formalization in which both ranks range over real witnesses would make the theorem false.
  • The goal is the printed existential. It is not a loophole: the milestones concern the paper's explicit tensor.
  • Readings of loose phrases: "Suppose not and that there exist ui,vi\mathbf u_i, \mathbf v_iui​,vi​ with (29). Identity (29) gives eight equations found in (30)" is split into a general statement (rank at most 2 over any field means a sum of two outer products) and the equivalence of (29) with (30) over every field of characteristic zero (milestone 2); both are stated in a generality in which their hypotheses can hold, because for A\mathcal AA over Q\mathbb QQ they cannot. "Polynomial consequences of (30)" is read as "holds at every solution of (30) in every field of characteristic zero" (milestone 3); over Q\mathbb QQ alone the statement would be vacuous, since (30) has no rational solution.
  • Corrected error. The paper prints the second consequence as c1d2d3−2=0c_1d_2d_3 - 2 = 0c1​d2​d3​−2=0. It is false: the real solution from milestone 1 has c1d2d3=−2c_1d_2d_3 = -2c1​d2​d3​=−2. The milestone states c1d2d3+2=0c_1d_2d_3 + 2 = 0c1​d2​d3​+2=0 (checked by a Gröbner basis computation over Q\mathbb QQ), which serves the paper's argument equally. The Appendix certificates GkG_kGk​, HkH_kHk​ (p. 0:34) are not used in any statement.
  • Out of scope: Theorem 1.15/8.2 (Håstad's construction over R\mathbb RR and C\mathbb CC) and the conjectures of §13.

Needed infrastructure: finite sums of arrays, Real.sqrt and irrational_sqrt_two, and an ideal-membership certificate for milestone 3. The array rank rankOver is reusable for any statement about tensor rank over a field. The platform's mme_tensor_rank (restriction-based rank of a TensorObj over a single field, from the matrix-multiplication exponent series) is a different object and is not reused. Proofs of any milestone, and alternative certificates for Lemma 8.1, are welcome.

Selected references

  • C. J. Hillar and L.-H. Lim, Most tensor problems are NP-hard, J. ACM 60(6), Art. 45, 2013. https://doi.org/10.1145/2512329 (arXiv: https://arxiv.org/abs/0911.1393)
  • J. Håstad, Tensor rank is NP-complete, J. Algorithms 11(4), 644–654, 1990. https://doi.org/10.1016/0196-6774(90)90014-6
  • V. de Silva and L.-H. Lim, Tensor rank and the ill-posedness of the best low-rank approximation problem, SIAM J. Matrix Anal. Appl. 30(3), 1084–1127, 2008. https://doi.org/10.1137/06066518X
  • F. L. Hitchcock, The expression of a tensor or a polyadic as a sum of products, J. Math. Phys. 6, 164–189, 1927. https://doi.org/10.1002/sapm192761164
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Mathematical Logic·Captain: marwahaha

Finite congruence lattices: characterization and undecidabilityOpen Problem

Motivation

A finite algebra has a lattice of congruences, ordered by inclusion. The source studies which finite lattices arise in this way, and the available goal captures its colored-graph characterization. The source is OpenAI's September 2026 manuscript.

Setting

A congruence is an equivalence relation preserved by every basic operation of an algebra. A graph witness assigns lattice-valued colors to pairs of finitely many vertices, with symmetry, diagonal, triangle, separation, and seed-connectivity conditions.

Formalization targets

Representable⁡(L)⟺HasGraphWitness⁡(L).\operatorname{Representable}(L)\quad\Longleftrightarrow\quad\operatorname{HasGraphWitness}(L).Representable(L)⟺HasGraphWitness(L).

For any finite type Lat carrying a lattice structure with a least element ⊥, Lat is Representable if and only if it HasGraphWitness. Representable means that there is a positive size n and an algebra on Fin n (a finite list of operations, each of some finite arity, acting on the carrier) such that Lat is order-isomorphic to the poset of congruences of that algebra, where a congruence is an equivalence relation compatible with every operation: if corresponding arguments are related coordinatewise, the outputs are related; congruences are ordered by the inherited order on equivalence relations. HasGraphWitness means that there is a positive size n and a Lat-valued coloring color of ordered pairs from Fin n satisfying five conditions: color is symmetric; color(a,b)=⊥ exactly when a=b; color(a,b) ≤ color(a,m) ⊔ color(m,b) for all a, b, m; whenever lower ≰ upper in Lat, some pair has color ≤ lower but not ≤ upper; and for every nonempty finite set of seed pairs, any pair whose color is at most the join of the seed colors is connected to the seeds. Connected is the equivalence closure of the relation Marked, where a,b are Marked if some self-map p of the vertices satisfies color(p x,p y) ≤ color(x,y) for all x,y and sends some seed pair (s,t) to (a,b).

The goal is OAI.FiniteCongruence.graph_criterion.

Significance

The equivalence provides a finite combinatorial certificate for representation as an entire congruence lattice. It is the characterization component of the manuscript. The manuscript presents a mathematical argument; the attached goal currently has status Open, so the requested contribution is a Lean proof of the displayed formal target.

Difficulty

Representing a lattice inside a congruence lattice is weaker than obtaining all congruences. The witness’s seed-connectivity condition must capture this fullness and work in both directions.

Formalization scope

The lattice is finite and has a least element. The algebra carrier and graph witness carrier each have positive finite size. Operations have finite arities, and representation is an order isomorphism. The manuscript’s undecidability conclusions are not among the attached targets.

The shared definitions are supplied by FiniteCongruenceGraph. The target uses Lean 4.33.1 with the pinned Mathlib environment. Contributions should preserve the existing statement and develop reusable supporting lemmas in its definitions.

Selected references

  • OpenAI, Finite congruence lattices: characterization and undecidability, preprint, September 2026. Manuscript.
  • OpenAI, accompanying Lean statement. Pinned source.
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Group Theory·Captain: marwahaha

A Counterexample to Kaplansky's Direct-Finiteness Conjecture in Odd CharacteristicOpen Problem

Motivation

The odd-characteristic version of direct finiteness has different coefficient constraints from the binary case. The source fixes one odd prime and links a group-algebra counterexample to a cellular automaton. The source is OpenAI's September 2026 manuscript.

Setting

For a finitely supported coefficient function bbb on a group, the cellular map sends a configuration x:G→Kx:G\to Kx:G→K to g↦∑ub(u)x(gu)g\mapsto\sum_u b(u)x(gu)g↦∑u​b(u)x(gu). The prime is the smallest prime factor of (m!)2+1(m!)^2+1(m!)2+1, where mmm is a fixed central binomial coefficient.

Formalization targets

p=min⁡PrimeDiv⁡ ⁣(((1200600)!)2+1),∣K∣=p4,ab=1≠ba,cellular⁡(b) injective and not surjective.p=\min\operatorname{PrimeDiv}\!\left((\binom{1200}{600}!)^2+1\right),\quad |K|=p^4,\quad ab=1\ne ba,\quad \operatorname{cellular}(b)\text{ injective and not surjective}.p=minPrimeDiv(((6001200​)!)2+1),∣K∣=p4,ab=1=ba,cellular(b) injective and not surjective.

The defined proposition MainClaim holds. Here sourceM is the central binomial coefficient C(1200,600), and sourcePrime is the smallest prime factor of (sourceM!)²+1. MainClaim asserts that this number p is prime and odd, and that there exist a finite field K of characteristic p with exactly p⁴ elements and a finitely generated group G containing a nontrivial element of finite order, together with two elements a and b of the group algebra K[G] such that ab = 1 but ba ≠ 1. Moreover, for the map cellular(b) sending x : G → K to g ↦ Σ_u b(u)·x(g·u), the sum running over the support of b, this map is injective but not surjective. The formal statement is admitted in the source rather than proved here.

The goal is OAI.OddKaplansky.main_theorem.

Significance

The conclusion combines a scalar one-sided inverse with failure of surjectivity of a finite-memory linear map. It specifies the characteristic and field size without claiming the construction works at every odd prime. The manuscript presents a mathematical argument; the attached goal currently has status Open, so the requested contribution is a Lean proof of the displayed formal target.

Difficulty

The group must retain nontrivial torsion while supporting the required finite sums. Matrix-level relations and an arbitrary choice of characteristic do not meet this target.

Formalization scope

The goal unfolds MainClaim. It proves primality and oddness of the fixed sourcePrime, then existentially supplies the finite field, finitely generated group, nontrivial finite-order element, and algebra elements. The cellular convention uses right-translated inputs gugugu.

The shared definitions are supplied by OddKaplansky. The target uses Lean 4.33.1 with the pinned Mathlib environment. Contributions should preserve the existing statement and develop reusable supporting lemmas in its definitions.

Selected references

  • OpenAI, A Counterexample to Kaplansky's Direct-Finiteness Conjecture in Odd Characteristic, preprint, September 2026. Manuscript.
  • OpenAI, accompanying Lean statement. Pinned source.
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Convex Optimization·Captain: marwahaha

A nonspectrahedral hyperbolicity coneOpen Problem

Motivation

Hyperbolic polynomials define convex optimization regions through real-rooted line restrictions. A spectrahedral representation would describe the same region by one finite symmetric positive-semidefinite matrix inequality. The source manuscript presents the surrounding research claim.

Setting

The formal ambient space consists of two real symmetric 4×4 matrices X,Z and a vector y∈ℝ³. A fixed determinant expression defines a multivariate polynomial p. At e=((I,I),0), the cone consists of x for which every complex root of t↦p(te−x) is real and nonnegative.

Formalization target

Prove dim(ambient)=23, p(e)=1, and

p is homogeneous of degree 20,deg⁡p=20,p\text{ is homogeneous of degree }20,\qquad\deg p=20,p is homogeneous of degree 20,degp=20,

with every line polynomial real-rooted. For every N>0 and linear symmetric pencil L, prove

cone⁡(p,e)≠{x:L(x)⪰0}.\operatorname{cone}(p,e)\ne\{x:L(x)\succeq0\}.cone(p,e)={x:L(x)⪰0}.

The selected formal target is OAI.Paper256.main_result.

Significance and status

The formal target rules out every finite homogeneous real symmetric pencil size. It also verifies the algebraic and root properties of its fixed polynomial. The published target is currently Open; the manuscript's argument and a checked Lean proof are separate deliverables.

Difficulty

Excluding one determinantal expression is weaker than excluding all matrix-inequality representations of the cone. The final universal quantifier ranges over all positive dimensions and all real linear pencils.

Formalization scope

The published Lean formula has asserted degree 20. The manuscript abstract describes degree 16; this draft follows the actual published degree-20 statement rather than substituting the manuscript number. Symmetric matrices use selfAdjoint, and positivity is Matrix.PosSemidef. No affine pencil or projected semidefinite lift is asserted here.

