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Geometry & Topology

34 missions · 14 completed

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Algebraic Topology·Captain: ryanshin

Smooth 4-dimensional Poincaré conjecture: foundations and reductionsOpen Problem

Motivation

The smooth four-dimensional Poincaré conjecture asks whether a smooth manifold with the topology of the four-sphere must also have its standard smooth structure, up to diffeomorphism. The distinction is between the existence of continuous coordinates and the compatibility of differentiable coordinates. The mission concerns this precise sphere question, listed as open in Problem 4.1 of K3 — A New Problem List in Low-Dimensional Topology. It does not treat a collection of algebraic obstructions as an existing proof of the conjecture. Baykur–Kirby–Ruberman, Problem 4.1

Historical landmarks

  • 1961: Smale proved that a closed smooth manifold homotopy equivalent to a sphere of dimension at least five is homeomorphic to that sphere. This is not a theorem that all such smooth manifolds are diffeomorphic to the standard sphere. Smale, Theorem A
  • 1982: Freedman established the topological four-dimensional Poincaré theorem: a topological four-manifold homotopy equivalent to the four-sphere is homeomorphic to it. Freedman, Theorem 1.6
  • 2026: The K3 problem list continues to distinguish this established topological result from the open smooth sphere problem. Problem 4.1, pp. 191–192

Setting

Let S4S^4S4 be the unit sphere in R5ℝ^5R5, with its standard stereographic smooth structure. A homeomorphism is a continuous bijection with continuous inverse; a diffeomorphism is a smooth bijection with smooth inverse. A smooth atlas is a collection of local Euclidean coordinates whose transition maps are smooth.

The manifold MMM is compact and Hausdorff, has no boundary, and is equipped with a specified smooth atlas modeled on R4ℝ^4R4. The given atlas is arbitrary: it is not defined by transporting the standard structure from S4S^4S4.

For a homeomorphism e:N→S4e:N\to S^4e:N→S4, let Ae\mathcal A_eAe​ denote the atlas transported from the standard sphere along eee. A structomorphism for the smooth structure groupoid is a homeomorphism whose coordinate expressions belong to that groupoid. The predicate SPC4Pullback\mathsf{SPC4Pullback}SPC4Pullback requires, for every given smooth atlas A\mathcal AA on such an NNN and every such eee, a structomorphism between (N,A)(N,\mathcal A)(N,A) and (N,Ae)(N,\mathcal A_e)(N,Ae​). It does not require that structomorphism to be the identity. These are the conventions of the source definitions, not additional uniqueness assumptions. [Shin, SPC4.lean, lines 53–81 and 211–221]

Formalization targets

Main open goal

For every manifold MMM with the preceding hypotheses, the goal is

M≅TopS4⟹M≅DiffS4.M\cong_{\mathrm{Top}}S^4 \quad\Longrightarrow\quad M\cong_{\mathrm{Diff}}S^4.M≅Top​S4⟹M≅Diff​S4.

This is the source predicate SPC4\mathsf{SPC4}SPC4. Its conclusion asserts the existence of a diffeomorphism; it does not assert that a particular supplied homeomorphism is smooth.

Structural and literature milestones

The atlas formulation has the exact equivalence

SPC4⟺SPC4Pullback.\mathsf{SPC4}\quad\Longleftrightarrow\quad\mathsf{SPC4Pullback}.SPC4⟺SPC4Pullback.

The source supplies a proof of this equivalence without invoking Freedman's theorem or assuming the conjecture as an unconditional fact. It is a reformulation, not a solution. Its foundations include the correspondence

Structomorph⁡(G∞,M,N)≃Diff⁡∞(M,N),\operatorname{Structomorph}(\mathcal G^{\infty},M,N) \simeq \operatorname{Diff}^{\infty}(M,N),Structomorph(G∞,M,N)≃Diff∞(M,N),

where G∞\mathcal G^{\infty}G∞ is the smooth coordinate-change groupoid for the common model. [Shin, SPC4.lean, lines 334–365; Bridge.lean]

Write F4F_4F4​ for the following compact Hausdorff, boundaryless instance of Freedman's topological theorem:

M≃S4⟹M≅TopS4,M\simeq S^4\quad\Longrightarrow\quad M\cong_{\mathrm{Top}}S^4,M≃S4⟹M≅Top​S4,

where ≃\simeq≃ denotes homotopy equivalence and only topological manifold charts are assumed. This is established mathematics, but a proof in the present formal development remains a target. If SPC4Homotopy\mathsf{SPC4Homotopy}SPC4Homotopy denotes the analogous smooth conclusion from a homotopy equivalence, the relation to the main goal is recorded with its hypothesis visible:

F4⟹(SPC4⟺SPC4Homotopy).F_4\quad\Longrightarrow\quad (\mathsf{SPC4}\Longleftrightarrow\mathsf{SPC4Homotopy}).F4​⟹(SPC4⟺SPC4Homotopy).

Explicit standard-disk foundations form another track. For every m≥0m\geq0m≥0, they concern the manifold-with-boundary structure on B‾m+1\overline B^{m+1}Bm+1, its boundary set SmS^mSm, and the smooth collar

c:Sm×[0,1]⟶B‾m+1,c(u,t)=(1−t/2)u.c:S^m\times[0,1]\longrightarrow\overline B^{m+1}, \qquad c(u,t)=(1-t/2)u.c:Sm×[0,1]⟶Bm+1,c(u,t)=(1−t/2)u.

The collar is a closed embedding, has image

{z∈B‾m+1:∥z∥≥1/2},\{z\in\overline B^{m+1}:\|z\|\geq1/2\},{z∈Bm+1:∥z∥≥1/2},

and satisfies c(u,0)=uc(u,0)=uc(u,0)=u, using the boundary inclusion. Its image is a neighborhood of every boundary point in the disk. A companion interface characterizes a CkC^kCk map from a CkC^kCk manifold with corners into the disk as precisely a continuous map whose inclusion into Euclidean space is CkC^kCk. These targets concern the actual disk smooth structure. [Shin, Disk.lean, lines 1076–1141 and 1263–1318]

Topological two-disk gluing

For each integer m≥0m\geq0m≥0, let Dm+1=B‾m+1D^{m+1}=\overline B^{m+1}Dm+1=Bm+1 be the closed unit disk in Rm+1\mathbb R^{m+1}Rm+1 and let φ:Sm→Sm\varphi:S^m\to S^mφ:Sm→Sm be any homeomorphism of its boundary. The twisted double identifies the boundary point uuu in a left copy of the disk with φ(u)\varphi(u)φ(u) in a right copy. With the quotient topology, the target is

Xφ:=(DLm+1⊔DRm+1)/(uL∼φ(u)R)≅TopSm+1.X_\varphi:=\bigl(D^{m+1}_L\sqcup D^{m+1}_R\bigr)/(u_L\sim\varphi(u)_R) \quad\cong_{\mathrm{Top}}\quad S^{m+1}.Xφ​:=(DLm+1​⊔DRm+1​)/(uL​∼φ(u)R​)≅Top​Sm+1.

This statement is published as SP4Gluing.twistedSphere_homeomorphic. The theorem and its supporting continuity and injectivity lemmas have accepted Lean proofs contributed by carlok. All three accepted proofs have also been checked locally with their proved dependencies. It concerns these explicit topological quotients, not arbitrary homotopy spheres or a prescribed smooth structure.

Seam–interior smooth compatibility

For every regional chart base point, the open-bicollar and left-interior transitions are smooth in both directions. Right-interior-to-seam smoothness requires smooth φ−1\varphi^{-1}φ−1; the reverse requires smooth φ\varphiφ. The single compatibility target concerns exact overlap sources, combining four source results internally. It provides neither a global smooth-manifold instance nor smooth standardness. [Shin, Hemisphere.lean, lines 2439–3577]

Significance

A proof of the main goal would identify every smooth structure in its stated sphere class with the standard one, up to diffeomorphism. A proof of the transported-atlas equivalence instead locates the same unresolved comparison in a different formal language. The distinction matters: constructing a smooth structure by transport is not the same as identifying an arbitrary pre-existing one.

The bridge, explicit disk atlas, and stated collar properties have accepted kernel-checked Lean proofs. The clean atlas equivalence also has a proof with no admitted theorem among its axioms. The conjecture remains open, and Freedman's topological theorem remains unproved in this formal development despite its published mathematical proof.

The topological two-disk gluing result identifies the homeomorphism type of these quotients for every boundary homeomorphism and every disk dimension at least one. The accepted formalization supplies a global topological comparison for this explicit quotient. It does not resolve the comparison with a prescribed smooth structure or recognition of general smooth four-manifolds.

Four supporting algebraic tracks concern orbit coinvariants, homology dimension budgets, finite-support shift rigidity, and Laurent-polynomial positivity. Their source results arose in route-specific obstruction studies. As of 6 September 2026, all eleven theorem targets in these algebraic tracks have accepted Lean proofs. The five additional formal proofs were contributed by wamlart: orbit augmentation, region homology budgets, two-corner homology budgets, the Laurent mass threshold, and mass-two positivity. No theorem currently connects their completion to a proof or disproof of SPC4\mathsf{SPC4}SPC4. They are exploratory tools, not established milestones in a proof of the main goal.

Difficulty

A homeomorphism can transport the standard atlas, but that observation does not compare the transported atlas with the one already specified on the manifold. Treating those two atlases as equal would remove the central mathematical question by changing its hypotheses.

Likewise, topological recognition does not supply a smooth recognition theorem. Standard disk and collar constructions establish local models; they do not establish a smooth gluing or recognition theorem for an arbitrary prescribed smooth structure, a recognition theorem for arbitrary smooth balls, or a smooth Schoenflies theorem. The missing global comparison cannot be replaced by successful finite algebraic tests or by constructing a standard local chart.

Formalization scope

The sphere goal quantifies over Type in universe zero, exactly as in the source. It uses real four-dimensional Euclidean chart models, compactness, the Hausdorff condition, and smoothness of order ∞\infty∞. Boundaryless manifolds are built into that model. No orientation, fixed parametrization, or identity-map uniqueness is imposed.

The geometric foundations use charted spaces, structure groupoids, models with corners, homotopy equivalences and diffeomorphisms. Disk results include every m≥0m\geq0m≥0, so their dimensions are m+1≥1m+1\geq1m+1≥1. The boundary-set identification does not by itself construct a general induced smooth boundary structure. Nor is smoothness asserted for a radial clamp across its nonsmooth locus.

The separate source assertion SPC4Ball is not treated as equivalent to the sphere goal: the required formal boundary, capping and gluing bridge is absent. The transported-annulus product diffeomorphism is not a current target; its chart instances serve only as constructor support. No unconditional implication is taken through the source's admitted Freedman declaration. Gaussian coupling, transport defects, partition incidence and merge-score results remain outside this mission because no mathematical dependency on them has been established.

Selected references

  • R. İnanç Baykur, Robion C. Kirby and Daniel Ruberman, eds., K3 — A New Problem List in Low-Dimensional Topology, Mathematical Surveys and Monographs 295, American Mathematical Society, 2026, Problem 4.1, pp. 191–192. Author PDF.

  • Michael Hartley Freedman, The topology of four-dimensional manifolds, Journal of Differential Geometry 17 (1982), 357–453, Theorem 1.6, p. 371. DOI; primary-article scan.

  • Stephen Smale, Generalized Poincaré's Conjecture in Dimensions Greater Than Four, Annals of Mathematics 74 (1961), 391–406, Theorem A. DOI; primary-article scan.

  • Ryan Shin, SPC4.lean, Bridge.lean and Disk.lean, unpublished source files, 2026; no public manuscript URL available. SHA-256, respectively: b17fdb932034e5211d0db8171c08e2b3a182016bceaecdd2deb49c39d6bfd5cc, e8ea6b66f6bd675ca272e862e0825ab2db1f8bb792eaffe1b9e8f5d89024d302, 889a9eccf9d2350aee7051ab7b6895e565f9f1a0c84e7120fb45c15acae0097e.

  • Ryan Shin, Hemisphere.lean, unpublished Lean source file, 2026, declaration twistedSphereHomeoSphere; source SHA-256 c48843d2c4ec6987acfd7f7ab3a92bfed990376206142e74712795b4e9399828. Published topological two-disk gluing target; the recovered local construction is checked; the accepted proof and its two supporting lemmas were contributed by carlok.

60 thms5 active usersReviewed
Group Theory·Captain: Lucas

Faithfulness of the Burau representation of B4Research Paper

Motivation

In 1935 Werner Burau attached to every braid on nnn strands a matrix over the ring of Laurent polynomials Z[t,t−1]\mathbb{Z}[t,t^{-1}]Z[t,t−1]. The resulting homomorphism ρn:Bn→GLn(Z[t,t−1])\rho_n : B_n \to \mathrm{GL}_n(\mathbb{Z}[t,t^{-1}])ρn​:Bn​→GLn​(Z[t,t−1]) is the oldest and most studied linear representation of the braid group, and whether it is faithful — whether a nontrivial braid can act as the identity matrix — became one of the best known questions about braid groups.

The history is short and sharp:

  • 1969 — Magnus and Peluso prove that ρ3\rho_3ρ3​ is faithful, by a direct algebraic computation.
  • 1991 — Moody proves ρn\rho_nρn​ is not faithful for n≥9n \ge 9n≥9.
  • 1993 — Long and Paton improve this to n≥6n \ge 6n≥6.
  • 1999 — Bigelow settles n=5n = 5n=5: ρ5\rho_5ρ5​ is not faithful.
  • This left exactly one open case, n=4n = 4n=4, which appears as Question 3.1 in Margalit's problem list for mapping class groups.
  • 2026 — Bharathram, Birman and Brendle prove that ρ4\rho_4ρ4​ is faithful (arXiv:2607.05283), closing the last case.

Setting

Let n≥1n \ge 1n≥1. The braid group BnB_nBn​ is taken here in Artin's presentation: generators σ1,…,σn−1\sigma_1,\dots,\sigma_{n-1}σ1​,…,σn−1​ subject to

σiσj=σjσi(∣i−j∣≥2),σiσi+1σi=σi+1σiσi+1.\sigma_i\sigma_j = \sigma_j\sigma_i \quad (|i-j| \ge 2), \qquad \sigma_i\sigma_{i+1}\sigma_i = \sigma_{i+1}\sigma_i\sigma_{i+1}.σi​σj​=σj​σi​(∣i−j∣≥2),σi​σi+1​σi​=σi+1​σi​σi+1​.