Selected references

  • OpenAI, A nonspectrahedral hyperbolicity cone, preprint, 2026. Pinned manuscript.
  • OpenAI, accompanying formal statements, commit adc7f1241b42. Goal source.
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Algebraic Geometry·Captain: marwahaha

An explicit noncoordinate polynomial with affine three-space zero fibreOpen Problem

Motivation

A hypersurface can be abstractly affine space without its defining equation being an ambient coordinate. Distinguishing these two properties is the embedding question behind the Abhyankar–Sathaye problem. The source manuscript presents the surrounding research claim.

Setting

For n ≥ 4, let R=ℂ[X₀,…,Xₙ₋₁]. A polynomial F is a coordinate if a ℂ-algebra automorphism of R sends some variable Xᵢ to F. Its zero fiber is represented by the quotient R/(F).

Formalization target

For every n ≥ 4, find F with

R/(F)≅CC[X0,…,Xn−2],F is not a coordinate.R/(F)\cong_{\mathbb C}\mathbb C[X_0,\ldots,X_{n-2}],\qquad F\text{ is not a coordinate}.R/(F)≅C​C[X0​,…,Xn−2​],F is not a coordinate.

The source supplies an explicit construction, while this selected goal asks for existence.

The selected formal target is OAI.AbhyankarSathaye.exists_noncoordinate_polynomial.

Significance and status

The target separates the intrinsic affine-space quotient from ambient polynomial equivalence in every dimension at least four. The published target is currently Open; the manuscript's argument and a checked Lean proof are separate deliverables.

Difficulty

An isomorphism of the quotient rings need not extend to an automorphism of the ambient ring. Both the quotient isomorphism and the failure of every possible coordinate automorphism must be established.

Formalization scope

The goal uses multivariate polynomials indexed by Fin n, a principal ideal, and ℂ-algebra equivalences. A separate published derivation target and its explicit polynomial definitions are retained as related references. That target concerns n−1 commuting locally nilpotent derivations, their common kernel and ordinary extra-variable partial derivatives; it is not asserted as a logical dependency of the existence goal.

Selected references

  • OpenAI, An explicit noncoordinate polynomial with affine three-space zero fibre, preprint, 2026. Pinned manuscript.
  • OpenAI, accompanying formal statements, commit adc7f1241b42. Goal source.
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Number Theory·Captain: marwahaha

The Deligne-Drinfeld conjectureOpen Problem

Motivation

Compatibility between reassociation and braiding imposes equations on formal Lie expressions. The question is whether those equations leave precisely the free family of odd-weight generators predicted by the Deligne–Drinfeld conjecture. The source manuscript presents the surrounding research claim.

Setting

Let L be the free Lie algebra over ℚ on x and y, each of weight one. The solution space W satisfies antisymmetry, the three-term relation, and the pentagon equation in the four-strand infinitesimal braid algebra. Its operation is the Ihara bracket {p,q}=Dₚq−D_qp+[p,q]. The free algebra F has generators indexed by k ≥ 0 with weights 2k+3.

Formalization target

Establish a graded bracket-preserving linear equivalence

F=Lie⁡Q⟨e3,e5,e7,…⟩  ≅  W,F=\operatorname{Lie}_{\mathbb Q}\langle e_3,e_5,e_7,\ldots\rangle\;\cong\;W,F=LieQ​⟨e3​,e5​,e7​,…⟩≅W,

together with mutually inverse continuous maps on the products of weight pieces. The completed maps must preserve the bracket degree by degree, including the finite convolution sum defining its weight-n component.

The selected formal target is OAI.DeligneDrinfeld.main.

Significance and status

The target simultaneously expresses freeness and exhaustion of the full equation space. Finding a free subalgebra alone leaves the exhaustion assertion unresolved. The published target is currently Open; the manuscript's argument and a checked Lean proof are separate deliverables.

Difficulty

The pentagon relation couples substitutions in the braid Lie algebra. Constructing odd-weight solutions does not by itself show that all solutions are generated by them, nor that the completed bracket has the required compatibility.

Formalization scope

The published definition block specifies the braid quotient, tangent construction of D, weighted Lie words, rational submodules and product completions. Generator k has weight 2k+3. The factor spaces carry the explicitly supplied discrete topology. The goal is exactly MainStatement, including its inverse, continuity and completed-bracket clauses. The available reference set supplies the definition block and one target, so no unsupported paper lemmas are attached as milestones.

Selected references

  • OpenAI, The Deligne-Drinfeld conjecture, preprint, 2026. Pinned manuscript.
  • OpenAI, accompanying formal statements, commit adc7f1241b42. Goal source.
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Algebraic GeometryRepresentation Theory·Captain: wurtle

Quadratic stabilization of the canonical Foulkes--Howe mapResearch Paper

Motivation: plethysm, Foulkes' conjecture and the canonical map

Plethysm — decomposing Sym⁡a(Sym⁡bV)\operatorname{Sym}^a(\operatorname{Sym}^b V)Syma(SymbV) into irreducible GL(V)\mathrm{GL}(V)GL(V)-representations — is one of the oldest open problems in the representation theory of the general linear group, and it is central to geometric complexity theory, where the coordinate rings of Chow varieties of products of linear forms control lower-bound arguments. Foulkes' conjecture (1950) predicts that for a≤ba\le ba≤b there is a GL(V)\mathrm{GL}(V)GL(V)-equivariant injection Sym⁡a(Sym⁡bV)↪Sym⁡b(Sym⁡aV)\operatorname{Sym}^a(\operatorname{Sym}^bV)\hookrightarrow\operatorname{Sym}^b(\operatorname{Sym}^aV)Syma(SymbV)↪Symb(SymaV). A natural candidate is supplied by a specific map, the canonical Foulkes–Howe map μa,b,V:Sym⁡b(Sym⁡aV)→Sym⁡a(Sym⁡bV)\mu_{a,b,V}:\operatorname{Sym}^b(\operatorname{Sym}^aV)\to\operatorname{Sym}^a(\operatorname{Sym}^bV)μa,b,V​:Symb(SymaV)→Syma(SymbV); its surjectivity yields such an embedding by complete reducibility. Its image is the degree-bbb part of the coordinate ring of the Chow variety of decomposable aaa-forms, so surjectivity for large bbb is a statement about that variety's normalization. The question is from which degree bbb on the map is surjective, uniformly in dim⁡V\dim VdimV.

Timeline

  • 1950 — Foulkes formulates the plethysm comparison (Foulkes, J. London Math. Soc. 1950).
  • 1993 — Brion proves eventual surjectivity of the canonical map for fixed aaa and VVV (Brion, Manuscripta Math. 1993); in 1997 he gives an effective bound depending on both aaa and dim⁡V\dim VdimV (Séminaires et Congrès 2, SMF, 1997, Theorem 3.3).
  • 2008 — McKay proves a propagation theorem for Foulkes-type injectivity (J. Algebra 2008); Ikenmeyer gives a weight-shift proof (arXiv:1509.04957, 2015).
  • 2015 — Landsberg's introduction to geometric complexity theory asks for a polynomial stabilization bound (Problem 7.19) (Ann. Univ. Ferrara 2015).
  • 2017 — Cheung, Ikenmeyer and Mkrtchyan show that the canonical map has nonzero kernel at (a,b)=(5,5)(a,b)=(5,5)(a,b)=(5,5) and (6,6)(6,6)(6,6) in suitable dimensions (J. Symbolic Comput. 2017).
  • 2022 — Raicu, Sam and Weyman bound the regularity of the Segre ring and modules of covariants on the Chow variety (Vietnam J. Math. 2022), without computing the top degree controlling stabilization.
  • 2026 — An OpenAI preprint, Quadratic stabilization of the canonical Foulkes–Howe map (OpenAI Math Release, September 25, 2026), claims surjectivity for all a≥2a\ge2a≥2, b≥a(a−1)b\ge a(a-1)b≥a(a−1) and every finite-dimensional VVV. The preprint has not been peer reviewed and its theorem is not formally verified.

Setting

Let VVV be a finite-dimensional complex vector space and Sym⁡V\operatorname{Sym}VSymV its symmetric algebra. Sym⁡nV⊆Sym⁡V\operatorname{Sym}^nV\subseteq\operatorname{Sym}VSymnV⊆SymV is the span of products v1⋯vnv_1\cdots v_nv1​⋯vn​ of nnn vectors. For vj,i∈Vv_{j,i}\in Vvj,i​∈V (1≤j≤b1\le j\le b1≤j≤b, 1≤i≤a1\le i\le a1≤i≤a), the canonical Foulkes–Howe map is the linear map determined by

μa,b,V(∏j=1b(vj,1⋯vj,a))=1(a!)b∑σ1,…,σb∈Sa ∏i=1a(∏j=1bvj,σj(i)),\mu_{a,b,V}\Bigl(\prod_{j=1}^{b}\bigl(v_{j,1}\cdots v_{j,a}\bigr)\Bigr) =\frac{1}{(a!)^{b}}\sum_{\sigma_1,\dots,\sigma_b\in S_a}\ \prod_{i=1}^{a}\Bigl(\prod_{j=1}^{b}v_{j,\sigma_j(i)}\Bigr),μa,b,V​(j=1∏b​(vj,1​⋯vj,a​))=(a!)b1​σ1​,…,σb​∈Sa​∑​ i=1∏a​(j=1∏b​vj,σj​(i)​),

where the outer products on the left and right are taken in Sym⁡(Sym⁡aV)\operatorname{Sym}(\operatorname{Sym}^aV)Sym(SymaV) and Sym⁡(Sym⁡bV)\operatorname{Sym}(\operatorname{Sym}^bV)Sym(SymbV) respectively. Equivalently: identify Sym⁡aW\operatorname{Sym}^aWSymaW with symmetric tensors via averaging, multiply bbb such tensors in (Sym⁡V)⊗a(\operatorname{Sym}V)^{\otimes a}(SymV)⊗a, and project back. That this formula is well defined on Sym⁡b(Sym⁡aV)\operatorname{Sym}^b(\operatorname{Sym}^aV)Symb(SymaV) is part of the content.

Formalization targets

Goal: quadratic stabilization (Theorem 1)

For every finite-dimensional complex VVV and integers a≥2a\ge2a≥2, b≥a(a−1)b\ge a(a-1)b≥a(a−1), there is a unique linear map

μ:Sym⁡b(Sym⁡aV)⟶Sym⁡a(Sym⁡bV)\mu:\operatorname{Sym}^b(\operatorname{Sym}^aV)\longrightarrow\operatorname{Sym}^a(\operatorname{Sym}^bV)μ:Symb(SymaV)⟶Syma(SymbV)

satisfying the displayed formula on monomials, and μ\muμ is surjective.

The bound a(a−1)a(a-1)a(a−1) is not claimed to be sharp; the content is a stabilization degree polynomial in aaa and independent of dim⁡V\dim VdimV. The goal statement is published on the platform with status Open: no machine-checked proof exists yet.

Significance

The result itself. Surjectivity gives, by complete reducibility, a GL(V)\mathrm{GL}(V)GL(V)-equivariant embedding Sym⁡a(Sym⁡bV)↪Sym⁡b(Sym⁡aV)\operatorname{Sym}^a(\operatorname{Sym}^bV)\hookrightarrow\operatorname{Sym}^b(\operatorname{Sym}^aV)Syma(SymbV)↪Symb(SymaV) for b≥a(a−1)b\ge a(a-1)b≥a(a−1) (Corollary 4 of the source), e.g. the sixth-power comparison for b≥30b\ge30b≥30. It answers positively the request for a polynomial bound in Landsberg's Problem 7.19, and it says that the coordinate ring of the Chow variety of decomposable aaa-forms agrees with its normalization in every degree b≥a(a−1)b\ge a(a-1)b≥a(a−1). Since the canonical map is known to fail to be injective at (5,5)(5,5)(5,5) and (6,6)(6,6)(6,6), an explicit range of surjectivity is the right kind of statement for this specific map.

Formalizing it. The statement is purely algebraic and uniform in VVV, aaa, bbb. A formal proof would need multilinear algebra over symmetric algebras (symmetric powers of symmetric powers), which is reusable for plethysm and invariant-theory projects.

Difficulty

Surjectivity is equivalent to the vanishing of every symmetric aaa-linear form on Sym⁡bV\operatorname{Sym}^bVSymbV whose diagonal vanishes on products of bbb vectors. The naive induction on aaa fails because the factors in different slots share a common product and cannot be varied independently; the dimension of VVV also grows the space of such forms without bound, so arguments using a fixed basis or dimension count do not give a uniform bound. Brion's effective bound depends on dim⁡V\dim VdimV, and regularity bounds for the normalization do not locate the top degree of the quotient that controls stabilization.

Formalization scope

  • Sym⁡nV\operatorname{Sym}^nVSymnV is represented as the submodule SymPow n V of Mathlib's SymmetricAlgebra ℂ V spanned by products of nnn vectors, and Sym⁡b(Sym⁡aV)\operatorname{Sym}^b(\operatorname{Sym}^aV)Symb(SymaV) is SymPow b (SymPow a V).
  • IsFoulkesMap a b V μ states the monomial formula above, with the normalizing factor (a!)−b(a!)^{-b}(a!)−b and the sum over bbb-tuples of permutations of Fin a.
  • The goal asserts existence, surjectivity and uniqueness of a linear map with this formula; uniqueness rules out choosing an arbitrary surjection, so the theorem is about the canonical map and not merely about dimensions.
  • VVV ranges over all finite-dimensional complex vector spaces in an arbitrary universe; a≥2a\ge2a≥2 and b≥a(a−1)b\ge a(a-1)b≥a(a−1) are natural numbers.
  • Needed infrastructure: symmetric powers inside the symmetric algebra, polarization/annihilator criteria, and directional-derivative operators on polynomial functions.

Selected references

  • H. O. Foulkes, Concomitants of the quintic and sextic up to degree four in the coefficients of the ground form, J. London Math. Soc. 25 (1950), 205–209. https://doi.org/10.1112/jlms/s1-25.3.205
  • M. Brion, Stable properties of plethysm: on two conjectures of Foulkes, Manuscripta Math. 80 (1993), 347–371. https://doi.org/10.1007/BF03026558
  • M. Brion, Sur certains modules gradués associés aux produits symétriques, Séminaires et Congrès 2, SMF, 1997, 157–183. https://smf.emath.fr/publications/sur-certains-modules-gradues-associes-aux-produits-symetriques
  • T. McKay, On plethysm conjectures of Stanley and Foulkes, J. Algebra 319 (2008), 2050–2071. https://doi.org/10.1016/j.jalgebra.2007.12.003
  • C. Ikenmeyer, On McKay's propagation theorem for the Foulkes conjecture, arXiv:1509.04957, 2015. https://arxiv.org/abs/1509.04957v1
  • J. M. Landsberg, Geometric complexity theory: an introduction for geometers, Ann. Univ. Ferrara 61 (2015), 65–117. https://doi.org/10.1007/s11565-014-0202-7
  • M.-W. Cheung, C. Ikenmeyer and S. Mkrtchyan, Symmetrizing tableaux and the 5th case of the Foulkes conjecture, J. Symbolic Comput. 80 (2017), 833–843. https://doi.org/10.1016/j.jsc.2016.09.002
  • C. Raicu, S. V. Sam and J. Weyman, On some modules supported in the Chow variety, Vietnam J. Math. 50 (2022), 501–521. https://doi.org/10.1007/s10013-021-00527-2
  • OpenAI, Quadratic stabilization of the canonical Foulkes–Howe map, OpenAI Math Release preprint, September 25, 2026 (source of the goal; Theorem 1, p. 1). https://github.com/openai/math/blob/adc7f1241b42e322a6451854ab7e4b4c146bf78a/preprints/Quadratic-Stabilization-of-the-Canonical-Foulkes-Howe-Map-September-25-2026/paper.pdf
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Algebraic TopologyGroup Theory·Captain: wurtle

A Torsion-Free Group Algebra with Zero DivisorsResearch Paper

Motivation: Kaplansky's zero-divisor conjecture

For a field KKK and a group GGG, the group algebra K[G]K[G]K[G] consists of finite formal sums ∑gagg\sum_g a_g g∑g​ag​g with ag∈Ka_g\in Kag​∈K, multiplied by extending the group law bilinearly. If g∈Gg\in Gg∈G has finite order m>1m>1m>1, then (1−g)(1+g+⋯+gm−1)=0(1-g)(1+g+\dots+g^{m-1})=0(1−g)(1+g+⋯+gm−1)=0, so K[G]K[G]K[G] has zero divisors. Kaplansky's zero-divisor conjecture asserts that this is the only source: if GGG is torsion-free, K[G]K[G]K[G] has no nonzero zero divisors. Together with the unit and idempotent conjectures it is one of the central problems connecting ring theory, group theory and topology, and positive answers are known for large classes of groups (elementary amenable groups, groups with the unique-product property, torsion-free 3-manifold groups).

Timeline

  • 1940 — Higman's thesis raises the question and proves the domain property for groups in which every nontrivial subgroup maps onto Z\mathbb ZZ (Higman, Proc. LMS 1940); the thesis formulation is reproduced by Sandling (1981).
  • 1956/1957 — Kaplansky poses the problem (Problem 6 in Problems in the theory of rings, National Research Council, 1957).
  • 1987 — Rips and Segev construct torsion-free groups without the unique-product property, removing the standard route to the conjecture (J. Algebra 1987); Steenbock gives a graphical small-cancellation treatment (J. Algebra 2015).
  • 1988 — Kropholler, Linnell and Moody prove the conjecture for torsion-free elementary amenable groups (Proc. AMS 1988).
  • 2021 — Gardam disproves the related unit conjecture over F2\mathbb F_2F2​ (Ann. of Math. 2021), and later over C\mathbb CC (arXiv:2312.05240, 2024). A nontrivial unit is not a zero divisor, so the zero-divisor conjecture remained open.
  • 2026 — Fisher and Sánchez-Peralta prove the domain conclusion for torsion-free 3-manifold groups and division-ring embeddings for virtually compact special groups (J. Comb. Algebra 2026).
  • 2026 — An OpenAI preprint, A Torsion-Free Group Algebra with Zero Divisors (OpenAI Math Release, September 23, 2026), claims a finitely presented torsion-free group GGG with a finite 2-dimensional classifying space such that F2[G]\mathbb F_2[G]F2​[G] has nonzero zero divisors. The preprint has not been peer reviewed and its theorem is not formally verified.

Setting

A group GGG is torsion-free if gn=1g^n=1gn=1 with n≥1n\ge1n≥1 implies g=1g=1g=1. It is finitely presented if it has a presentation with finitely many generators and relations. A classifying space (or K(G,1)K(G,1)K(G,1)) for GGG is a path-connected space XXX with π1(X)≅G\pi_1(X)\cong Gπ1​(X)≅G whose universal cover is contractible; it is finite two-dimensional if it is a finite CW complex with cells only in dimensions ≤2\le 2≤2. A group with a finite-dimensional classifying space is automatically torsion-free, but the formal goal asks for both properties explicitly.

The coefficient field is F2=Z/2\mathbb F_2=\mathbb Z/2F2​=Z/2, and F2[G]\mathbb F_2[G]F2​[G] is Mathlib's MonoidAlgebra (ZMod 2) G.

Formalization targets

Goal: a counterexample to the zero-divisor conjecture (Theorem 1.1)

There exist a group GGG and α,β∈F2[G]\alpha,\beta\in\mathbb F_2[G]α,β∈F2​[G] such that

G finitely presented,G torsion-free,G has a finite 2-dimensional K(G,1),α≠0, β≠0, αβ=0.G\ \text{finitely presented},\quad G\ \text{torsion-free},\quad G\ \text{has a finite 2-dimensional } K(G,1),\quad \alpha\neq0,\ \beta\neq0,\ \alpha\beta=0.G finitely presented,G torsion-free,G has a finite 2-dimensional K(G,1),α=0, β=0, αβ=0.

This is the full Theorem 1.1 of the source, including its "Moreover" clause. The source proves existence probabilistically; it does not exhibit a concrete presentation. The goal statement is published on the platform with status Open: no machine-checked proof exists yet.

Significance

The result itself. If correct, the theorem disproves Kaplansky's zero-divisor conjecture over F2\mathbb F_2F2​, a problem open since the 1940s, and shows that torsion-freeness — even together with finite presentability and a 2-dimensional classifying space — does not force K[G]K[G]K[G] to be a domain. It implies that GGG fails the unique-product property, and it bears on the implications among the Kaplansky conjectures (zero divisors, units, idempotents) and on approaches through the Atiyah conjecture and division-ring embeddings.

Formalizing it. The claim refutes a long-standing conjecture by an intricate probabilistic and topological construction, which is a strong case for machine verification. A full formal proof needs the probabilistic existence argument, planar separation, and asphericity of a 2-complex — none of which is a routine Mathlib application. Partial contributions (e.g. the characteristic-2 cancellation argument once asphericity and root separation are assumed, or the torsion-freeness of groups with finite-dimensional K(G,1)K(G,1)K(G,1)) are welcome. A related machine-checked result exists only for the weaker non-unique-product property of Gardam's A~2\widetilde A_2A2​ lattice (Mian–Siddique 2026).

Difficulty

Writing down α,β\alpha,\betaα,β whose product cancels in characteristic two is the easy part; the source does this by a parity argument on a graph of simultaneous steps. The hard part is two safeguards in the quotient group: both factors must remain nonzero (no vertex label other than the root can collapse to the identity), and the group must be torsion-free, which the source obtains by proving the 2-complex is aspherical. Standard tools — small-cancellation or CAT(0) criteria — are not applied; instead the source must exclude spherical arrangements of arbitrarily many paths of arbitrary length, which a union bound over sizes cannot handle.