Let R=Z[t,t−1]R = \mathbb{Z}[t,t^{-1}]R=Z[t,t−1]. The unreduced Burau representation is the homomorphism

ρn:Bn⟶GLn(R),σi⟼Ii−1⊕(1−tt10)⊕In−i−1,\rho_n : B_n \longrightarrow \mathrm{GL}_n(R), \qquad \sigma_i \longmapsto I_{i-1} \oplus \begin{pmatrix} 1-t & t \\ 1 & 0\end{pmatrix} \oplus I_{n-i-1},ρn​:Bn​⟶GLn​(R),σi​⟼Ii−1​⊕(1−t1​t0​)⊕In−i−1​,

i.e. the identity matrix altered only in the two rows and columns iii, i+1i+1i+1. That these matrices satisfy the two families of braid relations — so that ρn\rho_nρn​ is well defined — is proved in the mission's definition file, together with the invertibility of each generator matrix (its inverse is the identity altered by the block (01t−11−t−1)\begin{pmatrix} 0 & 1 \\ t^{-1} & 1-t^{-1}\end{pmatrix}(0t−1​11−t−1​)).

Equivalently, ρn\rho_nρn​ is the action of the mapping class group of the nnn-punctured disk DnD_nDn​ on the relative homology H1(Dn~,{p~∗})H_1(\widetilde{D_n}, \{\tilde p_*\})H1​(Dn​​,{p~​∗​}) of the infinite cyclic cover determined by total winding number; this is the description used throughout the source paper.

A representation is faithful when it is injective.

Target

The goal of the mission is the Main Theorem of the paper:

ρ4:B4⟶GL4(Z[t,t−1])  is injective.\rho_4 : B_4 \longrightarrow \mathrm{GL}_4(\mathbb{Z}[t,t^{-1}]) \ \text{ is injective.}ρ4​:B4​⟶GL4​(Z[t,t−1])  is injective.

The milestones are three supporting results, each of which can be attacked independently:

  1. Theorem 4.1 (Magnus–Peluso). ρ3\rho_3ρ3​ is injective. The paper gives a new topological proof of this classical statement, and the same argument is the model for the four-strand case.
  2. Observation 2.1. If a braid Φ∈Bn\Phi \in B_nΦ∈Bn​ satisfies ρn(Φ)=I\rho_n(\Phi) = Iρn​(Φ)=I, then its image under the standard inclusion Bn↪Bn+1B_n \hookrightarrow B_{n+1}Bn​↪Bn+1​ (add one unbraided strand) satisfies ρn+1(ι(Φ))=I\rho_{n+1}(\iota(\Phi)) = Iρn+1​(ι(Φ))=I. The paper uses this to move a four-strand braid into B5B_5B5​, where a parity obstruction can be applied.
  3. Long's criterion ([Long 1986, Theorem 2.2], quoted in Section 1 of the paper). If N⊴BnN \trianglelefteq B_nN⊴Bn​ is nontrivial and not contained in the centre, and ρn\rho_nρn​ is injective on NNN, then ρn\rho_nρn​ is injective. This is what reduces the Main Theorem to faithfulness on the Brunnian subgroup Brun4\mathrm{Brun}_4Brun4​.

Significance

Faithfulness of ρ4\rho_4ρ4​ closes the classification of the faithful Burau representations: ρn\rho_nρn​ is faithful exactly for n≤4n \le 4n≤4. It immediately gives faithfulness of the Jones representation of B4B_4B4​ (Corollary 1.1 of the paper), since the Jones representation contains the reduced Burau representation as a summand. Beyond the statement itself, the kernel and the image of ρn\rho_nρn​ for n≥5n \ge 5n≥5 remain poorly understood, and the paper's disk-sequence and parity technology is proposed by its authors as a tool for that problem.

For formalization, essentially nothing of this is machine-checked today: Mathlib has neither braid groups nor the Burau representation. This mission puts in place a checked definition of ρn\rho_nρn​ over Z[t,t−1]\mathbb{Z}[t,t^{-1}]Z[t,t−1] (including well-definedness and invertibility), and then asks for the mathematics. Even the three-strand case — Magnus–Peluso, known since 1969 — is not formalized anywhere, and it is the natural first target.

Difficulty

The obvious approach fails in both directions. One cannot simply compute: a braid in the kernel would have to be found or excluded among infinitely many words, and no normal form for B4B_4B4​ turns injectivity of ρ4\rho_4ρ4​ into a finite check. Nor can one argue by a free-subgroup / ping-pong pattern, which is how non-faithfulness is proved for n≥5n \ge 5n≥5.

The source argument is topological. To a braid Φ\PhiΦ one associates the arc β=(β∗3)Φ\beta = (\beta_*^3)\Phiβ=(β∗3​)Φ and the sequence of punctured disks cut out by its intersections with a fixed arc α\alphaα; the Moody polynomial M(α,β)∈Z[t,t−1]M(\alpha,\beta) \in \mathbb{Z}[t,t^{-1}]M(α,β)∈Z[t,t−1] then obstructs membership in the kernel provided no cancellation occurs among its monomials. Three-strand braids always satisfy the relevant parity condition; four-strand braids do not, and the paper repairs this by pushing a point-pushing braid Φ∈K4\Phi \in K_4Φ∈K4​ into B5B_5B5​ and applying Moody's theorem there. A complete formalization therefore needs curves on punctured disks, minimal position, and the Birman exact sequence — none of which exist in Mathlib. Contributions that build any of that infrastructure are as welcome as contributions to the statements themselves.

Formalization scope

Conventions fixed by the Lean development:

  1. BnB_nBn​ is the abstract group given by Artin's presentation, with generators indexed by Fin(n−1)\mathrm{Fin}(n-1)Fin(n−1) using truncated subtraction; the generator of index iii is σi+1\sigma_{i+1}σi+1​. This is the already-published definition reused by the mission, so results proved here interoperate with other braid-group missions.
  2. The representation is the unreduced Burau representation, of size n×nn \times nn×n, not the reduced (n−1)(n-1)(n−1)-dimensional one; the variable is written ttt and the coefficient ring is Z[t,t−1]\mathbb{Z}[t,t^{-1}]Z[t,t−1].
  3. Faithfulness is stated as injectivity of the group homomorphism, not as triviality of the kernel on some subgroup, and it is the genuine homomorphism out of the presented group: the braid relations are verified for the Burau matrices in the definition file, so no statement here is vacuous or conditional on well-definedness.
  4. Long's criterion is stated for all nnn; for n≤2n \le 2n≤2 its noncentrality hypothesis cannot be satisfied, so its content is the case n≥3n \ge 3n≥3 that the paper uses.

A complete development will additionally need: point-pushing subgroups and the Brunnian group Brun4\mathrm{Brun}_4Brun4​, the Moody polynomial of a pair of arcs, and winding-number sequences. These are not yet formalized and are deliberately not part of the current statements; proposals for faithful formalizations of them are welcome in the mission discussion.

Selected references

  • V. Bharathram, J. S. Birman, T. E. Brendle, The Burau representation is faithful for n = 4, 2026, arXiv:2607.05283.
  • W. Magnus, A. Peluso, On a theorem of V. I. Arnold, Comm. Pure Appl. Math. 22 (1969), 683–692, DOI:10.1002/cpa.3160220508.
  • D. D. Long, A note on the normal subgroups of mapping class groups, Math. Proc. Cambridge Philos. Soc. 99 (1986), 79–87, DOI:10.1017/S0305004100063969.
  • J. A. Moody, The Burau representation of the braid group BnB_nBn​ is unfaithful for large nnn, Bull. Amer. Math. Soc. 25 (1991), 379–384, DOI:10.1090/S0273-0979-1991-16080-5.
  • D. D. Long, M. Paton, The Burau representation is not faithful for n≥6n \ge 6n≥6, Topology 32 (1993), 439–447, DOI:10.1016/0040-9383(93)90030-Y.
  • S. Bigelow, The Burau representation is not faithful for n=5n = 5n=5, Geom. Topol. 3 (1999), 397–404, DOI:10.2140/gt.1999.3.397.
15 thms3 active usersReviewed
Differential Geometry·Captain: xuanji

Strong Whitney embedding in dimension 2nResearch Paper

Motivation: an intrinsic manifold in a fixed Euclidean space

A smooth manifold is a space that can be described locally by real coordinates, even when no single coordinate chart describes the whole space. Differential geometry works with these local descriptions, whereas an embedding realizes the entire space inside one Euclidean space without losing either its topology or its infinitesimal geometry. The strong Whitney embedding theorem supplies a dimension bound depending only on the dimension of the manifold. This mission targets the precise version selected by LeanEval v1, rather than a substitute formulation.

The benchmark attributes the strong result to Hassler Whitney's 1944 paper and distinguishes it from the earlier bound of 2n+12n+12n+1. The result is a known mathematical theorem; the remaining task here is its formal proof in Lean. The exact benchmark declaration is authoritative for the target and its hypotheses, not a reconstruction from the historical literature (source and attribution).

Setting: topology, smoothness, and the differential

Let nnn be a natural number satisfying 1≤n1\le n1≤n. Let MMM carry a topology and a smooth atlas modeled on Rn\mathbb R^nRn, with the usual model having no boundary. The topology is Hausdorff: distinct points admit disjoint neighborhoods. It is second countable: there is a countable collection of open sets from which every open set can be assembled as a union. These are explicit hypotheses, alongside the chosen charted-space and smooth-manifold structures, in the Lean statement.

A topological embedding is a map that is a homeomorphism onto its image, where the image has the subspace topology inherited from the codomain. An immersion has an injective differential at every point. For a smooth map eee, write dexd e_xdex​ for the induced linear map on tangent spaces at xxx. These are separate requirements: the target asks for global topological embedding and pointwise injectivity of the differential together, as well as infinite differentiability. Their precise Lean meanings are the existing Mathlib predicates used directly by the benchmark, not new mission-specific definitions.

Formalization target: the single root theorem

For every n≥1n\ge1n≥1 and every MMM with the structures and hypotheses just stated, establish

∃e:M⟶R2n,e∈C∞(M,R2n) ∧ e is a topological embedding ∧ ∀x∈M, dex is injective.\exists e:M\longrightarrow\mathbb R^{2n},\qquad e\in C^\infty(M,\mathbb R^{2n}) \ \land\ e\text{ is a topological embedding} \ \land\ \forall x\in M,\ d e_x\text{ is injective}.∃e:M⟶R2n,e∈C∞(M,R2n) ∧ e is a topological embedding ∧ ∀x∈M, dex​ is injective.

The codomain has dimension exactly 2n2n2n. The quantifier ranges over all such manifolds, including noncompact ones. There is exactly one goal theorem and no auxiliary theorem items, definition items, or milestones. The declaration is LeanEval.Geometry.WhitneyEmbeddingProblem.whitney_embedding, with the binders and conclusion preserved from the benchmark source.

Significance: the full theorem rather than an easier restriction

The result realizes the given manifold in a Euclidean space with a uniform dimension bound. Its value in this formulation is the simultaneous control of topology, smoothness, and the differential, without a compactness assumption. Replacing the image-topology condition with mere injectivity would omit part of the requested conclusion; replacing 2n2n2n with an unspecified dimension would omit the quantitative constraint. Both distinctions are explicit in the benchmark's explanation.

A completed formalization would supply a reusable strong embedding theorem on top of Mathlib's manifold language. This is a long-term infrastructure task, not a claim that a short proof is available. The September 5, 2026 LeanEval v1 snapshot supplied for this task records no accepted benchmark credit for this target. That dated benchmark status is not a claim about all formalization projects, and preparing an open theorem statement does not establish the theorem or earn benchmark credit.

Difficulty: the dimension bound and the noncompact scope

The existing compact embedding result discussed by the benchmark provides an embedding into some finite-dimensional Euclidean space. That does not settle the present goal: it assumes compactness and does not supply the 2n2n2n bound. Consequently, simply invoking that result cannot discharge the unrestricted benchmark statement. The source identifies substantial differential-topological infrastructure behind the strong theorem; this proposal does not advertise an easy proof or prescribe a decomposition (benchmark discussion).

All positive dimensions remain in scope, including n=1n=1n=1 and n=2n=2n=2. Noncompactness is not a later extension or optional strengthening. The absence of an assumption must not be replaced by an implicit restriction in a new definition or an easier surrogate theorem.

Formalization scope: unchanged Mathlib predicates

The source model is EuclideanSpace ℝ (Fin n), and the target is EuclideanSpace ℝ (Fin (2 * n)). Smoothness is expressed by ContMDiff (𝓡 n) (𝓡 (2 * n)) ∞ e; the other two conjuncts are IsEmbedding e and pointwise Function.Injective of mfderiv. The type MMM remains universe-polymorphic. No compactness, connectedness, orientability, or nonemptiness hypothesis is added. The empty manifold is included; dimension zero is excluded. Neither properness nor closedness of the image is demanded by the conclusion (exact declaration).

Mathlib already provides the vocabulary needed to state the goal: Euclidean spaces, charts, manifold smoothness, topological embeddings, and manifold derivatives. No custom definition item is necessary. Future proof work may develop reusable infrastructure, but this draft contains only the root theorem and intentionally imposes no supporting targets. A proof must establish that exact statement, not the compact-only, immersion-only, or weak 2n+12n+12n+1 alternative.

Selected references

  • LeanEval contributors, Whitney embedding theorem (strong form, sharp dimension 2n), LeanEval v1 source declaration and manifest, statement revision 1, pinned source and manifest. These specify the exact formal target.
  • H. Whitney, The self-intersections of a smooth n-manifold in 2n-space, Annals of Mathematics (2) 45 (1944), 220–246, DOI. Historical attribution as recorded in the LeanEval manifest; no alternate statement from this reference replaces the benchmark goal.
16 thms3 active usersReviewed
Differential GeometryNumber Theory·Captain: t4v1

Thurston's Question 23: rational relations among hyperbolic volumesOpen Problem

Motivation

In the last of the twenty-four questions that closed his 1982 survey Three-dimensional manifolds, Kleinian groups and hyperbolic geometry (Bull. Amer. Math. Soc. 6 (1982), 357–381), Thurston asked to "show that volumes of hyperbolic 333-manifolds are not all rationally related" (p. 380). Twenty-two of the twenty-four have since been answered — geometrization by Perelman, tameness by Agol and by Calegari–Gabai, the ending lamination conjecture by Brock–Canary–Minsky, virtual fibering by Agol — and this one is among the two that remain open.

Some rational relations are forced, and for a trivial reason: a degree nnn cover of a hyperbolic 333-manifold has nnn times its volume, so any two commensurable manifolds have rationally related volumes. The question, which remains open, is whether every rational relation arises that way — equivalently, whether some two hyperbolic 333-manifolds have irrational volume ratio. Remarkably, not a single such pair is known.

Setting

The bundle fixes the meaning of every term. Hyperbolic 333-space is the upper half-space {(x,y,z):z>0}\{(x,y,z) : z > 0\}{(x,y,z):z>0}. Its volume is Lebesgue measure with density z−3z^{-3}z−3 — the Riemannian volume of the metric (dx2+dy2+dz2)/z2(dx^2+dy^2+dz^2)/z^2(dx2+dy2+dz2)/z2 written out, so that no Riemannian machinery is required. The hyperbolic distance is given by its closed formula

cosh⁡d(p,q)  =  1+∣p−q∣22 p3 q3.\cosh d(p,q) \;=\; 1 + \frac{|p-q|^2}{2\,p_3\,q_3}.coshd(p,q)=1+2p3​q3​∣p−q∣2​.

A Kleinian action is a free, properly discontinuous action by hyperbolic isometries; the quotient is a complete hyperbolic 333-manifold, discreteness and torsion freeness being consequences rather than hypotheses. The volume of the quotient is the measure of a fundamental domain, in the sense of Mathlib's MeasureTheory.IsFundamentalDomain, and the set of volumes collects those that are finite and positive.

Two conventions are stated rather than derived, and are worth flagging. Isometries are not required to preserve orientation, so the set of volumes also contains those of non-orientable quotients; this enlarges the set but not its Q\mathbb{Q}Q-span, so neither goal is affected. And preservation of the hyperbolic volume is a field of the structure rather than a consequence of preserving the distance: it holds for every hyperbolic isometry, but deriving it amounts to classifying Isom(H3)\mathrm{Isom}(\mathbb{H}^3)Isom(H3), which is not the subject of this mission.

Formalization targets

The goal is that the volumes are not all rationally related: there are two of them, vvv and www, with v≠qwv \neq q wv=qw for every rational qqq.

Two milestones support it. The first is that passing to a subgroup of index nnn multiplies the volume by nnn, a fundamental domain for the subgroup being the union of nnn translates of one for the whole group; this is the source of every known rational relation, and it is why the question is phrased as it is. The second is that the set of volumes is nonempty — that some finite-volume hyperbolic 333-manifold exists at all — without which the goal would be vacuously false rather than open.

A stronger form of the question, that the Q\mathbb{Q}Q-span of the set of volumes is infinite dimensional, is also stated.

Significance

The question is a geometric statement whose difficulty is arithmetic. For the Bianchi groups of an imaginary quadratic field FFF, Humbert's formula gives the covolume as ∣δF∣3/2ζF(2)/4π2|\delta_F|^{3/2}\zeta_F(2)/4\pi^2∣δF​∣3/2ζF​(2)/4π2, so the ratio of two such volumes is, up to explicit algebraic factors, a ratio of Dedekind zeta values at 222; and Neumann and Yang showed that the Bloch invariant of a hyperbolic 333-manifold lies in a subgroup of finite Q\mathbb{Q}Q-rank determined by its invariant trace field, so that manifolds sharing an invariant trace field with a single complex place, such as an imaginary quadratic one, have rationally related volumes. Producing one irrational ratio therefore means separating two such transcendentals — a statement of the same order of difficulty as the irrationality of ζ(5)\zeta(5)ζ(5). The value of formalizing the question is not that it will be closed, but that its statement, and the elementary relations that make its naive form false, are pinned down exactly.

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Algebraic Topology·Captain: Lucas

Smale's question: the homotopy type of Diff(S⁴)Open Problem

Motivation

The diffeomorphism group Diff(M)\mathrm{Diff}(M)Diff(M) of a closed smooth manifold MMM, topologized so that two diffeomorphisms are close when they and all their derivatives are uniformly close, is a basic invariant of the smooth structure of MMM. Its set of path components π0 Diff(M)\pi_0\,\mathrm{Diff}(M)π0​Diff(M) is the group of isotopy classes of diffeomorphisms (the smooth mapping class group), and its higher homotopy groups classify smooth fibre bundles with fibre MMM. For spheres, the natural comparison is with the orthogonal group O(n+1)O(n+1)O(n+1) of isometries of the round metric, which sits inside Diff(Sn)\mathrm{Diff}(S^n)Diff(Sn).

S. Smale asked how far Diff(Sn)\mathrm{Diff}(S^n)Diff(Sn) is from O(n+1)O(n+1)O(n+1). The question was settled positively in dimensions n≤3n \le 3n≤3 and has been studied extensively in dimensions n≥5n \ge 5n≥5, where surgery theory and pseudo-isotopy theory apply. Dimension 444 is the remaining case, and it is where the least is known. The question is recorded on the Open Problem Garden (problem page) with importance "Outstanding".

Timeline.

  • 1959 — S. Smale: Diff(S2)≃O(3)\mathrm{Diff}(S^2) \simeq O(3)Diff(S2)≃O(3).
  • 1963 — M. Kervaire and J. Milnor compute the groups Θn\Theta_nΘn​ of homotopy spheres; combined with Cerf's pseudo-isotopy theorem this computes π0 Diff(Sn)\pi_0\,\mathrm{Diff}(S^n)π0​Diff(Sn) for many n≥5n \ge 5n≥5 (for example π0 Diff+(S6)≅Θ7≅Z/28\pi_0\,\mathrm{Diff}^+(S^6) \cong \Theta_7 \cong \mathbb Z/28π0​Diff+(S6)≅Θ7​≅Z/28).
  • 1970s — the Cerf–Morlet comparison theorem Diff(Dn)≃Ωn+1(PLn/On)\mathrm{Diff}(D^n) \simeq \Omega^{n+1}(PL_n/O_n)Diff(Dn)≃Ωn+1(PLn​/On​) (Kirby–Siebenmann, Foundational Essays).
  • 1978 — F.T. Farrell and W.C. Hsiang compute πi Diff(Dn)⊗Q\pi_i\,\mathrm{Diff}(D^n)\otimes\mathbb Qπi​Diff(Dn)⊗Q in a stable range of degrees for large nnn.
  • 1983 — A. Hatcher: Diff(S3)≃O(4)\mathrm{Diff}(S^3) \simeq O(4)Diff(S3)≃O(4) (the Smale conjecture).
  • 2007 — R. Budney: Diff(D4)\mathrm{Diff}(D^4)Diff(D4) is a 555-fold loop space, via little cubes acting on spaces of long knots.
  • 2018 — T. Watanabe: π∗ Diff(D4)⊗Q≠0\pi_*\,\mathrm{Diff}(D^4)\otimes\mathbb Q \ne 0π∗​Diff(D4)⊗Q=0; the 444-dimensional Smale conjecture is false (arXiv:1812.02448).

Whether Diff(D4)\mathrm{Diff}(D^4)Diff(D4) is connected is still unknown.

Setting

Write Rn\mathbb R^nRn for Euclidean space with the Euclidean norm, DnD^nDn for the closed unit ball and Sn⊂Rn+1S^n \subset \mathbb R^{n+1}Sn⊂Rn+1 for the round unit sphere.

  • Diff(Dn)\mathrm{Diff}(D^n)Diff(Dn) is the group of diffeomorphisms of the nnn-ball rel boundary. Concretely it is the group of smooth diffeomorphisms f ⁣:Rn→Rnf\colon \mathbb R^n \to \mathbb R^nf:Rn→Rn with f(x)=xf(x) = xf(x)=x whenever ∥x∥≥1\|x\| \ge 1∥x∥≥1. Two such maps are close when their kkk-th derivatives are uniformly close for every kkk (the C∞C^\inftyC∞ topology). The base point is the identity.
  • Diff(Sn)\mathrm{Diff}(S^n)Diff(Sn) is the group of all smooth diffeomorphisms of SnS^nSn (orientation-preserving or orientation-reversing), with the C∞C^\inftyC∞ topology. Derivatives are measured through the degree-one homogeneous extension x↦∥x∥ f(x/∥x∥)x \mapsto \|x\|\, f(x/\|x\|)x↦∥x∥f(x/∥x∥), taken on the sphere.
  • O(n)O(n)O(n) is the group of real orthogonal n×nn\times nn×n matrices with the matrix topology.
  • X≃YX \simeq YX≃Y means that XXX and YYY are homotopy equivalent. π0X\pi_0 Xπ0​X is the set of path components, and πi(X,x)\pi_i(X,x)πi​(X,x) is the iii-th homotopy group. Ωk(Y,y)\Omega^k(Y,y)Ωk(Y,y) is the kkk-fold loop space, the space of maps [0,1]k→Y[0,1]^k \to Y[0,1]k→Y sending the boundary of the cube to yyy.

The source states that Diff(S4)≃O(5)×Diff(D4)\mathrm{Diff}(S^4) \simeq O(5) \times \mathrm{Diff}(D^4)Diff(S4)≃O(5)×Diff(D4), so the homotopy type of Diff(S4)\mathrm{Diff}(S^4)Diff(S4) is determined by that of Diff(D4)\mathrm{Diff}(D^4)Diff(D4).

Formalization targets

Goal: connectivity of Diff(D4)\mathrm{Diff}(D^4)Diff(D4)

π0 Diff(D4)=0,i.e. Diff(D4) is path-connected.\pi_0\,\mathrm{Diff}(D^4) = 0, \qquad\text{i.e. } \mathrm{Diff}(D^4) \text{ is path-connected.}π0​Diff(D4)=0,i.e. Diff(D4) is path-connected.

The source asks to "determine some (any?) homotopy or homology groups of Diff(D4)\mathrm{Diff}(D^4)Diff(D4)" and singles out connectivity as unknown. The goal is the yes/no question for π0\pi_0π0​. It can be settled either way: a proof shows that every diffeomorphism of D4D^4D4 rel boundary is isotopic to the identity, and a disproof exhibits one that is not.

Milestones

  1. Diff(S4)≃O(5)×Diff(D4)\mathrm{Diff}(S^4) \simeq O(5)\times\mathrm{Diff}(D^4)Diff(S4)≃O(5)×Diff(D4) (problem statement).
  2. Diff(D4)≃Ω5(Y,y)\mathrm{Diff}(D^4) \simeq \Omega^5(Y,y)Diff(D4)≃Ω5(Y,y) for some pointed space (Y,y)(Y,y)(Y,y) (Cerf–Morlet, Budney).
  3. Diff(D4)\mathrm{Diff}(D^4)Diff(D4) is not contractible (Watanabe).
  4. Diff(S2)≃O(3)\mathrm{Diff}(S^2) \simeq O(3)Diff(S2)≃O(3) (Smale).
  5. Diff(S3)≃O(4)\mathrm{Diff}(S^3) \simeq O(4)Diff(S3)≃O(4) (Hatcher).
  6. ∣π0 Diff(S6)∣=56|\pi_0\,\mathrm{Diff}(S^6)| = 56∣π0​Diff(S6)∣=56 (Kervaire–Milnor and Cerf).
  7. For 2≤i<min⁡{n−43,n−72}2 \le i < \min\{\tfrac{n-4}{3}, \tfrac{n-7}{2}\}2≤i<min{3n−4​,2n−7​}: πi Diff(Dn)⊗Q≅Q\pi_i\,\mathrm{Diff}(D^n)\otimes\mathbb Q \cong \mathbb Qπi​Diff(Dn)⊗Q≅Q if nnn is odd and 4∣i+14 \mid i+14∣i+1, and 000 otherwise (Farrell–Hsiang).

Significance

The result itself. A positive answer would mean π0 Diff(S4)≅Z/2\pi_0\,\mathrm{Diff}(S^4) \cong \mathbb Z/2π0​Diff(S4)≅Z/2, detected by orientation alone, matching dimensions 111, 222 and 333. A negative answer would give an exotic diffeomorphism of S4S^4S4: one that is topologically isotopic to the identity (by the Alexander trick) but not smoothly isotopic. By the Cerf–Morlet theorem, π0 Diff(D4)≅π5(PL4/O4)\pi_0\,\mathrm{Diff}(D^4) \cong \pi_5(PL_4/O_4)π0​Diff(D4)≅π5​(PL4​/O4​), so the question is equivalent to a question about the homotopy of PL4/O4PL_4/O_4PL4​/O4​, the space controlling smoothings of PL 444-manifolds. The source lists the smooth 444-dimensional Schoenflies problem as a related problem.

Formalizing it. No part of this theory is currently formalized in Lean or Mathlib: there is no C∞C^\inftyC∞ topology on diffeomorphism groups and no known homotopy equivalence involving one. The milestones are classical theorems (Smale 1959, Hatcher 1983, Kervaire–Milnor 1963, Farrell–Hsiang 1978, Watanabe 2018). Formalizing any of them is new work, independent of the open goal.

Difficulty

In dimensions ≥5\ge 5≥5, π0 Diff(Dn)\pi_0\,\mathrm{Diff}(D^n)π0​Diff(Dn) is computed by combining Cerf's pseudo-isotopy theorem with the hhh-cobordism theorem. Both rely on the Whitney trick, which fails in dimension 444. In dimension 444 one also cannot reduce to a lower-dimensional problem as Smale and Hatcher did. The known invariants that detect non-trivial elements of π∗ Diff(D4)\pi_*\,\mathrm{Diff}(D^4)π∗​Diff(D4) (Watanabe's configuration-space integrals) are rational and live in positive degrees, so they say nothing about π0\pi_0π0​. Smale's and Hatcher's arguments for n=2,3n = 2, 3n=2,3 rely on understanding spaces of embedded spheres in SnS^nSn of one lower dimension; the corresponding spaces of 333-spheres in S4S^4S4 are not understood, so those arguments do not carry over.