Formalization scope

  • TorsionFree G is the plain group-theoretic notion (gn=1g^n=1gn=1, n>0n>0n>0 implies g=1g=1g=1); finite presentability is Group.IsFinitelyPresented.
  • HasFiniteTwoDimensionalClassifyingSpace G asks for a Hausdorff, path-connected space XXX with a finite CW structure on all of XXX, no cells above dimension 222, at least one 222-cell, a group isomorphism G≃π1(X,x)G\simeq\pi_1(X,x)G≃π1​(X,x), and a surjective covering map from a contractible space onto XXX (so XXX is aspherical). Requiring a 222-cell excludes only the case of free groups, whose group algebras are domains.
  • The witnessing group lives in Type and is existentially quantified together with its group structure; the zero divisors are elements of MonoidAlgebra (ZMod 2) G.
  • A trivializing reading is excluded because all three group properties and both nonvanishing conditions are required simultaneously.
  • Infrastructure needed: CW complexes and covering spaces (partially in Mathlib), the fundamental group of a 2-complex built by attaching cones, Hurewicz/Whitehead-type asphericity arguments, and random graph constructions.

Selected references

  • G. Higman, The units of group-rings, Proc. London Math. Soc. (2) 46 (1940). https://doi.org/10.1112/plms/s2-46.1.231
  • I. Kaplansky, Problems in the theory of rings, Report of a Conference on Linear Algebras (1956), National Research Council, 1957.
  • E. Rips and Y. Segev, Torsion-free group without unique product property, J. Algebra (1987). https://doi.org/10.1016/0021-8693(87)90125-6
  • P. H. Kropholler, P. A. Linnell and J. A. Moody, Applications of a new K-theoretic theorem to soluble group rings, Proc. Amer. Math. Soc. (1988). https://doi.org/10.2307/2046771
  • M. Steenbock, Rips–Segev torsion-free groups without the unique product property, J. Algebra (2015). https://doi.org/10.1016/j.jalgebra.2015.05.004
  • G. Gardam, A counterexample to the unit conjecture for group rings, Ann. of Math. 194 (2021). https://doi.org/10.4007/annals.2021.194.3.9
  • G. Gardam, Non-trivial units of complex group rings, preprint, 2024. https://arxiv.org/abs/2312.05240v2
  • S. P. Fisher and P. Sánchez-Peralta, Division rings for group algebras of virtually compact special groups and 3-manifold groups, J. Comb. Algebra (2026). https://doi.org/10.4171/JCA/89
  • I. Mian and S. Siddique, A machine-checked proof that Gardam's A~2\widetilde A_2A2​ lattice does not have unique products, preprint, 2026. https://arxiv.org/abs/2609.22380v1
  • OpenAI, A Torsion-Free Group Algebra with Zero Divisors, OpenAI Math Release preprint, September 23, 2026 (source of the goal; Theorem 1.1, p. 1). https://github.com/openai/math/blob/adc7f1241b42e322a6451854ab7e4b4c146bf78a/preprints/A-Torsion-Free-Group-Algebra-with-Zero-Divisors-September-23-2026/paper.pdf
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Algebraic Geometry·Captain: wurtle

An explicit failure of complex affine-space cancellationResearch Paper

Motivation

Zariski's cancellation problem asks whether affine space can be recognized from its cylinder: if a variety XXX satisfies X×A1≅An+1X\times\mathbb A^1\cong\mathbb A^{n+1}X×A1≅An+1, must X≅AnX\cong\mathbb A^nX≅An? Algebraically, for a finitely generated commutative C\mathbb CC-algebra AAA and an independent variable www,

A[w]≅C[n+1] ⟹? A≅C[n],A[w]\cong\mathbb C^{[n+1]}\ \overset{?}{\Longrightarrow}\ A\cong\mathbb C^{[n]},A[w]≅C[n+1] ⟹?​ A≅C[n],

where C[r]\mathbb C^{[r]}C[r] is a polynomial ring in rrr variables and all isomorphisms are C\mathbb CC-algebra isomorphisms. The problem is one of the central questions of affine algebraic geometry, closely tied to the recognition of affine space, coordinates of polynomial rings, and polynomial fibrations.

Background

  • 1972. Abhyankar, Heinzer and Eakin prove cancellation for the affine line (doi:10.1016/0021-8693(72)90134-2).
  • 1974. Dolgachev and Weisfeiler formulate the affine-fibration conjecture (doi:10.1070/IM1974v008n04ABEH002127).
  • 1979–1980. Fujita, and Miyanishi and Sugie, prove cancellation for the complex affine plane (doi:10.3792/pjaa.55.106, doi:10.1215/kjm/1250522319).
  • 1987. Asanuma constructs, in positive characteristic, threefolds whose cylinders are affine four-space (doi:10.1007/BF01389155).
  • 1996. Makar-Limanov uses additive group actions to show that the Russell cubic is not C3\mathbb C^3C3 (doi:10.1007/BF02937314).
  • 2014. Gupta proves failure of cancellation in every dimension ≥3\ge3≥3 over every field of positive characteristic (doi:10.1007/s00222-013-0455-2, doi:10.1016/j.aim.2014.07.012).
  • 2018–2021. El Kahoui–Ouali and Dutta–Lahiri prove that residual coordinates are one-stably coordinates (doi:10.1216/JCA-2018-10-3-317, doi:10.1016/j.jpaa.2021.106707).
  • 2026. Gaifullin and Petrov still list the characteristic-zero problem in dimension ≥3\ge3≥3 as unresolved (arXiv:2607.13593).

The source of this mission is an OpenAI preprint dated September 23, 2026.

Setting

Let p,s,u,F,Jp,s,u,F,Jp,s,u,F,J be independent variables over C\mathbb CC and P=C[p,s,u,F,J]P=\mathbb C[p,s,u,F,J]P=C[p,s,u,F,J]. Put

x=s2+u3+p2F,H=x2F−(1+2sx)J−p2J2−pu,A=P/(H).x=s^2+u^3+p^2F,\qquad H=x^2F-(1+2sx)J-p^2J^2-pu,\qquad A=P/(H).x=s2+u3+p2F,H=x2F−(1+2sx)J−p2J2−pu,A=P/(H).

So AAA is the coordinate ring of the hypersurface {H=0}⊂A5\{H=0\}\subset\mathbb A^5{H=0}⊂A5. For a C\mathbb CC-algebra AAA, A[w]A[w]A[w] denotes the polynomial ring in one further variable, and C[r]\mathbb C^{[r]}C[r] the polynomial ring in rrr variables.

Formalization targets

Goal: Theorem 1.1

A is a finitely generated integral domain of Krull dimension 4,A[w]≅CC[5],A̸≅CC[4].A\ \text{is a finitely generated integral domain of Krull dimension }4,\qquad A[w]\cong_{\mathbb C}\mathbb C^{[5]},\qquad A\not\cong_{\mathbb C}\mathbb C^{[4]}.A is a finitely generated integral domain of Krull dimension 4,A[w]≅C​C[5],A≅C​C[4].

The Lean statement OAI.ComplexCancellation.main is open on the platform.

Significance

Theorem 1.1 gives a negative answer to Zariski's cancellation problem over C\mathbb CC in dimension four, with an explicit counterexample of degree small enough to write in one line. The same polynomial yields two further consequences proved in the paper: HHH is a coordinate of P[w]P[w]P[w] but not of PPP, so the Stable Coordinate Conjecture fails in ambient dimension five (Corollary 1.2); and the maps p:Spec⁡A→A1p:\operatorname{Spec}A\to\mathbb A^1p:SpecA→A1 and (p,H):A5→A2(p,H):\mathbb A^5\to\mathbb A^2(p,H):A5→A2 are smooth A3\mathbb A^3A3-fibrations that are not Zariski-locally trivial, disproving the Dolgachev–Weisfeiler conjecture over these bases (Corollary 7.1). Cancellation in dimension three over C\mathbb CC is not addressed.

The result is proved in an OpenAI preprint, which has not been peer reviewed. No machine-checked proof exists.

Difficulty

The cylinder isomorphism A[w]≅C[5]A[w]\cong\mathbb C^{[5]}A[w]≅C[5] is comparatively explicit: a locally nilpotent derivation sends HHH to p3p^3p3, and exponentiating converts HHH into H+p3wH+p^3wH+p3w. The hard part is proving A≇C[4]A\not\cong\mathbb C^{[4]}A≅C[4]. Standard invariants do not help: AAA is smooth, factorial-type obstructions vanish, and topologically Spec⁡A\operatorname{Spec}ASpecA is contractible like C4\mathbb C^4C4 since its cylinder is C5\mathbb C^5C5. The paper uses additive group actions (locally nilpotent derivations), passing to an associated graded algebra along p=0p=0p=0, lifting actions through a line bundle over a smooth affine quadric, and a rigidity argument based on the Mason–Stothers polynomial abc inequality.

Formalization scope

  • P := MvPolynomial (Fin 5) ℂ with p, s, u, F, J := X 0, …, X 4; x and H are transcribed literally; A := P ⧸ Ideal.span {H}.
  • Dimension is ringKrullDim A = 4; integrality is IsDomain A; finite generation is Algebra.FiniteType ℂ A.
  • The cylinder statement is Nonempty (Polynomial A ≃ₐ[ℂ] MvPolynomial (Fin 5) ℂ); the non-polynomiality is ¬ Nonempty (A ≃ₐ[ℂ] MvPolynomial (Fin 4) ℂ). All isomorphisms are C\mathbb CC-algebra isomorphisms.

A complete development needs: explicit polynomial automorphisms (for the cylinder), Krull dimension of hypersurface quotients, locally nilpotent derivations and their kernels, filtrations and associated graded rings, and the Mason–Stothers theorem for polynomials. Contributions formalizing Proposition 2.2, Proposition 3.4 (the graded identification), Propositions 4.1–4.3, Lemma 5.1 (order of a locally nilpotent derivation), Lemma 6.1 (Mason–Stothers) and Proposition 6.3 are welcome.