Formalization scope

All statements import the single definition file SmaleDiffS4_Basic and live in the namespace SmaleDiffS4.

  • DiffDisk n is the subtype of Mathlib's Diffeomorph 𝓘(ℝ, ℝⁿ) 𝓘(ℝ, ℝⁿ) ℝⁿ ℝⁿ ∞ (smooth = C^∞) of maps fixing every point of norm ≥1\ge 1≥1. Its topology is induced by the family of iterated derivatives iteratedFDeriv ℝ k f, k∈Nk \in \mathbb Nk∈N, each with the topology of uniform convergence on Rn\mathbb R^nRn. This "identity outside the open ball" model is the standard model of Diff(Dn rel ∂)\mathrm{Diff}(D^n \text{ rel } \partial)Diff(Dn rel ∂) and is homotopy equivalent to the "identity on the boundary" and "identity near the boundary" variants.
  • DiffSphere n is Mathlib's Diffeomorph (𝓡 n) (𝓡 n) (sphere 0 1) (sphere 0 1) ∞ on the unit sphere of Rn+1\mathbb R^{n+1}Rn+1. Its topology is induced by the iterated derivatives of the radial extension, restricted to the sphere and uniformly topologized.
  • OrthGroup n is Matrix.orthogonalGroup (Fin n) ℝ with the subspace topology.
  • Homotopy equivalence is ContinuousMap.HomotopyEquiv. Ω5\Omega^5Ω5 is GenLoop (Fin 5) Y y, π0\pi_0π0​ is ZerothHomotopy, and πi\pi_iπi​ is HomotopyGroup (Fin i). πi⊗Q\pi_i\otimes\mathbb Qπi​⊗Q is TensorProduct ℤ ℚ (Additive π_i), and "≅Q\cong\mathbb Q≅Q" is stated as Q\mathbb QQ-rank 111.
  • The Farrell–Hsiang milestone covers only i≥2i \ge 2i≥2, where πi\pi_iπi​ is abelian in Mathlib. It includes the parity hypothesis "nnn odd" of the original theorem, which is lost in the source page's rendering.

A trivializing formalization is ruled out: the topology is the genuine C∞C^\inftyC∞ topology rather than the discrete or indiscrete one, and the goal is not vacuous because DiffDisk 4 is nonempty (it contains the identity).

A complete development needs reusable infrastructure: the C∞C^\inftyC∞ topology and topological-group structure on diffeomorphism groups, isotopy extension and fibration theorems (Cerf–Palais), restriction to a disc, and the Alexander trick. Contributions of this infrastructure as separate theorems are welcome.

Selected references

  • Open Problem Garden, What is the homotopy type of the group of diffeomorphisms of the 4-sphere? (posted 2009). http://www.openproblemgarden.org/op/what_is_the_homotopy_type_of_the_group_of_diffeomorphisms_of_the_4_sphere
  • S. Smale, Diffeomorphisms of the 2-sphere, Proc. Amer. Math. Soc. 10 (1959), 621–626. https://doi.org/10.1090/S0002-9939-1959-0112149-8
  • M. Kervaire, J. Milnor, Groups of homotopy spheres I, Ann. of Math. 77 (1963), 504–537. https://doi.org/10.2307/1970128
  • R. Kirby, L. Siebenmann, Foundational Essays on Topological Manifolds, Smoothings, and Triangulations, Princeton University Press, 1977.
  • F.T. Farrell, W.C. Hsiang, On the rational homotopy groups of the diffeomorphism groups of discs, spheres and aspherical manifolds, Proc. Sympos. Pure Math. 32 (1978), 403–415.
  • A. Hatcher, A proof of a Smale conjecture, Diff(S3)≃O(4)\mathrm{Diff}(S^3)\simeq O(4)Diff(S3)≃O(4), Ann. of Math. (2) 117 (1983), 553–607. https://doi.org/10.2307/2007035
  • R. Budney, Little cubes and long knots, Topology 46 (2007), 1–27. https://arxiv.org/abs/math/0309427
  • T. Watanabe, Some exotic nontrivial elements of the rational homotopy groups of Diff(S4)\mathrm{Diff}(S^4)Diff(S4), 2018. https://arxiv.org/abs/1812.02448
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Dynamical Systems·Captain: Lucas

Building Anosov flows on 3-manifolds (Béguin–Bonatti–Yu)Research Paper

Motivation

Anosov flows are the model of uniformly hyperbolic, chaotic continuous-time dynamics: a nonsingular vector field XXX on a closed manifold MMM is Anosov when the tangent bundle splits as TM=Es⊕RX⊕EuTM=E^s\oplus\mathbb RX\oplus E^uTM=Es⊕RX⊕Eu, with EsE^sEs uniformly contracted and EuE^uEu uniformly expanded by the derivative of the flow. They are structurally stable, so one can hope to classify them up to topological equivalence. In dimension three this classification is far from complete: it is not known which closed 3-manifolds carry Anosov flows, nor how many inequivalent Anosov flows a given manifold can carry.

The classical examples — suspensions of hyperbolic toral automorphisms and geodesic flows of hyperbolic surfaces — are rigid (Plante; Ghys). Non-algebraic examples were built by Franks–Williams (a nontransitive Anosov flow, 1980), Handel–Thurston, Goodman, Fried, Bonatti–Langevin, Fenley, Barbot and others. Several of these examples glue together neighbourhoods of hyperbolic sets along their boundaries. Béguin, Bonatti and Yu (Geom. Topol. 21 (2017)) turned this into a general theory, and used it to answer questions of Katok and of Barbot–Fenley.

Setting

A plug (U,X)(U,X)(U,X) is a compact 3-manifold UUU with boundary and a nonsingular C¹ vector field XXX transverse to ∂U\partial U∂U. The boundary splits into the entrance boundary ∂inU\partial^{in}U∂inU (where XXX points inwards) and the exit boundary ∂outU\partial^{out}U∂outU. The maximal invariant set Λ\LambdaΛ consists of the points whose orbit stays in UUU for all times. The plug is hyperbolic if Λ\LambdaΛ is a hyperbolic set with one-dimensional strong stable and strong unstable bundles. The entrance lamination LXs=Ws(Λ)∩∂inUL^s_X=W^s(\Lambda)\cap\partial^{in}ULXs​=Ws(Λ)∩∂inU and the exit lamination LXu=Wu(Λ)∩∂outUL^u_X=W^u(\Lambda)\cap\partial^{out}ULXu​=Wu(Λ)∩∂outU are one-dimensional laminations of the boundary surfaces. The plug has filling MS laminations when every component of ∂inU∖LXs\partial^{in}U\setminus L^s_X∂inU∖LXs​ (and of ∂outU∖LXu\partial^{out}U\setminus L^u_X∂outU∖LXu​) is a strip: a disc whose accessible boundary consists of two leaves asymptotic to each other at both ends.

A diffeomorphism φ:∂outU→∂inU\varphi:\partial^{out}U\to\partial^{in}Uφ:∂outU→∂inU is a strongly transverse gluing map if φ∗(LXu)\varphi_*(L^u_X)φ∗​(LXu​) and LXsL^s_XLXs​ are transverse and cut ∂inU\partial^{in}U∂inU into squares with sides alternately on leaves of the two laminations. Gluing then gives a closed manifold U/φU/\varphiU/φ with an induced vector field ZZZ. Two triples (U,X,φ)(U,X,\varphi)(U,X,φ) and (U,Y,ψ)(U,Y,\psi)(U,Y,ψ) are strongly isotopic if they are joined by a continuous path of such data.

Formalization targets

Goal: the gluing theorem (Theorem 1.5)

(U,X) hyperbolic plug with filling MS laminations, Λ without attractors or repellers, φ strongly transverse⟹ ∃ (Y,ψ) strongly isotopic to (X,φ) with the field induced by Y on U/ψ Anosov.\begin{gathered}(U,X)\ \text{hyperbolic plug with filling MS laminations},\ \Lambda\ \text{without attractors or repellers},\ \varphi\ \text{strongly transverse}\\ \Longrightarrow\ \exists\,(Y,\psi)\ \text{strongly isotopic to}\ (X,\varphi)\ \text{with the field induced by } Y \text{ on } U/\psi\ \text{Anosov}.\end{gathered}(U,X) hyperbolic plug with filling MS laminations, Λ without attractors or repellers, φ strongly transverse⟹ ∃(Y,ψ) strongly isotopic to (X,φ) with the field induced by Y on U/ψ Anosov.​

Milestones

  • Proposition 1.1: gluing two hyperbolic plugs along transverse laminations gives a hyperbolic plug. Proposition 1.3: strongly transverse gluing preserves filling MS laminations.
  • Lemma 3.27 (self-gluing case): the glued manifold U/φU/\varphiU/φ exists as a closed smooth manifold with an induced vector field.
  • Proposition 1.6: if the graph of basic pieces is strongly connected, the Anosov flow of Theorem 1.5 is transitive.
  • Theorem 1.8: every transitive Anosov flow on a closed 3-manifold is a factor of a transitive Anosov flow on another closed 3-manifold, restricted to a compact invariant set.
  • Theorem 1.9: some closed orientable 3-manifold carries both a transitive and a nontransitive Anosov flow.
  • Theorem 1.10 and Corollary 1.11: every MS foliation of a closed orientable surface is the entrance foliation of a transitive attracting hyperbolic plug; in particular incoherent transitive hyperbolic attractors exist.
  • Theorem 1.12: every hyperbolic plug with filling MS laminations embeds, up to topological equivalence, in an Anosov flow on a closed orientable 3-manifold, which can be taken transitive when Λ\LambdaΛ has no attractors or repellers.
  • Theorem 1.13: for every n≥1n\ge1n≥1 some closed orientable 3-manifold carries nnn pairwise inequivalent transitive Anosov flows.
  • Theorem 1.15: some transitive Anosov flow admits infinitely many pairwise nonisotopic transverse tori.

Significance

Theorem 1.5 lets one build Anosov flows on closed 3-manifolds by gluing hyperbolic plugs. Proposition 1.6 gives a combinatorial criterion for the result to be transitive. Together they answer a question of Katok (Theorem 1.9) and questions of Barbot and Fenley on manifolds with several hyperbolic JSJ pieces supporting transitive Anosov flows (Theorem 1.13). They also show that transitive Anosov flows admit no fully canonical decomposition into finitely many transverse tori (Theorem 1.15). The results are proved in the source paper. None of them is formalized, and Mathlib has no theory of hyperbolic sets for flows, stable manifolds or laminations. A formal proof therefore needs a substantial amount of reusable smooth dynamics.

Difficulty

The glued vector field is generally not hyperbolic: perturbing the gluing map can create solid tori of parallel periodic orbits. The difficulty is to choose the gluing map (and the vector field within its topological equivalence class) so that cone fields on ∂inU\partial^{in}U∂inU are mapped into themselves by the return map. The return map is the composition of the crossing map of the plug with the gluing map. Contraction and expansion must therefore be controlled simultaneously along two transverse invariant foliations. The paper achieves this after reducing to plugs with an affine Markov partition. The naive approach — fixing φ\varphiφ and trying to verify hyperbolicity — fails in general (Question 1.4 of the paper remains open).

Formalization scope

  • Manifolds are modelled on the half-space EuclideanHalfSpace 3 with a C∞C^\inftyC∞ structure; closed manifolds are compact, Hausdorff and BoundarylessManifold, and connected where the paper's statements concern a single manifold. Orientability is given by an atlas with positive Jacobians.
  • Vector fields are C¹ sections; flows are encoded by integral curves, so that partial flows on manifolds with boundary make sense; flowMap X t x is xxx when the orbit is undefined.
  • Hyperbolicity is quantified over a continuous Riemannian metric, invariant line fields and constants C,λ>0C,\lambda>0C,λ>0; continuity of the splitting is not imposed (it is automatic).
  • Filling MS laminations are encoded through the strip condition (Lemma 3.21); leaves of LsL^sLs are path components of intersections of weak stable manifolds with ∂inU\partial^{in}U∂inU.
  • The glued manifold U/φU/\varphiU/φ is not a quotient type: statements quantify over every closed smooth 3-manifold NNN with a surjective C¹ immersion q:U→Nq:U\to Nq:U→N realising the identification. Lemma 3.27 (a milestone) guarantees such NNN exists, so these statements are not vacuous. The induced field is not required to be C¹ and "Anosov" there means hyperbolicity of the whole manifold.
  • Useful reusable infrastructure: flows of C¹ vector fields on compact manifolds (with boundary), stable manifold theory, the λ-lemma, laminations and foliations of surfaces, and gluing of manifolds along boundary components.

Selected references

  • F. Béguin, C. Bonatti, B. Yu, Building Anosov flows on 3-manifolds, Geom. Topol. 21 (2017) 1837–1930. https://doi.org/10.2140/gt.2017.21.1837
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Algebraic Geometry·Captain: Lucas

Algebraicity of Weil classes on abelian sixfolds of discriminant -1Research Paper

Motivation

The Hodge conjecture predicts that on a non-singular complex projective variety XXX every rational cohomology class of type (p,p)(p,p)(p,p) is a rational linear combination of the classes of algebraic subvarieties of XXX. Abelian varieties are the oldest testing ground for the conjecture, and the hardest known classes on them were isolated by A. Weil. A 2n2n2n-dimensional complex abelian variety AAA is of Weil type for an imaginary quadratic field K=Q(−d)K=\mathbb{Q}(\sqrt{-d})K=Q(−d​) if KKK embeds into EndQ(A)\mathrm{End}_{\mathbb{Q}}(A)EndQ​(A) in such a way that both eigenspaces of η(−d)\eta(\sqrt{-d})η(−d​) meet H1,0(A)H^{1,0}(A)H1,0(A) in an nnn-dimensional subspace. Such an AAA carries a distinguished two-dimensional space of rational (n,n)(n,n)(n,n)-classes, the Weil classes, which for a generic AAA of Weil type does not lie in the subring generated by divisor classes. Weil classes are therefore the standard obstruction to the Hodge conjecture in low dimension: for abelian fourfolds the conjecture reduces to their algebraicity.

Timeline of the unconditional results on algebraicity of Weil classes:

  • A. Weil (1977) constructed the classes and showed that the generic abelian variety of Weil type has a three-dimensional space of rational (n,n)(n,n)(n,n)-classes, spanned by hnh^nhn and the two-dimensional Weil plane.
  • C. Schoen (Compositio Math. 65 (1988) and its 1998 Addendum, Compositio Math. 114) proved algebraicity for fourfolds of Weil type with K=Q(−3)K=\mathbb{Q}(\sqrt{-3})K=Q(−3​) and arbitrary discriminant, for sixfolds with K=Q(−3)K=\mathbb{Q}(\sqrt{-3})K=Q(−3​) and trivial discriminant, and for fourfolds with K=Q(−1)K=\mathbb{Q}(\sqrt{-1})K=Q(−1​) and discriminant −1-1−1; a second proof of the last case is in B. van Geemen's survey (1994).
  • K. Koike (Canad. Math. Bull. 47 (2004)) proved algebraicity for sixfolds with K=Q(−1)K=\mathbb{Q}(\sqrt{-1})K=Q(−1​) and discriminant −1-1−1, which yields fourfolds with K=Q(−1)K=\mathbb{Q}(\sqrt{-1})K=Q(−1​) and arbitrary discriminant.
  • E. Markman (JEMS 25 (2023)) proved algebraicity for fourfolds, arbitrary KKK, and discriminant 111.
  • E. Markman, arXiv:2502.03415, proves algebraicity for sixfolds of discriminant −1-1−1 and every imaginary quadratic KKK, and deduces the Hodge conjecture for all abelian fourfolds.

Setting

Fix ggg and present a ggg-dimensional complex torus by its first homology: a complex structure JJJ on H1(A,R)=R2gH_1(A,\mathbb{R})=\mathbb{R}^{2g}H1​(A,R)=R2g with J2=−1J^2=-1J2=−1, the lattice being Z2g⊂R2g\mathbb{Z}^{2g}\subset\mathbb{R}^{2g}Z2g⊂R2g. A polarization is a rational alternating form EEE on H1(A,Q)=Q2gH_1(A,\mathbb{Q})=\mathbb{Q}^{2g}H1​(A,Q)=Q2g satisfying the Riemann relations E(Jx,Jy)=E(x,y)E(Jx,Jy)=E(x,y)E(Jx,Jy)=E(x,y) and E(x,Jx)>0E(x,Jx)>0E(x,Jx)>0 for x≠0x\neq 0x=0. Cohomology is Hk(A,C)=∧kH1(A,C)H^k(A,\mathbb{C})=\wedge^k H^1(A,\mathbb{C})Hk(A,C)=∧kH1(A,C), realized as the alternating C\mathbb{C}C-multilinear forms on H1(A,C)=C2gH_1(A,\mathbb{C})=\mathbb{C}^{2g}H1​(A,C)=C2g; a class is rational if its values on rational vectors are rational, and it has type (p,q)(p,q)(p,q) if it is multiplied by zpzˉqz^p\bar z^{q}zpzˉq under the scaling action v↦(Re z)v+(Im z)Jvv\mapsto (\mathrm{Re}\,z)v+(\mathrm{Im}\,z)Jvv↦(Rez)v+(Imz)Jv of z∈Cz\in\mathbb{C}z∈C. A Hodge class of degree 2p2p2p is a rational class of type (p,p)(p,p)(p,p).

Let g=2ng=2ng=2n and K=Q(−d)K=\mathbb{Q}(\sqrt{-d})K=Q(−d​) with d>0d>0d>0. A polarized abelian 2n2n2n-fold of Weil type is such an (A,E)(A,E)(A,E) together with a rational endomorphism M=η(−d)M=\eta(\sqrt{-d})M=η(−d​) of H1(A,Q)H_1(A,\mathbb{Q})H1​(A,Q) with

M2=−d,MJ=JM,E(Mx,My)=d E(x,y),M^2=-d,\qquad MJ=JM,\qquad E(Mx,My)=d\,E(x,y),M2=−d,MJ=JM,E(Mx,My)=dE(x,y),

the last condition saying that η(k)\eta(k)η(k) multiplies the polarization class by the norm Nm(k)\mathrm{Nm}(k)Nm(k), and such that each of the two eigenspaces W,W‾⊂H1(A,C)W,\overline{W}\subset H_1(A,\mathbb{C})W,W⊂H1​(A,C) of MMM meets the iii-eigenspace of JJJ in an nnn-dimensional subspace. The Hodge–Weil classes are the rational classes in

HW^  =  (∧2nW  ⊕  ∧2nW‾)∩H2n(A,Q),\widehat{HW}\;=\;\big(\wedge^{2n}W\;\oplus\;\wedge^{2n}\overline{W}\big)\cap H^{2n}(A,\mathbb{Q}),HW=(∧2nW⊕∧2nW)∩H2n(A,Q),

equivalently the rational degree-2n2n2n classes that vanish on every tuple of vectors containing both a vector of WWW and a vector of W‾\overline{W}W.

The form H(x,y)=E(Mx,y)+−d E(x,y)H(x,y)=E(Mx,y)+\sqrt{-d}\,E(x,y)H(x,y)=E(Mx,y)+−d​E(x,y) is KKK-valued and hermitian on H1(A,Q)H_1(A,\mathbb{Q})H1​(A,Q), viewed as a KKK-vector space through η\etaη. The determinant of its Gram matrix in a KKK-basis lies in Q×\mathbb{Q}^{\times}Q×, and its class in Q×/Nm(K×)\mathbb{Q}^{\times}/\mathrm{Nm}(K^{\times})Q×/Nm(K×) is the discriminant det⁡H\det HdetH of (A,η,h)(A,\eta,h)(A,η,h). Discriminant −1-1−1 means that this determinant equals −(a2+dc2)-(a^2+dc^2)−(a2+dc2) for some rationals a,ca,ca,c not both zero.

Algebraicity is not modelled abstractly. An abelian variety is tied to a genuine non-singular projective variety X⊆PNX\subseteq\mathbb{P}^NX⊆PN by a projective realization: a smooth, Z2g\mathbb{Z}^{2g}Z2g-periodic immersion u:R2g→Xu:\mathbb{R}^{2g}\to Xu:R2g→X, surjective onto XXX and injective modulo the lattice, whose differential intertwines JJJ with the complex structure of PN\mathbb{P}^NPN. A class w∈H2p(A,C)w\in H^{2p}(A,\mathbb{C})w∈H2p(A,C) is algebraic when some de Rham class of XXX whose periods over the 2p2p2p-cycles swept out by rational vectors λ1,…,λ2p\lambda_1,\dots,\lambda_{2p}λ1​,…,λ2p​ equal w(λ1,…,λ2p)w(\lambda_1,\dots,\lambda_{2p})w(λ1​,…,λ2p​) is a rational combination of cycle classes cl(Z)\mathrm{cl}(Z)cl(Z) of irreducible subvarieties Z⊆XZ\subseteq XZ⊆X of dimension g−pg-pg−p. Cycle classes, de Rham cohomology of a projective variety, (p,q)(p,q)(p,q)-types and Hodge classes are taken from the platform's HodgeConjecture bundle, which formalizes §1 of Deligne's Clay problem description.

Formalization targets

Goal — Theorem 1.5.1 of arXiv:2502.03415

For every d>0: the Hodge–Weil classes of a polarized abelian sixfold of Weil type with CM by Q(−d) and discriminant −1 are algebraic.\text{For every } d>0:\ \text{the Hodge–Weil classes of a polarized abelian sixfold of Weil type with CM by }\mathbb{Q}(\sqrt{-d})\text{ and discriminant }-1\text{ are algebraic.}For every d>0: the Hodge–Weil classes of a polarized abelian sixfold of Weil type with CM by Q(−d​) and discriminant −1 are algebraic.

The statement fixes neither the field KKK nor the sixfold: it quantifies over every d>0d>0d>0, every polarized abelian sixfold of Weil type of discriminant −1-1−1, and every projective realization of it.

Milestone — Weil's plane of Hodge–Weil classes (§1.1)

HW^ is a two-dimensional Q-space, and each of its elements has type (n,n).\widehat{HW}\ \text{is a two-dimensional }\mathbb{Q}\text{-space, and each of its elements has type }(n,n).HW is a two-dimensional Q-space, and each of its elements has type (n,n).

Milestone — Schoen's degeneration step (§1.6)

Goal for all sixfolds of discriminant −1 ⟹ Hodge–Weil classes of every abelian fourfold of Weil type are algebraic,\text{Goal for all sixfolds of discriminant }-1\ \Longrightarrow\ \text{Hodge–Weil classes of every abelian fourfold of Weil type are algebraic,}Goal for all sixfolds of discriminant −1 ⟹ Hodge–Weil classes of every abelian fourfold of Weil type are algebraic,

for every imaginary quadratic KKK and every discriminant; this is the use made of Schoen's Proposition 10 (Compositio Math. 114 (1998)) in the paper.

Milestone — Corollary 1.6.1

The Hodge conjecture holds for abelian fourfolds.\text{The Hodge conjecture holds for abelian fourfolds.}The Hodge conjecture holds for abelian fourfolds.

Milestone — Lefschetz (1,1)(1,1)(1,1)

Divisor classes: every Hodge class in H2H^2H2 of a non-singular projective variety is algebraic. This is an already published platform statement, imported here as a reference, since the reduction in Corollary 1.6.1 uses the algebraicity of divisor classes.

Significance

Weil classes are, by the results of Moonen–Zarhin (Duke Math. J. 77 (1995), Math. Ann. 315 (1999)), the only obstruction left in dimension four: for a simple abelian fourfold H2,2(A,Q)H^{2,2}(A,\mathbb{Q})H2,2(A,Q) is spanned by quadratic expressions in divisor classes and by Weil classes, and the non-simple cases reduce to products treated by Ramón Marí (Collect. Math. 59 (2008)) and Moonen–Zarhin. The goal theorem therefore closes the Hodge conjecture for abelian fourfolds, the first dimension in which the conjecture for abelian varieties was open.

Formalizing it produces, first, a reusable Lean model of polarized abelian varieties, of complex multiplication of Weil type, of the Hodge–Weil plane and of the discriminant, tied to an honest notion of algebraic cohomology class through projective realizations. None of these objects exists in Mathlib today. The result itself is proved in the source preprint and has no machine-checked proof; the milestones below are equally unformalized, including the classical statements of Weil and Schoen that the paper's Corollary depends on.

Difficulty

The naive attack — write down subvarieties whose classes span HW^\widehat{HW}HW — fails because Weil classes are not expressible through divisors: for a generic abelian variety of Weil type the Néron–Severi group is cyclic while Hn,n(A,Q)H^{n,n}(A,\mathbb{Q})Hn,n(A,Q) is three-dimensional, so no product of divisor classes reaches the Weil plane. The source constructs instead a reflexive sheaf E\mathcal{E}E on X×X^X\times\hat XX×X^, for XXX the Jacobian of a genus-333 curve, whose characteristic class κ(E)\kappa(\mathcal{E})κ(E) remains of Hodge type along all deformations of (X×X^,η,h)(X\times\hat X,\eta,h)(X×X^,η,h) as a polarized abelian sixfold of Weil type, and deforms the pair over that moduli space using a semiregularity theorem for twisted sheaves. Each of these steps — Orlov's derived equivalence, spinor geometry of the Mukai lattice, semiregularity — is itself missing from Mathlib, which is why the milestone list stays on the Hodge-theoretic side of the argument rather than transcribing the sheaf-theoretic core.

Formalization scope

Conventions the Lean development commits to:

  1. Complex tori are presented by (J,E)(J,E)(J,E) on R2g\mathbb{R}^{2g}R2g with the lattice Z2g\mathbb{Z}^{2g}Z2g; the polarization form is rational rather than integral, which is the isogeny-invariant form of the Riemann relations.
  2. Cohomology is the space of alternating multilinear forms on H1(A,C)H_1(A,\mathbb{C})H1​(A,C), i.e. invariant forms on the torus; a period over a lattice cube is used to compare it with the de Rham cohomology of a projective realization.
  3. The Weil condition is imposed symmetrically on both eigenspaces of η(−d)\eta(\sqrt{-d})η(−d​), so it does not depend on the choice of convention for H1,0H^{1,0}H1,0 versus H0,1H^{0,1}H0,1.
  4. Discriminant −1-1−1 is stated as the existence of a KKK-basis in which the Gram determinant of HHH is −Nm(k)-\mathrm{Nm}(k)−Nm(k); changing the basis multiplies the determinant by a norm, so the condition is basis-independent.
  5. Algebraicity always refers to cycle classes of subvarieties of an actual projective variety, in the sense of Deligne's formulation, never to an abstract subspace of "algebraic" classes; in particular the goal cannot be satisfied by exhibiting a formal object, and the hypotheses are satisfiable — abelian varieties of Weil type of discriminant −1-1−1 exist for every KKK, and abelian varieties admit projective realizations.

A complete development needs, beyond what is drafted here: the spin representation of the Mukai lattice of an abelian nnn-fold, pure spinors and KKK-secant lines, Orlov's equivalence, Atiyah classes and semiregularity for twisted sheaves. Contributions establishing any of these, or proving the Hodge-theoretic milestones, are welcome.