Selected references

  • OpenAI, An explicit failure of complex affine-space cancellation, preprint, September 23, 2026. https://github.com/openai/math/blob/adc7f1241b42e322a6451854ab7e4b4c146bf78a/preprints/An-explicit-failure-of-complex-affine-space-cancellation-September-23-2026/paper.pdf
  • N. Gupta, On Zariski's cancellation problem in positive characteristic, Adv. Math., 2014. https://doi.org/10.1016/j.aim.2014.07.012
  • N. Gupta, On the cancellation problem for the affine space A3\mathbb A^3A3 in characteristic ppp, Invent. Math., 2014. https://doi.org/10.1007/s00222-013-0455-2
  • S. S. Abhyankar, W. Heinzer, P. Eakin, On the uniqueness of the coefficient ring in a polynomial ring, J. Algebra, 1972. https://doi.org/10.1016/0021-8693(72)90134-2
  • T. Fujita, On Zariski problem, Proc. Japan Acad. Ser. A, 1979. https://doi.org/10.3792/pjaa.55.106
  • L. Makar-Limanov, On the hypersurface x+x2y+z2+t3=0x+x^2y+z^2+t^3=0x+x2y+z2+t3=0 in C4\mathbb C^4C4 or a C3\mathbb C^3C3-like threefold which is not C3\mathbb C^3C3, Israel J. Math., 1996. https://doi.org/10.1007/BF02937314
  • A. K. Dutta, A. Lahiri, On residual and stable coordinates, J. Pure Appl. Algebra, 2021. https://doi.org/10.1016/j.jpaa.2021.106707
  • M. El Kahoui, M. Ouali, A note on residual coordinates of polynomial rings, J. Commut. Algebra, 2018. https://doi.org/10.1216/JCA-2018-10-3-317
  • B. Yu. Weisfeiler, I. V. Dolgachev, Unipotent group schemes over integral rings, Math. USSR-Izv., 1974. https://doi.org/10.1070/IM1974v008n04ABEH002127
  • S. Gaifullin, M. Petrov, Non-cancellative varieties, maximal tori, and the Makar-Limanov invariant, preprint, 2026. https://arxiv.org/abs/2607.13593
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CombinatoricsInformation TheoryTheoretical Computer Science·Captain: mikedeng1

Fuzzy Extractors: How to Generate Strong Keys from Biometrics and Other Noisy Data 2: The Improved Juels–Sudan Sketch Is an Average-Case Secure Sketch for s-Element Sets with Entropy Loss t log nResearch Paper

Motivation

Many security-relevant inputs are noisy and do not repeat exactly: fingerprint minutiae, iris codes, lists of personal preferences, the set of features extracted from a document. A cryptographic key derived from such an input must be reproducible from a later, slightly different reading, without storing the input itself. Dodis, Ostrovsky, Reyzin and Smith (SIAM J. Comput. 38(1), 2008; arXiv:cs/0602007) introduced secure sketches for this purpose: public helper data that lets the holder of a nearby reading recover the original exactly, while revealing as little as possible about it.

When the input is a set of features, the natural distance is the size of the symmetric difference. Juels and Sudan proposed the fuzzy vault for this setting (Des. Codes Cryptogr. 38, 2006). Section 6.2 of Dodis et al. gives a simpler, deterministic variant, the improved Juels–Sudan sketch (Construction 5), whose storage and entropy loss are both tlog⁡nt\log ntlogn for sss-element subsets of an nnn-element universe, independent of sss. The paper's Theorem 6.1 is the analysis of that construction. This mission formalizes it.

Setting

Laws and average min-entropy. A random variable is identified with its law. For a pair (A,B)(A,B)(A,B),

H~∞(A∣B)=−log⁡2∑bmax⁡aPr⁡[A=a∧B=b],\tilde H_\infty(A\mid B) = -\log_2 \sum_b \max_a \Pr[A=a \wedge B=b],H~∞​(A∣B)=−log2​b∑​amax​Pr[A=a∧B=b],

which equals −log⁡2Eb←B[max⁡aPr⁡[A=a∣B=b]]-\log_2 \mathbb E_{b\leftarrow B}\big[\max_a\Pr[A=a\mid B=b]\big]−log2​Eb←B​[maxa​Pr[A=a∣B=b]], the average min-entropy of §2.4: the negative logarithm of the best probability of guessing AAA after seeing BBB.

Secure sketches. Let M\mathcal MM be a set with an integer-valued distance dis\mathrm{dis}dis. A pair of procedures (SS,Rec)(\mathsf{SS},\mathsf{Rec})(SS,Rec) is an average-case (M,m,m~,t)(\mathcal M,m,\tilde m,t)(M,m,m~,t)-secure sketch (Definitions 3 and 4) if

  1. (correctness) dis(w,w′)≤t\mathrm{dis}(w,w')\le tdis(w,w′)≤t implies Rec(w′,SS(w))=w\mathsf{Rec}(w',\mathsf{SS}(w))=wRec(w′,SS(w))=w;
  2. (security) for all random variables WWW over M\mathcal MM and III with H~∞(W∣I)≥m\tilde H_\infty(W\mid I)\ge mH~∞​(W∣I)≥m, one has H~∞(W∣(SS(W),I))≥m~\tilde H_\infty(W\mid (\mathsf{SS}(W),I))\ge\tilde mH~∞​(W∣(SS(W),I))≥m~.

The difference m−m~m-\tilde mm−m~ is the entropy loss.

The metric. For a finite universe U\mathcal UU with n=∣U∣n=|\mathcal U|n=∣U∣, SDifs(U)\mathrm{SDif}_s(\mathcal U)SDifs​(U) is the set of sss-element subsets of U\mathcal UU with dis(w,w′)=∣w△w′∣\mathrm{dis}(w,w')=|w\triangle w'|dis(w,w′)=∣w△w′∣.

Construction 5. Identify U\mathcal UU with a finite field F\mathcal FF of nnn elements and let t≤st\le st≤s.

  • SS(w)\mathsf{SS}(w)SS(w): form p′(z)=∏x∈w(z−x)p'(z)=\prod_{x\in w}(z-x)p′(z)=∏x∈w​(z−x), monic of degree sss, and output its coefficients as−1,…,as−ta_{s-1},\dots,a_{s-t}as−1​,…,as−t​ of degree s−1s-1s−1 down to s−ts-ts−t.
  • Rec(w′,(as−1,…,as−t))\mathsf{Rec}(w',(a_{s-1},\dots,a_{s-t}))Rec(w′,(as−1​,…,as−t​)): form phigh(z)=zs+∑i=s−ts−1aizip_{\mathrm{high}}(z)=z^s+\sum_{i=s-t}^{s-1}a_iz^iphigh​(z)=zs+∑i=s−ts−1​ai​zi; find a polynomial plowp_{\mathrm{low}}plow​ of degree at most s−t−1s-t-1s−t−1 that agrees with phighp_{\mathrm{high}}phigh​ on at least s−t/2s-t/2s−t/2 points of w′w'w′ (Reed–Solomon decoding); output the roots of phigh−plowp_{\mathrm{high}}-p_{\mathrm{low}}phigh​−plow​.

The Lean development names these charPoly, sketchCoeffs, sketch, pHigh, Step3Cond and recover, and the metric SDifS with distance sdifDist, in the namespace FuzzyExtractors.ImprovedJS.

Formalization targets

Goal: Theorem 6.1

For every finite field F\mathcal FF with nnn elements, all t≤st\le st≤s and every real mmm,

(SS,Rec) is an average-case (SDifs(F), m, m−tlog⁡2n, t)-secure sketch.(\mathsf{SS},\mathsf{Rec})\ \text{is an average-case}\ \big(\mathrm{SDif}_s(\mathcal F),\,m,\,m-t\log_2 n,\,t\big)\text{-secure sketch}.(SS,Rec) is an average-case (SDifs​(F),m,m−tlog2​n,t)-secure sketch.

The goal is uniform in mmm: the entropy loss tlog⁡nt\log ntlogn does not depend on the input distribution.

Milestones (the correctness half)

The paper's argument on p. 21 splits into four steps, each a milestone:

  1. p′=phigh+qp'=p_{\mathrm{high}}+qp′=phigh​+q with deg⁡q≤s−t−1\deg q\le s-t-1degq≤s−t−1, and phigh=−qp_{\mathrm{high}}=-qphigh​=−q on www;
  2. ∣w△w′∣≤t|w\triangle w'|\le t∣w△w′∣≤t implies ∣w∩w′∣≥s−t/2|w\cap w'|\ge s-t/2∣w∩w′∣≥s−t/2, so −q-q−q is a valid plowp_{\mathrm{low}}plow​;
  3. any two valid plowp_{\mathrm{low}}plow​ coincide;
  4. Rec(w′,SS(w))=w\mathsf{Rec}(w',\mathsf{SS}(w))=wRec(w′,SS(w))=w whenever ∣w△w′∣≤t|w\triangle w'|\le t∣w△w′∣≤t.

A fifth, off the goal's path, records Step 2's remark that the sketch consists of the first ttt elementary symmetric polynomials of www, up to sign.

The security half is the entropy bound: since SS\mathsf{SS}SS takes at most ntn^tnt values, H~∞(W∣(SS(W),I))≥H~∞(W∣I)−tlog⁡n\tilde H_\infty(W\mid(\mathsf{SS}(W),I))\ge\tilde H_\infty(W\mid I)-t\log nH~∞​(W∣(SS(W),I))≥H~∞​(W∣I)−tlogn (the paper cites its Lemma 3.1, which is posed in the first mission of this series and is not restated here).

Significance

The result. Theorem 6.1 gives a secure sketch for set difference whose sketch length and entropy loss are tlog⁡nt\log ntlogn, which the paper shows is essentially optimal when n≫sn\gg sn≫s (§6.2, via Lemma C.1 and a constant-weight code bound). It improves the original fuzzy vault, whose entropy loss the paper analyses in Appendix D and finds good only when the stored data is very large. Through the paper's generic composition with randomness extractors (Lemma 4.1), it yields fuzzy extractors for set-valued inputs in large universes, the regime of biometric feature sets.

Formalizing it. The theorem is proved in the paper; no machine-checked version exists on Prove2Me or, to our knowledge, elsewhere. A formal proof combines three pieces of reusable infrastructure: a probabilistic layer (average min-entropy of laws on arbitrary types, and the chain-rule-type bound for a function with few values), the combinatorics of symmetric differences of equal-size sets, and the algebra of Reed–Solomon unique decoding (a low-degree polynomial is determined by its values on enough points). Each of these is useful beyond this mission.

Difficulty

No step is deep; the difficulty is in the bookkeeping. The correctness argument relies on exact degree accounting: phighp_{\mathrm{high}}phigh​ must agree with p′p'p′ in every coefficient of degree at least s−ts-ts−t, so that the remainder has degree at most s−t−1s-t-1s−t−1, and the uniqueness count ("two candidates agree on at least s−ts-ts−t points") requires the threshold to be at least s−t/2s-t/2s−t/2; the paper's sentence says "more than", which does not support the argument as written. The roots of phigh−plowp_{\mathrm{high}}-p_{\mathrm{low}}phigh​−plow​ must be shown to form exactly the set www, with no multiplicities lost. The security half needs the average min-entropy of a joint law with a deterministic, ntn^tnt-valued component bounded uniformly over all auxiliary variables, including those with infinite or uncountable range, where sums are infinite sums of extended nonnegative reals.

Formalization scope

Conventions committed to in Lean:

  • Laws are PMFs; the procedures are kernels M → PMF S, here deterministic (PMF.pure). Average min-entropy is the joint form above, logarithms base 2, and the auxiliary III ranges over an arbitrary ι : Type (a superset of the paper's {0,1}∗\{0,1\}^*{0,1}∗), never restricted to finite types.
  • The universe is the field F\mathcal FF itself, [Field 𝔽] [Fintype 𝔽], with nnn = Fintype.card 𝔽; the paper's "nnn is a prime power" is then automatic.
  • The paper leaves t≤st\le st≤s implicit; every statement assumes it. No parity condition on ttt is imposed: "at least s−t/2s-t/2s−t/2" is written 2⋅#≥2s−t2\cdot\#\ge 2s-t2⋅#≥2s−t in N\mathbb NN, which covers odd ttt.
  • "Degree at most s−t−1s-t-1s−t−1" is degree < s - t, so plow=0p_{\mathrm{low}}=0plow​=0 when t=st=st=s.
  • The sketch is a vector in Ft\mathcal F^tFt indexed from 000: entry iii is the coefficient of degree s−1−is-1-is−1−i. The storage bound tlog⁡nt\log ntlogn holds by this type and is not restated.
  • Rec\mathsf{Rec}Rec takes an arbitrary valid plowp_{\mathrm{low}}plow​ (by choice) instead of running a decoding algorithm. The paper's "fail" output is encoded as returning w′w'w′, which only occurs when correctness makes no claim.
  • Running time is out of scope. Theorem 6.1's clause that SS\mathsf{SS}SS and Rec\mathsf{Rec}Rec run in time polynomial in sss, ttt and log⁡n\log nlogn is dropped, and no surrogate predicate replaces it.

A formalization that checks only correctness, drops or trivializes the entropy clause, or lets Rec\mathsf{Rec}Rec see www itself, would not be Theorem 6.1. The goal states both clauses through the definition of an average-case secure sketch, with Rec\mathsf{Rec}Rec given only w′w'w′ and the sketch.

Contributions welcome: proofs of the milestones, a general lemma bounding average min-entropy loss by the logarithm of the number of sketch values (the paper's Lemma 2.2(b) and Lemma 3.1), and Reed–Solomon uniqueness lemmas stated for reuse.

Selected references

  • Y. Dodis, R. Ostrovsky, L. Reyzin, A. Smith, Fuzzy Extractors: How to Generate Strong Keys from Biometrics and Other Noisy Data, SIAM J. Comput. 38(1):97–139, 2008. https://doi.org/10.1137/060651380 ; arXiv:cs/0602007v4, https://arxiv.org/abs/cs/0602007
  • A. Juels, M. Sudan, A Fuzzy Vault Scheme, Designs, Codes and Cryptography 38(2):237–257, 2006. https://doi.org/10.1007/s10623-005-6343-z
  • E. Agrell, A. Vardy, K. Zeger, Upper Bounds for Constant-Weight Codes, IEEE Trans. Inform. Theory 46(7):2373–2395, 2000. https://doi.org/10.1109/18.887851
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Numerical Analysis·Captain: Lucas

Métodos Numéricos (Freitas) II: Zeros de Polinômios e o Algoritmo de HornerTextbook

Motivation

Polynomial equations are the special case of root finding where algebra says a great deal before analysis is needed: the number of roots is known, the roots of a real polynomial come in conjugate pairs, the rational candidates can be listed, and the whole complex plane can be narrowed down to an annulus that must contain every root. A numerical method that exploits this information starts closer to the answer and needs fewer evaluations; and each evaluation itself can be made cheaper by Horner's scheme, which also delivers the deflated quotient for free.

This mission is the second in a series formalizing the lecture notes Métodos Numéricos by Sergio Roberto de Freitas (UFMS, 2000). It covers Chapter 4, Zeros de Polinômios.

Setting

Throughout, a polynomial is written in the book's convention

P(z)=a0zn+a1zn−1+dots+an−1z+an,P(z) = a_0 z^n + a_1 z^{n-1} + \\dots + a_{n-1} z + a_n,P(z)=a0​zn+a1​zn−1+dots+an−1​z+an​,

so the index iii names the coefficient of zn−iz^{n-i}zn−i and a0a_0a0​ is the leading coefficient. The coefficients are real (integral, in the rational-root milestone) and zzz ranges over mathbbC\\mathbb{C}mathbbC unless stated otherwise.

Horner's algorithm computes P(c)P(c)P(c) by the recurrence b0=a0b_0 = a_0b0​=a0​, bi=ai+c,bi−1b_i = a_i + c\\,b_{i-1}bi​=ai​+c,bi−1​, so that P(c)=bnP(c) = b_nP(c)=bn​, using nnn multiplications and nnn additions. The same numbers b0,dots,bn−1b_0, \\dots, b_{n-1}b0​,dots,bn−1​ are the coefficients of the deflated polynomial QQQ with P(w)=(w−c),Q(w)+P(c)P(w) = (w - c)\\,Q(w) + P(c)P(w)=(w−c),Q(w)+P(c).

With A=max∣a1∣,dots,∣an∣A = \\max\\{|a_1|, \\dots, |a_n|\\}A=max∣a1​∣,dots,∣an​∣ and B=max∣a0∣,dots,∣an−1∣B = \\max\\{|a_0|, \\dots, |a_{n-1}|\\}B=max∣a0​∣,dots,∣an−1​∣, the chapter's two localization results confine the roots to the annulus

frac11+B/∣an∣;le;∣z∣;le;1+fracA∣a0∣.\\frac{1}{1 + B/|a_n|} \\;\\le\\; |z| \\;\\le\\; 1 + \\frac{A}{|a_0|}.frac11+B/∣an​∣;le;∣z∣;le;1+fracA∣a0​∣.

Target

The goal theorem is the outer bound (Proposição 4.2.1): every complex root of PPP satisfies ∣z∣le1+A/∣a0∣|z| \\le 1 + A/|a_0|∣z∣le1+A/∣a0​∣, where AAA is the largest absolute value among the non-leading coefficients.

The milestones are the companion results of the chapter: the inner bound (Proposição 4.2.2), the fact that non-real roots of a real polynomial occur in conjugate pairs (Proposição 4.1.1), the existence of a real root in odd degree (Proposição 4.1.2), the correctness of Horner's evaluation scheme, and the deflation identity that accompanies it.

Significance

The two localization bounds are what makes a search for complex roots finite: they give an explicit compact region to sweep, and they give scale information that prevents an iteration from wandering off. The conjugate-pair statement halves the work for real polynomials and is the reason odd-degree real polynomials always have a real root. The rational-root test turns exact factorization into a finite search. Horner's scheme is the standard way a polynomial is evaluated inside every root finder, and its deflation identity is what lets a method remove a root that has already been found and continue with a polynomial of lower degree.

Mathlib already contains general results close to some of these (a polynomial over a real closed field of odd degree has a root; rational-root divisibility), so those milestones are accessible; the two localization bounds and the Horner statements in the book's index convention are the substantive new work.

Difficulty

The localization proofs in the source are short but rest on a geometric-series estimate that is only valid for ∣z∣>1|z| > 1∣z∣>1; the boundary cases ∣z∣le1|z| \\le 1∣z∣le1 have to be treated separately in a formal proof, and the degenerate situations (n=1n = 1n=1, coefficients all zero except the leading one) must be checked rather than waved through. The inner bound is obtained from the outer one by the substitution w=1/zw = 1/zw=1/z, which requires knowing that zneq0z \\neq 0zneq0 is a root of PPP if and only if www is a root of the reversed polynomial — an argument that has to be made explicit. The Horner statements look computational but need a careful induction because the exponents are natural-number subtractions.

Formalization scope

Coefficients are given as a function a:mathbbNtomathbbRa : \\mathbb{N} \\to \\mathbb{R}a:mathbbNtomathbbR together with a degree nnn, and the polynomial is the finite sum sumi=0naizn−i\\sum_{i=0}^{n} a_i z^{n-i}sumi=0n​ai​zn−i; two versions are provided, one evaluated at a real point and one at a complex point, with the coefficients coerced into mathbbC\\mathbb{C}mathbbC. Only indices 0leilen0 \\le i \\le n0leilen are read, so the values of aaa beyond nnn are irrelevant to every statement. The exponent n−in - in−i is natural-number subtraction, which is harmless in this range. No hypothesis says that the family aaa describes a polynomial of exact degree nnn beyond the explicit assumptions a0neq0a_0 \\neq 0a0​neq0 or anneq0a_n \\neq 0an​neq0 where they appear. The constants AAA and BBB are given as hypotheses equating them to the maximum of the relevant finite family of absolute values, rather than being defined separately. The rational-root and odd-degree milestones are stated with Mathlib's polynomial type instead of the coefficient-family encoding, since their statements involve no index convention.

Selected references

  • S. R. Freitas, Métodos Numéricos, Departamento de Computação e Estatística, Universidade Federal de Mato Grosso do Sul, 2000. Chapter 4, Zeros de Polinômios, pp. 71–84. (Course notes supplied with this mission.)
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Mathematical Physics·Captain: Lucas

Brown-Gabrielse Invariance Theorem for an Imperfect Penning TrapResearch Paper

Motivation

The most precisely measured property of an elementary particle is the magnetic moment of the electron. The 2022 Northwestern measurement of Fan, Myers, Sukra and Gabrielse (arXiv:2209.13084) reports −μ/μB=g/2=1.001 159 652 180 59 (13)-\mu/\mu_B=g/2=1.001\,159\,652\,180\,59\,(13)−μ/μB​=g/2=1.00115965218059(13), and, combined with the Standard-Model prediction, α−1=137.035 999 166 (15)\alpha^{-1}=137.035\,999\,166\,(15)α−1=137.035999166(15). Those numbers are experimental results, not theorems, and nothing in this mission asserts them.

What is a theorem is the piece of mathematics the measurement rests on. A single electron is held in a Penning trap: a uniform magnetic field plus an electrostatic quadrupole potential. The quantity the experiment needs is the free-space cyclotron frequency νc=eB/(2πm)\nu_c=eB/(2\pi m)νc​=eB/(2πm), but what a trap lets you observe are its three normal-mode frequencies — the trap-modified cyclotron frequency νˉc\bar\nu_cνˉc​, the axial frequency νˉz\bar\nu_zνˉz​, and the magnetron frequency νˉm\bar\nu_mνˉm​. A real apparatus is never perfect: the magnetic field is tilted relative to the axis of the potential, and the potential is elliptically distorted. The invariance theorem of Brown and Gabrielse (Phys. Rev. A 25, 2423 (1982)), quoted as Eq. (4) of the measurement paper, says that a particular combination of the three observed frequencies is completely insensitive to both imperfections:

νc=νˉc2+νˉz2+νˉm2.\nu_c=\sqrt{\bar\nu_c^{2}+\bar\nu_z^{2}+\bar\nu_m^{2}}.νc​=νˉc2​+νˉz2​+νˉm2​​.

This is what makes a part-per-trillion measurement possible with an imperfect trap, and it is the object of this mission.

Setting

Work in R3\mathbb{R}^3R3. A particle of charge qqq and mass mmm sits in a uniform magnetic field B=B b\mathbf B=B\,bB=Bb with bbb a unit vector, and in the static field of a quadratic electrostatic potential. Dividing the Hessian of that potential by the mass gives a real 3×33\times33×3 matrix KKK, and the equation of motion of the particle is linear:

r′′(t)  =  −K r(t)  +  ωc (r′(t)×b),ωc=qBm.r''(t)\;=\;-K\,r(t)\;+\;\omega_c\,\big(r'(t)\times b\big),\qquad \omega_c=\frac{qB}{m}.r′′(t)=−Kr(t)+ωc​(r′(t)×b),ωc​=mqB​.