Selected references

  • E. Markman, Cycles on abelian 2n2n2n-folds of Weil type from secant sheaves on abelian nnn-folds, arXiv:2502.03415. https://arxiv.org/abs/2502.03415
  • A. Weil, Abelian varieties and the Hodge ring, Collected Papers III, Springer 1980, 421–429.
  • C. Schoen, Hodge classes on self-products of a variety with an automorphism, Compositio Math. 65 (1988), 3–32; Addendum, Compositio Math. 114 (1998), 329–336. https://eudml.org/doc/89880
  • B. van Geemen, An introduction to the Hodge conjecture for abelian varieties, Lecture Notes in Math. 1594, Springer 1994, 233–252. https://doi.org/10.1007/BFb0094425
  • K. Koike, Algebraicity of some Weil Hodge classes, Canad. Math. Bull. 47 (2004), 566–572. https://doi.org/10.4153/CMB-2004-055-3
  • B. Moonen, Y. Zarhin, Hodge classes and Tate classes on simple abelian fourfolds, Duke Math. J. 77 (1995), 553–581. https://doi.org/10.1215/S0012-7094-95-07717-5
  • B. Moonen, Y. Zarhin, Hodge classes on abelian varieties of low dimension, Math. Ann. 315 (1999), 711–733. https://doi.org/10.1007/s002080050333
  • J. Ramón Marí, On the Hodge conjecture for products of certain surfaces, Collect. Math. 59 (2008), 1–26. https://doi.org/10.1007/BF03191179
  • E. Markman, The monodromy of generalized Kummer varieties and algebraic cycles on their intermediate Jacobians, J. Eur. Math. Soc. 25 (2023), 231–321. https://doi.org/10.4171/JEMS/1199
  • P. Deligne, The Hodge conjecture, Clay Mathematics Institute Millennium Prize Problem description, 2000. https://www.claymath.org/wp-content/uploads/2022/06/hodge.pdf
7 thms2 active usersReviewed
Topology·Captain: Lucas

Which homology 3-spheres bound homology 4-balls?Open Problem

Motivation

Every closed oriented 3-manifold bounds a compact oriented 4-manifold, but asking for a bounding 4-manifold with the homology of a point turns this into one of the long-standing questions of 3/4-manifold topology. The question, recorded on the Open Problem Garden as an outstanding problem of ancient/folklore origin, is whether there is a complete and computable set of invariants that determines which (rational) homology 3-spheres bound (rational) homology 4-balls (Open Problem Garden).

The question organizes the homology cobordism group ΘZ3\Theta^3_{\mathbb Z}ΘZ3​ (integral homology spheres modulo homology cobordism): an integral homology sphere represents zero in ΘZ3\Theta^3_{\mathbb Z}ΘZ3​ exactly when it bounds a smooth integral homology ball. It is also tied to the slice-ribbon problem, listed on the Open Problem Garden as a related problem.

Timeline (as recorded in the source's bibliography).

  • 1952 — Rokhlin: the signature of a closed smooth spin 4-manifold is divisible by 16. The resulting Rokhlin invariant μ∈Z/2\mu \in \mathbb Z/2μ∈Z/2 shows that the Poincaré dodecahedral space Σ(2,3,5)\Sigma(2,3,5)Σ(2,3,5) does not bound a smooth integral homology ball.
  • 1961 — Mazur: contractible 4-manifolds whose boundary is a homology sphere different from S3S^3S3.
  • 1979 — Akbulut–Kirby: the Brieskorn spheres Σ(2,5,7)\Sigma(2,5,7)Σ(2,5,7), Σ(3,4,5)\Sigma(3,4,5)Σ(3,4,5), Σ(2,3,13)\Sigma(2,3,13)Σ(2,3,13) bound contractible (Mazur) 4-manifolds.
  • 1981 — Casson–Harer: infinite families of Brieskorn spheres bounding contractible 4-manifolds, and lens spaces L(m2,mk−1)L(m^2, mk-1)L(m2,mk−1) bounding rational homology balls.
  • 1981 — Fintushel–Stern: Σ(2,3,7)\Sigma(2,3,7)Σ(2,3,7) bounds a rational homology ball.
  • 1984 — Fickle: further homology spheres bounding contractible 4-manifolds.
  • 2007 — Lisca: complete classification of connected sums of lens spaces that bound rational homology balls.

Setting

A closed topological 3-manifold MMM is a compact Hausdorff space locally homeomorphic to R3\mathbb R^3R3. Write Hn(X;Z)H_n(X;\mathbb Z)Hn​(X;Z) and Hn(X;Q)H_n(X;\mathbb Q)Hn​(X;Q) for singular homology. MMM is an integral homology 3-sphere if Hn(M;Z)≅Hn(S3;Z)H_n(M;\mathbb Z) \cong H_n(S^3;\mathbb Z)Hn​(M;Z)≅Hn​(S3;Z) for all nnn, and a rational homology 3-sphere if the same holds with Q\mathbb QQ coefficients.

A smooth integral homology 4-ball is a compact smooth 4-manifold WWW with boundary such that Hn(W;Z)≅Hn(pt;Z)H_n(W;\mathbb Z) \cong H_n(\mathrm{pt};\mathbb Z)Hn​(W;Z)≅Hn​(pt;Z) for all nnn; a rational homology 4-ball is defined with Q\mathbb QQ coefficients. MMM bounds WWW if the manifold boundary ∂W\partial W∂W is homeomorphic to MMM.

The Brieskorn manifold Σ(p,q,r)={z∈C3:z0p+z1q+z2r=0, ∣z∣=1}\Sigma(p,q,r) = \{ z \in \mathbb C^3 : z_0^p + z_1^q + z_2^r = 0,\ |z| = 1 \}Σ(p,q,r)={z∈C3:z0p​+z1q​+z2r​=0, ∣z∣=1} is an integral homology sphere when p,q,rp,q,rp,q,r are pairwise coprime; Σ(2,3,5)\Sigma(2,3,5)Σ(2,3,5) is the Poincaré homology sphere PPP. The lens space L(p,q)L(p,q)L(p,q) is the quotient of S3⊂C2S^3 \subset \mathbb C^2S3⊂C2 by the Z/p\mathbb Z/pZ/p-action generated by (z0,z1)↦(ζz0,ζqz1)(z_0,z_1) \mapsto (\zeta z_0, \zeta^q z_1)(z0​,z1​)↦(ζz0​,ζqz1​), ζ=e2πi/p\zeta = e^{2\pi i/p}ζ=e2πi/p.

To speak of algorithms, a 3-manifold is presented by a finite simplicial complex KKK, a list of simplices each given as a list of vertex labels in N\mathbb NN, with geometric realization ∣K∣⊆RN|K| \subseteq \mathbb R^{\mathbb N}∣K∣⊆RN. Every closed 3-manifold is triangulable (Moise).

Formalization targets

Goal: decidability of bounding an integral homology ball

∃ f computable,∀K, ∣K∣ is an integral homology 3-sphere  ⟹  (f(K)=true  ⟺  ∣K∣ bounds a smooth integral homology 4-ball).\exists\, f \text{ computable},\quad \forall K,\ |K| \text{ is an integral homology 3-sphere} \implies \bigl(f(K) = \mathtt{true} \iff |K| \text{ bounds a smooth integral homology 4-ball}\bigr).∃f computable,∀K, ∣K∣ is an integral homology 3-sphere⟹(f(K)=true⟺∣K∣ bounds a smooth integral homology 4-ball).

A complete and computable set of invariants is, in particular, a decision procedure; conversely a decision procedure is itself a complete computable invariant. The goal is stated for integral homology spheres and integral homology balls (the title question).

Milestones: what is known

P=Σ(2,3,5) is an integral homology 3-sphere,P does not bound a smooth Z-homology ball (Rokhlin),P = \Sigma(2,3,5) \text{ is an integral homology 3-sphere}, \qquad P \text{ does not bound a smooth } \mathbb Z\text{-homology ball (Rokhlin)},P=Σ(2,3,5) is an integral homology 3-sphere,P does not bound a smooth Z-homology ball (Rokhlin), P#(−P) bounds a smooth Z-homology ball,P \# (-P) \text{ bounds a smooth } \mathbb Z\text{-homology ball},P#(−P) bounds a smooth Z-homology ball, Σ(2,5,7), Σ(3,4,5), Σ(2,3,13) bound contractible 4-manifolds (Akbulut–Kirby),\Sigma(2,5,7),\ \Sigma(3,4,5),\ \Sigma(2,3,13) \text{ bound contractible 4-manifolds (Akbulut–Kirby)},Σ(2,5,7), Σ(3,4,5), Σ(2,3,13) bound contractible 4-manifolds (Akbulut–Kirby), Σ(p,ps−1,ps+1) (p even,s odd), Σ(p,ps±1,ps±2) (p odd) bound contractible 4-manifolds (Casson–Harer),\Sigma(p, ps-1, ps+1)\ (p \text{ even}, s \text{ odd}),\ \Sigma(p, ps\pm1, ps\pm2)\ (p \text{ odd}) \text{ bound contractible 4-manifolds (Casson–Harer)},Σ(p,ps−1,ps+1) (p even,s odd), Σ(p,ps±1,ps±2) (p odd) bound contractible 4-manifolds (Casson–Harer), L(m2,mk−1) (0<k<m, gcd⁡(m,k)=1) bounds a smooth Q-homology ball (Casson–Harer),L(m^2, mk-1)\ (0<k<m,\ \gcd(m,k)=1) \text{ bounds a smooth } \mathbb Q\text{-homology ball (Casson–Harer)},L(m2,mk−1) (0<k<m, gcd(m,k)=1) bounds a smooth Q-homology ball (Casson–Harer), Σ(2,3,7) bounds a smooth Q-homology ball (Fintushel–Stern).\Sigma(2,3,7) \text{ bounds a smooth } \mathbb Q\text{-homology ball (Fintushel–Stern)}.Σ(2,3,7) bounds a smooth Q-homology ball (Fintushel–Stern).

Significance

A decision procedure would settle membership in the zero class of ΘZ3\Theta^3_{\mathbb Z}ΘZ3​ for every presented homology sphere. Without one, each new example requires an ad hoc construction (to show bounding) or an obstruction (to rule it out). The known obstructions — the Rokhlin invariant, Siebenmann's μ‾\overline{\mu}μ​-invariant, the Ozsváth–Szabó ddd-invariant and others — are spin or spinc^cc cobordism invariants and are not known to be complete.

None of the milestone results is formalized in Lean. Formalizing even the milestones requires substantial infrastructure (smooth 4-manifolds with boundary, intersection forms, Rokhlin's theorem, explicit handle constructions), which is reusable well beyond this mission.

Difficulty

The answer to the goal is unknown; a disproof (undecidability) would equally resolve the mission. On the obstruction side, every known invariant is a homology cobordism invariant that is computable for special families but not known to detect bounding in general. On the construction side, homology balls are produced by explicit handle decompositions with no general recipe. The topological category is no substitute: by Freedman's work every integral homology 3-sphere bounds a contractible topological 4-manifold, so the problem lives entirely in the smooth category.

Formalization scope

  • Homology is Mathlib's singular homology functor with coefficients in Z\mathbb ZZ (resp. Q\mathbb QQ), valued in modules; "has the homology of XXX" means an isomorphism of HnH_nHn​ for every nnn.
  • 3-manifolds are topological (an atlas modelled on R3\mathbb R^3R3); since every topological 3-manifold has a unique smooth structure up to diffeomorphism (Moise), "∂W\partial W∂W homeomorphic to MMM" is the standard notion. Bounding 4-manifolds are compact, Hausdorff and C∞C^\inftyC∞, modelled on the half-space {x∈R4:x0≥0}\{x \in \mathbb R^4 : x_0 \ge 0\}{x∈R4:x0​≥0}. Orientations are not tracked: a homology ball bounded by MMM also, with reversed orientation, bounds −M-M−M.
  • P#(−P)P \# (-P)P#(−P) is modelled as the double of PPP minus an open chart ball, with the closed ball required to lie inside the chart.
  • The goal's input is a list of simplices; the realization lives in RN\mathbb R^{\mathbb N}RN with the product topology. The hypothesis "∣K∣|K|∣K∣ is an integral homology 3-sphere" makes this a promise problem: the algorithm is unconstrained on other inputs, which rules out trivializing via undecidability of recognizing manifolds.
  • Natural-number subtraction appears only with hypotheses ensuring it does not truncate.

Selected references

  • Open Problem Garden, Which homology 3-spheres bound homology 4-balls?, posted by rybu, 2009. http://www.openproblemgarden.org/op/which_homology_3_spheres_bound_homology_4_balls
  • R. Kirby, The topology of 4-manifolds, Lecture Notes in Mathematics 1374, Springer-Verlag, 1989.
  • V. A. Rokhlin, New results in the theory of four-dimensional manifolds, Doklady Akad. Nauk SSSR (N.S.) 84 (1952), 221–224.
  • B. Mazur, A note on some contractible 4-manifolds, Annals of Mathematics (2) 73 (1961), 221–228.
  • S. Akbulut, R. Kirby, Mazur manifolds, Michigan Math. J. 26 (1979), 259–284.
  • A. Casson, J. Harer, Some homology lens spaces which bound rational homology balls, Pacific J. Math. 96 (1981), no. 1, 23–36.
  • R. Fintushel, R. Stern, An exotic free involution on S4S^4S4, Ann. of Math. (2) 113 (1981), no. 2, 357–365.
  • H. Fickle, Knots, Z\mathbb ZZ-homology 3-spheres and contractible 4-manifolds, Houston J. Math. 10 (1984), no. 4, 467–493.
  • P. Lisca, Sums of lens spaces bounding rational balls, Algebr. Geom. Topol. 7 (2007), 2141–2164.
10 thms1 active userReviewed
Topology·Captain: Lucas

Slice–ribbon conjectureOpen Problem

Motivation

A knot is a smooth simple closed curve KKK in the 333-sphere S3S^3S3. Since S3S^3S3 is the boundary of the 444-ball B4B^4B4, one can ask whether KKK bounds a smoothly embedded disc in B4B^4B4; if so, KKK is called slice. Slice knots are the identity element of the smooth knot concordance group, so deciding which knots are slice is a central question of 444-dimensional topology. A more restrictive and more combinatorial notion is that of a ribbon knot: a knot bounding an immersed disc in S3S^3S3 whose only self-intersections are ribbon singularities (arcs of double points whose two preimages are an interior arc and an arc running across the disc from boundary to boundary). Every ribbon knot is slice: pushing the interior of a ribbon disc into B4B^4B4 removes the double points. In 1962 R. H. Fox asked for the converse ([F]). The Open Problem Garden lists this slice–ribbon problem as Outstanding (source): given a knot in S3S^3S3 which is slice, is it a ribbon knot?

Timeline

  • 1962 — Fox, Some problems in knot theory ([F]): asks whether every slice knot is ribbon.
  • 1966 — Fox–Milnor: the Alexander polynomial of a slice knot factors as f(t)f(t−1)f(t)f(t^{-1})f(t)f(t−1), the first obstruction to sliceness.
  • 1982 — Gilmer ([G], Invent. Math. 66): lower bounds on the slice genus from Casson–Gordon invariants.
  • 1983 — Hass ([H], Math. Proc. Cambridge Philos. Soc. 94): studies the problem through minimal surfaces in B4B^4B4; a knot bounding a minimal disc in B4B^4B4 is ribbon.
  • 2007 — Lisca: the slice–ribbon conjecture holds for all 222-bridge knots.
  • 2008–2015 — Owens (arXiv:0802.2109), Greene–Jabuka (odd 333-strand pretzel knots), Lecuona (families of Montesinos knots, arXiv:0910.4601): further families where slice implies ribbon.
  • 2010 — Gompf–Scharlemann–Thompson: candidate counterexamples arising from fibered knots and Property 2R.
  • The general question remains open.

Setting

Write R4\mathbb R^4R4 for Euclidean 444-space (R4), S3={x:∥x∥=1}S^3=\{x:\|x\|=1\}S3={x:∥x∥=1}, B4={x:∥x∥≤1}B^4=\{x:\|x\|\le1\}B4={x:∥x∥≤1}, and D2={z∈R2:∥z∥≤1}D^2=\{z\in\mathbb R^2:\|z\|\le 1\}D2={z∈R2:∥z∥≤1} for the closed unit disc in the parameter plane R2\mathbb R^2R2 (R2).

  1. Knot (IsKnot γ). A map γ:R→R4\gamma:\mathbb R\to\mathbb R^4γ:R→R4 which is C∞C^\inftyC∞, 111-periodic, takes values in S3S^3S3, is injective on [0,1)[0,1)[0,1), and has nowhere-vanishing velocity. The knot is the image K=γ(R)K=\gamma(\mathbb R)K=γ(R).
  2. Slice disc (IsSliceDisk γ F). A C∞C^\inftyC∞ map F:R2→R4F:\mathbb R^2\to\mathbb R^4F:R2→R4 that is injective on D2D^2D2 with injective differential at every point of D2D^2D2, maps the open disc into the open ball, maps the unit circle onto KKK, and is transverse to S3S^3S3 along the boundary: ⟨F(z),dFz(z)⟩>0\langle F(z), dF_z(z)\rangle>0⟨F(z),dFz​(z)⟩>0 for ∥z∥=1\|z\|=1∥z∥=1. A knot is slice (IsSlice γ) if it has a slice disc.
  3. Ribbon disc (IsRibbonImmersedDisk γ f, Fox's definition). A C∞C^\inftyC∞ map f:R2→R4f:\mathbb R^2\to\mathbb R^4f:R2→R4 that maps D2D^2D2 into S3S^3S3 with injective differential on D2D^2D2, maps the unit circle injectively onto KKK, has no triple points, has transverse double points, and whose double-point set in D2D^2D2 is a disjoint union of arcs a1,b1,…,an,bna_1,b_1,\dots,a_n,b_na1​,b1​,…,an​,bn​ with f∘ai=f∘bif\circ a_i=f\circ b_if∘ai​=f∘bi​, each aia_iai​ contained in the open disc and each bib_ibi​ running from the boundary circle through the open disc back to the boundary circle. A knot is ribbon (IsRibbon γ) if it bounds a ribbon disc.
  4. Ribbon slice disc (IsRibbonSliceDisk γ F). A slice disc on which the squared radial function rF(z)=∥F(z)∥2r_F(z)=\|F(z)\|^2rF​(z)=∥F(z)∥2 is Morse in the open disc with no local maxima.
  5. Minimal disc (IsMinimalOnDisk F). With E=⟨∂0F,∂0F⟩E=\langle\partial_0F,\partial_0F\rangleE=⟨∂0​F,∂0​F⟩, G′=⟨∂0F,∂1F⟩G'=\langle\partial_0F,\partial_1F\rangleG′=⟨∂0​F,∂1​F⟩, G=⟨∂1F,∂1F⟩G=\langle\partial_1F,\partial_1F\rangleG=⟨∂1​F,∂1​F⟩, the vector G ∂0∂0F−2G′ ∂0∂1F+E ∂1∂1FG\,\partial_0\partial_0F-2G'\,\partial_0\partial_1F+E\,\partial_1\partial_1FG∂0​∂0​F−2G′∂0​∂1​F+E∂1​∂1​F is tangent to the surface at every interior point, i.e. the mean curvature vector of FFF vanishes on the open disc.

Formalization targets

Goal: slice implies ribbon

∀ γ,IsKnot(γ) ∧ IsSlice(γ) ⟹ IsRibbon(γ).\forall\,\gamma,\quad \mathrm{IsKnot}(\gamma)\ \wedge\ \mathrm{IsSlice}(\gamma)\ \Longrightarrow\ \mathrm{IsRibbon}(\gamma).∀γ,IsKnot(γ) ∧ IsSlice(γ) ⟹ IsRibbon(γ).

Milestones

  1. [F] Ribbon knots are slice — the converse direction, observed by Fox.
  2. Ribbon discs in S3S^3S3 versus ribbon discs in B4B^4B4 — a knot is ribbon iff it bounds a slice disc on which the radial function is Morse without local maxima.
  3. [H] Hass — a knot bounding a minimal slice disc in B4B^4B4 is ribbon.

A further (non-milestone) sanity item asserts that the round unknot t↦(cos⁡2πt,sin⁡2πt,0,0)t\mapsto(\cos 2\pi t,\sin 2\pi t,0,0)t↦(cos2πt,sin2πt,0,0) is a ribbon knot, which shows that the definitions are not vacuous.

A supporting (non-milestone) item isolates the maximum-principle step behind [H]: on a minimal disc, the radial function ∥F∥2\|F\|^2∥F∥2 has no local maximum in the open disc.

Significance

A positive answer would make sliceness, a 444-dimensional property defined by the existence of an embedded disc in B4B^4B4, equivalent to a 333-dimensional property that can be certified by a finite diagrammatic object (a ribbon presentation). A counterexample would exhibit a slice knot whose slice discs all need local maxima of the radial function; several proposed candidates (Gompf–Scharlemann–Thompson) are tied to the smooth 444-dimensional Poincaré conjecture and to Property 2R. The problem is closely related to the question of which homology 333-spheres bound homology 444-balls.

On the formal side no part of this theory is in Mathlib: there are no knots, no slice or ribbon discs, no Morse functions on surfaces and no minimal surfaces. The milestones (Fox's easy direction, the 333D/444D equivalence, Hass's theorem) are classical theorems that have not been machine-checked; formalizing them builds the infrastructure any later attack needs.

Difficulty

Turning a slice disc into a ribbon disc requires removing the local maxima of the radial function on the disc. Cancelling a maximum against a saddle is possible only when the handles are in suitable position, and there is no known procedure that achieves this in general; the known positive results rely on classifying the rational homology balls bounded by branched double covers, using Donaldson's diagonalization theorem, which applies only to special families of knots.

Formalization scope

Everything is stated in Euclidean coordinates: knots are periodic parametrisations R→S3⊂R4\mathbb R\to S^3\subset\mathbb R^4R→S3⊂R4, discs are C∞C^\inftyC∞ maps R2→R4\mathbb R^2\to\mathbb R^4R2→R4 whose restriction to D2D^2D2 is the disc in question. Smoothness is C∞C^\inftyC∞; slice discs are required to be smooth up to the boundary and transverse to S3S^3S3 there (the standard notion of a properly embedded disc). The knot enters only through its image, so orientation and parametrization play no role. The problem is the smooth one; topologically locally flat slice discs are not allowed. Definitions under which the conjecture holds trivially (for example, a ribbon condition implied by the slice condition by definition) are excluded: the goal uses Fox's 333-dimensional ribbon discs, and the 444-dimensional characterisation is a separate milestone.

Contributions welcome: smooth embedded discs and their collars, Morse theory for functions on D2D^2D2, the push-in construction, and minimal-surface tools (the maximum principle for ∥x∥2\|x\|^2∥x∥2 on minimal surfaces).

Selected references

  • [F] R. H. Fox, Some problems in knot theory, Topology of 3-manifolds and related topics (Proc. Univ. of Georgia Institute, 1961), Prentice-Hall, 1962, pp. 168–176.
  • [G] P. M. Gilmer, On the slice genus of knots, Invent. Math. 66 (1982), 191–197.
  • [H] J. Hass, The geometry of the slice-ribbon problem, Math. Proc. Cambridge Philos. Soc. 94 (1983), 101–108.
  • A. G. Lecuona, On the slice-ribbon conjecture for Montesinos knots, arXiv:0910.4601.
  • B. Owens, On slicing invariants of knots, arXiv:0802.2109.
  • P. Lisca, Lens spaces, rational balls and the ribbon conjecture, Geom. Topol. 11 (2007), 429–472. https://doi.org/10.2140/gt.2007.11.429
  • R. E. Gompf, M. Scharlemann, A. Thompson, Fibered knots and potential counterexamples to the Property 2R and slice-ribbon conjectures, Geom. Topol. 14 (2010), 2305–2347. https://doi.org/10.2140/gt.2010.14.2305
  • Open Problem Garden, Slice-ribbon problem (posted by rybu, 2009). http://www.openproblemgarden.org/op/slice_ribbon_problem
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Topology·Captain: Lucas

Smooth 4-dimensional Poincaré conjectureOpen Problem

Motivation

The generalized Poincaré conjecture asks whether a closed nnn-manifold with the homotopy type of the sphere SnS^nSn must be the sphere. In the topological category (conclusion: homeomorphic) it is now known in every dimension: n=1,2n = 1, 2n=1,2 classically, n≥5n \ge 5n≥5 by Smale (and Stallings, Newman), n=4n = 4n=4 by Freedman (1982), and n=3n = 3n=3 by Perelman (2003). In the smooth category (conclusion: diffeomorphic) it fails in general: Milnor (1956) found exotic smooth structures on S7S^7S7, and Kervaire–Milnor showed that exotic spheres exist in many dimensions. The single case that remains completely open is the smooth one in dimension 444; the Open Problem Garden rates it Outstanding.

Timeline

  • 1904 — Poincaré raises the question for 3-manifolds.
  • 1956 — Milnor: exotic smooth 7-spheres.
  • 1960–62 — Smale (and Stallings): the topological Poincaré conjecture for n≥5n \ge 5n≥5.
  • 1963 — Kervaire–Milnor: classification of homotopy spheres in dimensions ≥5\ge 5≥5.
  • 1982 — Freedman: the topological Poincaré conjecture for n=4n = 4n=4.
  • 1982–87 — Donaldson, Freedman, Gompf, Taubes: exotic R4\mathbb{R}^4R4's, in fact a continuum of them.
  • 2002–03 — Perelman: the Poincaré conjecture for n=3n = 3n=3 (see Morgan–Tian).

Setting

All manifolds are Hausdorff, compact, without boundary and smooth (C∞C^\inftyC∞). The model sphere is Sn={x∈Rn+1:∥x∥=1}S^n = \{x \in \mathbb{R}^{n+1} : \|x\| = 1\}Sn={x∈Rn+1:∥x∥=1} with its standard smooth structure. Two spaces have the same homotopy type if there is a homotopy equivalence between them.

Formalization targets

Goal

M closed smooth 4-manifold, M≃S4  ⟹  M≅C∞S4.M \text{ closed smooth 4-manifold},\ M \simeq S^4 \implies M \cong_{C^\infty} S^4.M closed smooth 4-manifold, M≃S4⟹M≅C∞​S4.

This is the conjecture exactly as stated in the source.

Significance

By Freedman's theorem a homotopy 4-sphere is already homeomorphic to S4S^4S4, so the conjecture is equivalent to the statement that S4S^4S4 has no exotic smooth structure. It would complete the generalized Poincaré conjectures in the smooth category in the one dimension where the answer is unknown. A disproof would give the first exotic smooth structure on a closed simply connected 4-manifold with small homology.

Difficulty

The h-cobordism technology that settles dimensions ≥5\ge 5≥5 (the Whitney trick) fails in dimension 4. Freedman's topological methods give a homeomorphism but no smoothing, and gauge-theoretic invariants (Donaldson, Seiberg–Witten) give no information on homotopy 4-spheres. Many candidate counterexamples (Gluck twists, Cappell–Shaneson spheres) have since been shown to be standard.

Formalization scope

Manifolds use Mathlib's ChartedSpace (EuclideanSpace ℝ (Fin n)) M together with IsManifold (𝓡 n) ∞ M. The model with corners 𝓡 n has no boundary, and ∞ means C∞C^\inftyC∞ (not analytic). The sphere is Metric.sphere (0 : EuclideanSpace ℝ (Fin (n+1))) 1 with Mathlib's standard smooth structure. A homotopy equivalence is ContinuousMap.HomotopyEquiv, and diffeomorphisms are Diffeomorph (≃ₘ^∞⟮𝓡 n, 𝓡 n⟯). Closedness is CompactSpace plus T2Space; second countability follows from compactness. The milestones are the known results the source cites: low dimensions, Perelman, Smale, Milnor's exotic spheres, Freedman, and the continuum of exotic R4\mathbb{R}^4R4's. They also include the equivalent reformulation "there is no exotic S4S^4S4". Formalizing any of them requires substantial new manifold-topology infrastructure in Mathlib, and that work is welcome.

Selected references

  • M. Freedman, F. Quinn, Topology of 4-manifolds, Princeton University Press, 1990.
  • S. Smale, On the structure of manifolds, Amer. J. Math. 84 (1962), 387–399.
  • J. Morgan, G. Tian, Ricci Flow and the Poincaré Conjecture, AMS/CMI, 2007.
  • J. Milnor, On manifolds homeomorphic to the 7-sphere, Ann. of Math. 64 (1956), 399–405.
  • C. Taubes, Gauge theory on asymptotically periodic 4-manifolds, J. Differential Geom. 25 (1987), 363–430.
  • Open Problem Garden, Smooth 4-dimensional Poincaré conjecture.
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Topology·Captain: Lucas

Smooth 4-dimensional Schoenflies problemOpen Problem

Motivation

The Schoenflies problem asks whether a codimension-one sphere sitting smoothly inside a sphere can be knotted. In every dimension except one the answer is known to be "no"; the remaining case, a smooth 333-sphere in S4S^4S4, is listed as an outstanding problem in the Open Problem Garden (source). It is one of the central open questions of smooth 444-manifold topology, closely tied to the existence of exotic smooth structures on the 444-ball and to the smooth 444-dimensional Poincaré conjecture.