Two properties of KKK carry all the physics of the trap: KKK is symmetric, because it is a Hessian, and traceless, because the potential satisfies Laplace's equation in the vacuum region where the particle moves. Beyond that, KKK is arbitrary — an arbitrary KKK is exactly what "the axis of the potential is tilted relative to bbb, and the potential is elliptically distorted" means, so no separate tilt angle or ellipticity parameter appears anywhere.

Substituting the ansatz r(t)=u e−iωtr(t)=u\,e^{-i\omega t}r(t)=ue−iωt with u∈C3u\in\mathbb{C}^3u∈C3 turns the equation of motion into the linear system M(ω) u=0M(\omega)\,u=0M(ω)u=0, where

M(ω)  =  K−ω2I−i ω ωc C(b),C(b)=(0−b3b2b30−b1−b2b10)M(\omega)\;=\;K-\omega^{2}I-i\,\omega\,\omega_c\,C(b), \qquad C(b)=\begin{pmatrix}0&-b_3&b_2\\ b_3&0&-b_1\\ -b_2&b_1&0\end{pmatrix}M(ω)=K−ω2I−iωωc​C(b),C(b)=​0b3​−b2​​−b3​0b1​​b2​−b1​0​​

is the matrix of u↦b×uu\mapsto b\times uu↦b×u. A frequency ω\omegaω is a normal mode of the trap precisely when det⁡M(ω)=0\det M(\omega)=0detM(ω)=0. The three eigenfrequencies of the trap, written ωˉc,ωˉz,ωˉm\bar\omega_c,\bar\omega_z,\bar\omega_mωˉc​,ωˉz​,ωˉm​ (angular versions of νˉc,νˉz,νˉm\bar\nu_c,\bar\nu_z,\bar\nu_mνˉc​,νˉz​,νˉm​), are the non-negative solutions of that equation.

Target

The goal is the invariance theorem in the form: if the three numbers ωˉc,ωˉz,ωˉm\bar\omega_c,\bar\omega_z,\bar\omega_mωˉc​,ωˉz​,ωˉm​ are the eigenfrequencies of the trap, in the sense that

det⁡M(ω)=−(ω2−ωˉc2)(ω2−ωˉz2)(ω2−ωˉm2)for all ω∈R,\det M(\omega)=-\big(\omega^{2}-\bar\omega_c^{2}\big)\big(\omega^{2}-\bar\omega_z^{2}\big)\big(\omega^{2}-\bar\omega_m^{2}\big)\quad\text{for all }\omega\in\mathbb{R},detM(ω)=−(ω2−ωˉc2​)(ω2−ωˉz2​)(ω2−ωˉm2​)for all ω∈R,

then, for every symmetric traceless KKK and every unit vector bbb,

ωˉc2+ωˉz2+ωˉm2  =  ωc2.\bar\omega_c^{2}+\bar\omega_z^{2}+\bar\omega_m^{2}\;=\;\omega_c^{2}.ωˉc2​+ωˉz2​+ωˉm2​=ωc2​.

The milestones are the three steps of the argument, in increasing order of dependence:

  1. Mode equation. The exponential ansatz solves the equation of motion at every time if and only if its amplitude lies in the kernel of M(ω)M(\omega)M(ω). This is what makes M(ω)M(\omega)M(ω) the right object to take determinants of.
  2. Characteristic polynomial. For symmetric KKK, det⁡M(ω)\det M(\omega)detM(ω) is real and depends on ω\omegaω only through ω2\omega^2ω2: it equals −q(ω2)-q(\omega^2)−q(ω2) with q(λ)=det⁡(λI−K)−ωc2λ(λ⟨b,b⟩−⟨b,Kb⟩)q(\lambda)=\det(\lambda I-K)-\omega_c^{2}\lambda(\lambda\langle b,b\rangle-\langle b,Kb\rangle)q(λ)=det(λI−K)−ωc2​λ(λ⟨b,b⟩−⟨b,Kb⟩).
  3. Ideal trap. For K=diag⁡(−ωz2/2,−ωz2/2,ωz2)K=\operatorname{diag}(-\omega_z^2/2,-\omega_z^2/2,\omega_z^2)K=diag(−ωz2​/2,−ωz2​/2,ωz2​), b=(0,0,1)b=(0,0,1)b=(0,0,1) and ωc2≥2ωz2\omega_c^2\ge 2\omega_z^2ωc2​≥2ωz2​, the determinant factors explicitly, with eigenfrequencies (ωc±ωc2−2ωz2)/2(\omega_c\pm\sqrt{\omega_c^2-2\omega_z^2})/2(ωc​±ωc2​−2ωz2​​)/2 and ωz\omega_zωz​.

Significance

The result. The invariance theorem is why the electron magnetic moment can be measured to 0.130.130.13 parts per trillion in an apparatus whose magnetic field and electrode axis are not, and cannot be, exactly aligned. Without it, every misalignment and every elliptic distortion would enter the extracted νc\nu_cνc​ as a systematic error, and the frequency ratio νa/νc\nu_a/\nu_cνa​/νc​ that gives g/2g/2g/2 would have to be corrected with a model of the imperfections rather than being invariant under them.

Formalizing it. The theorem is a short, completely classical piece of linear algebra — the point of formalizing it is to have the frequency-metrology identity available as a machine-checked statement, together with a reusable model of linear motion in crossed electric and magnetic fields (the mode matrix, its characteristic cubic, and the correspondence between the exponential ansatz and the kernel of the mode matrix).

Status — please read before treating this as open. All four statements in this proposal have been proved by the drafting agent on a local Lean 4.28 / Mathlib installation; the proofs are deliberately not uploaded, so the platform statements are genuinely open here, but this is a formalization-transfer mission, not an open research problem. Milestone 3 is included precisely so that the goal's factorization hypothesis is known to be satisfiable and the goal is not vacuously true. The statements themselves were additionally compiled in this platform's default Lean environment before this proposal was assembled.

Difficulty

The obvious first idea — solve det⁡M(ω)=0\det M(\omega)=0detM(ω)=0 and add up the roots — is exactly the thing not to do: for a tilted, elliptically distorted trap the three eigenfrequencies have no usable closed form. The whole content of the theorem is that the sum of their squares is the coefficient of ω4\omega^4ω4 in the characteristic polynomial and therefore needs no root formula at all: it is Vieta plus the two structural facts tr⁡K=0\operatorname{tr}K=0trK=0 and ⟨b,b⟩=1\langle b,b\rangle=1⟨b,b⟩=1. The work in Lean is consequently not analysis but bookkeeping: computing a 3×33\times33×3 determinant with complex off-diagonal entries and extracting one coefficient of the resulting cubic in ω2\omega^2ω2. The one place real care is needed is the mode-equation milestone, where derivatives of complex-valued functions of a real variable must be handled honestly.

Formalization scope

Conventions fixed by the Lean statements, and not visible in the prose:

  1. Vectors are functions on a three-element index set and matrices are 3×33\times33×3; no abstract inner-product space is used.
  2. KKK is an arbitrary real matrix in the definitions; symmetry and tracelessness are hypotheses on the individual theorems, not part of the model.
  3. "Unit vector" is the algebraic condition ⟨b,b⟩=1\langle b,b\rangle=1⟨b,b⟩=1; no norm is used.
  4. The magnetic term is −i ω ωc C(b)-i\,\omega\,\omega_c\,C(b)−iωωc​C(b) with C(b)u=b×uC(b)u=b\times uC(b)u=b×u, i.e. the sign convention is fixed by the ansatz r(t)=u e−iωtr(t)=u\,e^{-i\omega t}r(t)=ue−iωt and the force ωc (r′×b)\omega_c\,(r'\times b)ωc​(r′×b).
  5. "The eigenfrequencies are ωˉc,ωˉz,ωˉm\bar\omega_c,\bar\omega_z,\bar\omega_mωˉc​,ωˉz​,ωˉm​" is formalized as the functional identity det⁡M(ω)=−(ω2−ωˉc2)(ω2−ωˉz2)(ω2−ωˉm2)\det M(\omega)=-(\omega^2-\bar\omega_c^2)(\omega^2-\bar\omega_z^2)(\omega^2-\bar\omega_m^2)detM(ω)=−(ω2−ωˉc2​)(ω2−ωˉz2​)(ω2−ωˉm2​) for all real ω\omegaω — that is, as a factorization with multiplicity, not as a set of solutions of det⁡M(ω)=0\det M(\omega)=0detM(ω)=0, which would not pin down multiplicities and would make the sum rule false in degenerate cases.
  6. No sign conditions are imposed on ωˉc,ωˉz,ωˉm\bar\omega_c,\bar\omega_z,\bar\omega_mωˉc​,ωˉz​,ωˉm​; the conclusion involves only their squares.
  7. Nothing in this mission formalizes any measured quantity: g/2g/2g/2, α\alphaα, and the frequencies of the actual apparatus appear only as motivation.

Only Mathlib is needed: matrices over R\mathbb{R}R and C\mathbb{C}C, determinants of 3×33\times33×3 matrices, the cross product, and derivatives of complex-valued functions of a real variable. The definitions are reusable for any linear-motion-in-a-magnetic-field problem.

Selected references

  • X. Fan, T. G. Myers, B. A. D. Sukra, G. Gabrielse, Measurement of the Electron Magnetic Moment, Phys. Rev. Lett. 130, 071801 (2023), arXiv:2209.13084 — Eq. (4) is the statement formalized here.
  • L. S. Brown, G. Gabrielse, Precision spectroscopy of a charged particle in an imperfect Penning trap, Phys. Rev. A 25, 2423 (1982), doi:10.1103/PhysRevA.25.2423 — the original invariance theorem.
  • L. S. Brown, G. Gabrielse, Geonium theory: Physics of a single electron or ion in a Penning trap, Rev. Mod. Phys. 58, 233 (1986), doi:10.1103/RevModPhys.58.233 — the trap eigenfrequencies and the hierarchy νˉc≫νˉz≫νˉm\bar\nu_c\gg\bar\nu_z\gg\bar\nu_mνˉc​≫νˉz​≫νˉm​.
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Mathematical Physics·Captain: Lucas

Koide Mass Relation: Exact Algebraic ContentResearch Paper

Motivation

In 1982 Yoshio Koide, searching for an empirical formula for the Cabibbo angle, noticed that the three charged-lepton masses satisfy

me+mμ+mτ  =  23(me+mμ+mτ)2.m_e + m_\mu + m_\tau \;=\; \frac{2}{3}\left(\sqrt{m_e}+\sqrt{m_\mu}+\sqrt{m_\tau}\right)^2 .me​+mμ​+mτ​=32​(me​​+mμ​​+mτ​​)2.

With the present-day values me=0.510998910±0.000000013m_e = 0.510998910 \pm 0.000000013me​=0.510998910±0.000000013 MeV, mμ=105.6583663±0.0000038m_\mu = 105.6583663 \pm 0.0000038mμ​=105.6583663±0.0000038 MeV and mτ=1776.99±0.29m_\tau = 1776.99 \pm 0.29mτ​=1776.99±0.29 MeV, the dimensionless ratio on the left over the bracket on the right equals 0.666667±0.0000160.666667 \pm 0.0000160.666667±0.000016 — the value 23\tfrac{2}{3}32​ to five digits. Whether this is numerology or a shadow of flavour physics beyond the Standard Model is an open physics question; what is not open, and what this mission is about, is the exact mathematical content of the relation: which triples of nonnegative reals satisfy it, what its polynomial (square-root-free) consequences are, and what its geometric reading is.

The material formalized here is Chapter 3 ("A Mass Relation") of F. Goffinet's 2008 doctoral thesis A bottom-up approach to fermion masses (Université catholique de Louvain), which collects the algebraic and geometric properties of the relation and proposes a mixing-matrix generalization. None of the statements below depends on any physics input: they are elementary real-algebraic facts about the function qqq defined next. The physics enters only in which numbers one plugs in.

Setting

For a family of nnn nonnegative "masses" m=(m1,…,mn)m = (m_1,\dots,m_n)m=(m1​,…,mn​), not all zero, define the Koide splitting parameter

q(m)  =  ∑imi(∑imi)2.q(m) \;=\; \frac{\sum_{i} m_i}{\bigl(\sum_i \sqrt{m_i}\bigr)^{2}} .q(m)=(∑i​mi​​)2∑i​mi​​.

In Lean this is koideRatio, defined by exactly this quotient for m : Fin n → ℝ (with Lean's convention that x=0\sqrt{x}=0x​=0 for x<0x<0x<0 and x/0=0x/0 = 0x/0=0, so the definition is total; every statement in the mission carries the nonnegativity and nondegeneracy hypotheses that make it meaningful).

Two further objects from the chapter are formalized alongside it.

  • The degeneracy angle. Put S=(m1,…,mn)S = (\sqrt{m_1},\dots,\sqrt{m_n})S=(m1​​,…,mn​​) in "generation space" and let ψ\psiψ be the angle between SSS and the democratic direction (1,…,1)(1,\dots,1)(1,…,1). In Lean, koideCos is the cosine ⟨S,1⟩/(∥S∥ ∥1∥)\langle S,\mathbf 1\rangle/(\lVert S\rVert\,\lVert\mathbf 1\rVert)⟨S,1⟩/(∥S∥∥1∥) written out as a quotient of sums, and koideAngle is its arccos⁡\arccosarccos.
  • The pseudo-masses of the chapter's generalization: given a mixing matrix U∈Cn×nU \in \mathbb{C}^{n\times n}U∈Cn×n, m~i=∣∑jUijmj∣\tilde m_i = \bigl|\sum_j U_{ij} m_j\bigr|m~i​=​∑j​Uij​mj​​ (pseudoMass).

Koide's relation is the statement q(me,mμ,mτ)=23q(m_e,m_\mu,m_\tau) = \tfrac{2}{3}q(me​,mμ​,mτ​)=32​; the value q=13q=\tfrac13q=31​ corresponds to exact degeneracy m1=m2=m3m_1=m_2=m_3m1​=m2​=m3​ and q=1q=1q=1 to maximal hierarchy.

Target

The goal theorem is the exact solution of the relation for the third mass. For m1,m2,m3>0m_1,m_2,m_3>0m1​,m2​,m3​>0, writing P=m1m2P = \sqrt{m_1 m_2}P=m1​m2​​ and R=m1+4P+m2R = \sqrt{m_1 + 4P + m_2}R=m1​+4P+m2​​,

q(m1,m2,m3)=23  ⟺  m3=7(m1+m2)+20P+43 (m1+m2)Rq(m_1,m_2,m_3) = \tfrac{2}{3} \iff m_3 = 7(m_1+m_2) + 20P + 4\sqrt3\,(\sqrt{m_1}+\sqrt{m_2})Rq(m1​,m2​,m3​)=32​⟺m3​=7(m1​+m2​)+20P+43​(m1​​+m2​​)R or( 4P<m1+m2  and  m3=7(m1+m2)+20P−43 (m1+m2)R ).\textrm{or}\quad \bigl(\, 4P < m_1+m_2 \ \textrm{ and }\ m_3 = 7(m_1+m_2) + 20P - 4\sqrt3\,(\sqrt{m_1}+\sqrt{m_2})R \,\bigr).or(4P<m1​+m2​  and  m3​=7(m1​+m2​)+20P−43​(m1​​+m2​​)R).

This is equation (3.25) of the source, made precise: the "−-−" branch of (3.25) is a genuine solution exactly when 4m1m2<m1+m24\sqrt{m_1m_2} < m_1+m_24m1​m2​​<m1​+m2​, and is a spurious root of the squared equation otherwise (for instance at m1=m2m_1=m_2m1​=m2​, where the "−-−" value is positive but fails the relation).

The milestones cover, in the source's order: the range 1n≤q≤1\tfrac1n \le q \le 1n1​≤q≤1 and its two equality cases (Table 3.1); the geometric reading cos⁡ψ=1/n q\cos\psi = 1/\sqrt{n\,q}cosψ=1/nq​ and the equivalence ψ=45∘  ⟺  q=23\psi = 45^\circ \iff q = \tfrac23ψ=45∘⟺q=32​ (eq. (3.5)–(3.6), Fig. 3.1); the square-root-free polynomial consequence (eq. (3.24)) and its matrix form (eq. (3.30)); the failure of the converse (eqs. (3.26)–(3.28)); the ∑izi=0\sum_i z_i = 0∑i​zi​=0 reformulation in the composite-model parametrization (eqs. (3.18)–(3.22)); the τ\tauτ-mass prediction (eq. (3.4)); and the fact that the pseudo-mass extension (3.31)–(3.32) reduces to the original relation at U=IdU = \mathrm{Id}U=Id.

Significance

The result itself. The goal theorem turns an empirical numerical coincidence into a complete description of its solution set: given any two masses, it says exactly which third masses are admissible, and it separates the two roots by an explicit inequality. This is what licenses the standard use of the relation as a prediction: fixing mem_eme​ and mμm_\mumμ​ and the normal hierarchy mτ>mμm_\tau > m_\mumτ​>mμ​ singles out one root, giving mτ=1776.968874m_\tau = 1776.968874mτ​=1776.968874 MeV, a number two orders of magnitude more precise than the direct measurement (milestone on eq. (3.4)). The bound 13≤q≤1\tfrac13 \le q \le 131​≤q≤1 with its equality cases explains why the relation can never hold for the neutrinos in a near-degenerate spectrum, and why the up-quark family sits near the opposite boundary. The square-root-free form (3.24)/(3.30) is what any Lagrangian-level model must reproduce, since square roots of masses do not appear in a mass matrix; the failure of its converse is the price paid for removing them, and the mission pins that failure down with an explicit witness.

Formalizing it. All the statements here are classical-strength real algebra, and none is formalized in Mathlib: there is no koideRatio, no Cauchy–Schwarz-style equality analysis for the ∑m\sum m∑m vs. (∑m)2(\sum\sqrt m)^2(∑m​)2 pair, and no treatment of the 45∘45^\circ45∘ geometry. The mission produces a small reusable development — the parameter, its sharp bounds with equality cases, and its angle formulation — that any later formalization of mass-relation phenomenology can import. It also records, machine-checked, where the source text is imprecise: the "±\pm±" discussion after (3.25) and the claim that (3.1) has exactly two solutions for the third mass.

Difficulty

Nothing here needs heavy machinery, and everything here needs care with square roots.

The bounds are Cauchy–Schwarz in one direction and (∑mi)2≥∑mi\bigl(\sum\sqrt{m_i}\bigr)^2 \ge \sum m_i(∑mi​​)2≥∑mi​ in the other, but the equality cases are where the work is: the upper bound saturates exactly when at most one mass is nonzero, and a proof must handle the mixed terms without assuming positivity of all entries. The goal theorem is a quadratic in z=m3z = \sqrt{m_3}z=m3​​ — z2−4(x+y)z+(x2+y2−4xy)=0z^2 - 4(x+y)z + (x^2+y^2-4xy) = 0z2−4(x+y)z+(x2+y2−4xy)=0 with x=m1x=\sqrt{m_1}x=m1​​, y=m2y=\sqrt{m_2}y=m2​​ — so the difficulty is not solving it but keeping the equivalence exact in both directions: passing from m3m_3m3​ back to zzz requires z≥0z \ge 0z≥0, which is precisely where the "−-−" branch survives or dies, and the discriminant has to be recognized as a perfect square times 333. The obvious route of squaring the relation twice, as the source does to reach (3.24), is not reversible; a solver who squares must come back and discharge the sign conditions, and the counterexample milestone shows that the lost information is real.

Formalization scope

Masses are real numbers, not physical quantities with units, and are indexed by Fin n (Fin 3 for the three-generation statements); the mixing matrix in the pseudo-mass definition is complex, as in the source. koideRatio, koideCos, koideAngle and pseudoMass are total functions and rely on Lean's junk conventions outside their intended domain, so each statement carries its own hypotheses — nonnegativity of every entry and the existence of a strictly positive entry — rather than delegating them to the definitions. No statement is vacuous: every hypothesis set is satisfied by the physical charged-lepton triple, and the degenerate configurations the quantifiers admit (all-zero families, the n=0n=0n=0 family) are excluded by those hypotheses rather than by a side condition that can never hold.

The angle statements use Real.arccos and are stated for the cosine written out as an explicit quotient of sums, not through an inner-product-space instance; a solver is free to route the proof through EuclideanSpace if that is convenient. The matrix milestone uses Matrix.IsHermitian.eigenvalues for a 3×33\times33×3 complex Hermitian matrix and states the conclusion as an identity in C\mathbb{C}C between tr⁡M\operatorname{tr} MtrM, tr⁡M2\operatorname{tr} M^2trM2 and det⁡M\det MdetM. Contributions of general-nnn versions of the three-generation statements, and of the equality analysis as standalone lemmas, are welcome.

Selected references

  • F. Goffinet, A bottom-up approach to fermion masses, PhD thesis, Université catholique de Louvain, December 2008. Chapter 3, pp. 59–86. http://hdl.handle.net/2078.1/20873
  • Y. Koide, A fermion–boson composite model of quarks and leptons, Phys. Lett. B 120 (1983) 161–165. https://doi.org/10.1016/0370-2693(83)90644-5
  • Y. Koide, Challenge to the mystery of the charged lepton mass formula, https://arxiv.org/abs/hep-ph/0506247
  • R. Foot, A note on Koide's lepton mass relation, https://arxiv.org/abs/hep-ph/9402242 (the 45∘45^\circ45∘ geometric reading).
  • J.-M. Gérard, F. Goffinet, M. Herquet, A new look at an old mass relation, Phys. Lett. B 633 (2006) 563–566. https://arxiv.org/abs/hep-ph/0510289 (the pseudo-mass extension).
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