Timeline.

  • Early 1900s — Schoenflies: every Jordan curve in the plane bounds a disc (the case n=1n = 1n=1 below).
  • 1924 — Alexander: every (polyhedral, hence smooth) 222-sphere in S3S^3S3 bounds a 333-ball on each side (PNAS); a modern exposition is in Hatcher's notes on 333-manifolds.
  • 1959–1960 — Mazur (Bull. AMS) and Brown (Bull. AMS): the generalized Schoenflies theorem. A (locally flat) embedded Sn⊂Sn+1S^n \subset S^{n+1}Sn⊂Sn+1 bounds a topological (n+1)(n+1)(n+1)-ball on each side, in every dimension.
  • 1960s — The hhh-cobordism theorem implies that Dn+1D^{n+1}Dn+1 has no exotic smooth structure restricting to the standard one on the boundary when n≥4n \ge 4n≥4. Combined with Mazur–Brown, this settles the smooth problem for n≥4n \ge 4n≥4.
  • 1984–2008 — Scharlemann proves the smooth 444-dimensional statement for restricted classes of embeddings: genus-two embeddings (Topology 23, 1984), spheres with four critical points (Invent. Math. 79, 1985), and further cases via Generalized Property R (Comment. Math. Helv. 83, 2008).
  • The case n=3n = 3n=3 remains open.

Setting

For n≥0n \ge 0n≥0 let Sn={x∈Rn+1:∥x∥=1}S^n = \{x \in \mathbb{R}^{n+1} : \|x\| = 1\}Sn={x∈Rn+1:∥x∥=1} be the unit sphere with its standard smooth structure, and let Dn+1={x∈Rn+1:∥x∥≤1}D^{n+1} = \{x \in \mathbb{R}^{n+1} : \|x\| \le 1\}Dn+1={x∈Rn+1:∥x∥≤1} be the closed unit ball. In the Lean development SnS^nSn is Sph n.

A smooth embedding f:Sn→Sn+1f : S^n \to S^{n+1}f:Sn→Sn+1 is a C∞C^\inftyC∞ map that is injective and whose differential dfxdf_xdfx​ is injective at every point (an injective immersion; since SnS^nSn is compact this is an embedding). Its image M=f(Sn)M = f(S^n)M=f(Sn) is a smooth nnn-dimensional submanifold of Sn+1S^{n+1}Sn+1 diffeomorphic to SnS^nSn (Lean predicate IsSmoothEmbeddingSph n f).

By the Jordan–Brouwer separation theorem, Sn+1∖MS^{n+1} \setminus MSn+1∖M has exactly two connected components, and MMM is the frontier of each. Their closures are compact connected (n+1)(n+1)(n+1)-manifolds with common boundary MMM.

A subset K⊆Sn+1K \subseteq S^{n+1}K⊆Sn+1 is a smoothly embedded closed ball if it is diffeomorphic to Dn+1D^{n+1}Dn+1 (with the smooth structure inherited from Sn+1S^{n+1}Sn+1). Concretely, K=e(Dn+1)K = e(D^{n+1})K=e(Dn+1) for a C∞C^\inftyC∞ map e:Rn+1→Sn+1e : \mathbb{R}^{n+1} \to S^{n+1}e:Rn+1→Sn+1 that is injective on Dn+1D^{n+1}Dn+1 and has injective differential at every point of Dn+1D^{n+1}Dn+1, boundary points included (Lean predicate IsSmoothClosedBallIn n K). The topological counterpart, KKK homeomorphic to Dn+1D^{n+1}Dn+1, is IsTopClosedBallIn n K.

Formalization targets

Goal: the smooth Schoenflies problem in dimension 4

For every smooth embedding f:S3→S4f : S^3 \to S^4f:S3→S4 and every point x∈S4∖f(S3)x \in S^4 \setminus f(S^3)x∈S4∖f(S3), writing CxC_xCx​ for the connected component of S4∖f(S3)S^4 \setminus f(S^3)S4∖f(S3) containing xxx,

Cx‾ is diffeomorphic to D4.\overline{C_x} \text{ is diffeomorphic to } D^4 .Cx​​ is diffeomorphic to D4.

Equivalently: f(S3)f(S^3)f(S3) is unknotted.

Milestones (known results)

  1. Jordan–Brouwer separation, all nnn: Sn+1∖f(Sn)S^{n+1} \setminus f(S^n)Sn+1∖f(Sn) has exactly two components, each with frontier f(Sn)f(S^n)f(Sn).
  2. Generalized Schoenflies theorem (Mazur, Brown), all nnn: each Cx‾\overline{C_x}Cx​​ is homeomorphic to Dn+1D^{n+1}Dn+1.
  3. Schoenflies, n=1n = 1n=1: each Cx‾\overline{C_x}Cx​​ is diffeomorphic to D2D^2D2.
  4. Alexander, n=2n = 2n=2: each Cx‾\overline{C_x}Cx​​ is diffeomorphic to D3D^3D3.
  5. High dimensions, n≥4n \ge 4n≥4: each Cx‾\overline{C_x}Cx​​ is diffeomorphic to Dn+1D^{n+1}Dn+1.

Significance

The result itself. By milestone 2, MMM always bounds two topological 444-balls. So a counterexample to the goal would produce an exotic smooth structure on D4D^4D4 that embeds in S4S^4S4; a proof would show that no exotic D4D^4D4, if one exists, embeds in S4S^4S4. The problem is related to, but independent of, the smooth 444-dimensional Poincaré conjecture. For example, the Poincaré conjecture could hold while D4D^4D4 carries an exotic smooth structure. The goal also completes the uniform statement "every smooth Sn⊂Sn+1S^n \subset S^{n+1}Sn⊂Sn+1 is unknotted" across all dimensions.

Formalizing it. The goal is open. Milestones 1–5 are classical theorems, and no existing machine-checked proof of them for smooth spheres is relied on here. Formalizing them is substantial independent work and would add basic infrastructure to Mathlib's manifold library: separation theorems, collars, and smoothing of balls.

Difficulty

The topological statement is known in every dimension (milestone 2), so the difficulty is purely smooth. In dimensions ≥5\ge 5≥5 the passage from "homeomorphic to a ball" to "diffeomorphic to a ball" goes through the hhh-cobordism theorem. That theorem fails in the smooth category in dimension 444, because the Whitney trick is unavailable. Freedman's topological methods do not control smooth structures. The naive approach is to apply the high-dimensional argument verbatim, and this breaks at exactly this step. Known partial results (Scharlemann) need strong restrictions on the embedding, such as genus bounds or few critical points of a height function.

Formalization scope

  • Spheres are the unit spheres in EuclideanSpace ℝ (Fin (n+1)), with Mathlib's standard smooth manifold structure modelled on EuclideanSpace ℝ (Fin n). Smoothness means C∞C^\inftyC∞ (ContMDiff … ∞), not analytic.
  • A smooth embedding of SnS^nSn is encoded as a C∞C^\inftyC∞ injective immersion (injective mfderiv everywhere). This is equivalent because SnS^nSn is compact.
  • "Diffeomorphic to Dn+1D^{n+1}Dn+1" is encoded as the image of the closed unit ball under a globally C∞C^\inftyC∞ map Rn+1→Sn+1\mathbb{R}^{n+1} \to S^{n+1}Rn+1→Sn+1 that is injective with injective differential on the closed ball. Requiring smoothness on all of Rn+1\mathbb{R}^{n+1}Rn+1 loses no generality: a map smooth on a neighbourhood of the ball can be precomposed with a smooth radial retraction.
  • The components of the complement are connectedComponentIn (Set.range f)ᶜ x for x∉f(Sn)x \notin f(S^n)x∈/f(Sn). The conclusion is required for every such xxx, so for both sides of MMM.
  • The statement does not hold vacuously: the hypotheses are satisfied by the standard equator, and the immersion condition rules out degenerate maps, since a non-differentiable map has zero mfderiv, which is not injective.
  • A complete development needs collar neighbourhoods, separation theorems for smooth hypersurfaces, and tools for comparing smooth structures on balls. Contributions to any milestone are welcome.

Selected references

  • Open Problem Garden, Smooth 4-dimensional Schoenflies problem (posted by rybu, 2009). https://www.openproblemgarden.org/op/smooth_4_dimensional_schoenflies_problem
  • J. W. Alexander, On the subdivision of 3-space by a polyhedron, Proc. Nat. Acad. Sci. USA 10 (1924), 6–8. https://doi.org/10.1073/pnas.10.1.6
  • B. Mazur, On embeddings of spheres, Bull. Amer. Math. Soc. 65 (1959), 59–65. https://doi.org/10.1090/S0002-9904-1959-10274-3
  • M. Brown, A proof of the generalized Schoenflies theorem, Bull. Amer. Math. Soc. 66 (1960), 74–76. https://doi.org/10.1090/S0002-9904-1960-10400-4
  • M. Morse, E. Baiada, Homotopy and homology related to the Schoenflies problem, Ann. of Math. 58 (1953), 142–165.
  • M. Freedman, F. Quinn, Topology of 4-manifolds, Princeton University Press, 1990.
  • M. Scharlemann, The four-dimensional Schoenflies conjecture is true for genus two imbeddings, Topology 23 (1984), 211–217.
  • M. Scharlemann, Smooth spheres in R4\mathbb{R}^4R4 with four critical points are standard, Invent. Math. 79 (1985), 125–141.
  • M. Scharlemann, Generalized Property R and the Schoenflies conjecture, Comment. Math. Helv. 83 (2008), 421–449.
  • A. Hatcher, Notes on basic 3-manifold topology. http://www.math.cornell.edu/~hatcher/3M/3Mdownloads.html
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CombinatoricsGraph Theory·Captain: mikedeng1

Planar Graphs Have Bounded Queue-Number 2: Every Graph of Euler Genus g Has Queue-Number at Most 4g + 49Research Paper

Motivation

A queue layout of a graph places its vertices on a line and splits its edges into classes, called queues, so that inside one queue no edge is nested inside another. The minimum number of queues is the queue-number. Queue layouts were introduced by Heath, Leighton and Rosenberg (1992) and Heath and Rosenberg (1992) as the dual of stack layouts (book embeddings): reading the vertex order from left to right, the edges of one queue are opened and closed in first-in first-out order. Queue layouts are closely tied to track layouts and, through them, to three-dimensional grid drawings of graphs (§9 of the paper).

Whether planar graphs have bounded queue-number was asked by Heath, Leighton and Rosenberg in 1992 and stayed open for 27 years. The best general bounds before 2019 grew with the number of vertices: O(n)O(\sqrt n)O(n​) by Heath, Leighton and Rosenberg (1992), O(log⁡2n)O(\log^2 n)O(log2n) by Di Battista, Frati and Pach (2013), and O(log⁡n)O(\log n)O(logn) by Dujmović (2015); for Euler genus ggg, Dujmović, Morin and Wood (2017) had O(g+log⁡n)O(g + \log n)O(g+logn). Dujmović, Joret, Micek, Morin, Ueckerdt and Wood (arXiv:1904.04791, J. ACM 2020) proved that every planar graph has queue-number at most 494949 (Theorem 1), and extended the result to every graph embeddable in a fixed surface (Theorem 2) and to every proper minor-closed class (Theorem 3).

This mission is Theorem 2: graphs of Euler genus ggg have queue-number at most 4g+494g + 494g+49. It is the second mission of a two-mission series; the first poses Theorem 1.

Setting

All graphs are finite and simple. A linear ordering ⪯\preceq⪯ of the vertex set V(G)V(G)V(G) is fixed. Two edges vwvwvw and xyxyxy with four distinct ends nest if v≺x≺y≺wv \prec x \prec y \prec wv≺x≺y≺w (after renaming the ends). A queue is a set of edges no two of which nest. A kkk-queue layout of GGG is a linear ordering together with a partition of E(G)E(G)E(G) into kkk queues, and qn⁡(G)≤k\operatorname{qn}(G) \le kqn(G)≤k means that a kkk-queue layout exists.

A layering of GGG is an ordered partition (V0,V1,… )(V_0, V_1, \dots)(V0​,V1​,…) of V(G)V(G)V(G) such that every edge joins two vertices of the same or of consecutive layers. A BFS layering takes one root rrr in each connected component and puts vvv in layer dist⁡(r,v)\operatorname{dist}(r, v)dist(r,v). A BFS spanning tree of a connected graph GGG rooted at rrr is a spanning tree TTT with dist⁡T(r,v)=dist⁡G(r,v)\operatorname{dist}_T(r, v) = \operatorname{dist}_G(r, v)distT​(r,v)=distG​(r,v) for every vvv. A path in TTT is vertical if the distance to rrr grows by exactly one at every step.

The Euler genus of the orientable surface with hhh handles is 2h2h2h, and that of the non-orientable surface with ccc cross-caps is ccc; the Euler genus of a graph is the least Euler genus of a surface it embeds in (footnote 2 of the paper). Planar graphs are exactly the graphs of Euler genus 000. Combinatorially, an embedding of a graph is described by an embedding scheme: a cyclic order of the edges at each vertex (a rotation system) together with a sign on every edge (twisted or not). Tracing faces through the scheme gives a face count fff, and with nnn vertices, mmm edges and ccc components the scheme has Euler genus 2c−n+m−f2c - n + m - f2c−n+m−f.

Formalization targets

Goal: Theorem 2 with the paper's bound

Euler genus of G≤g ⟹ qn⁡(G)≤4g+49.\text{Euler genus of } G \le g \ \Longrightarrow\ \operatorname{qn}(G) \le 4g + 49 .Euler genus of G≤g ⟹ qn(G)≤4g+49.

The paper states Theorem 2 as qn⁡(G)=O(g)\operatorname{qn}(G) = O(g)qn(G)=O(g) and proves the explicit bound 4g+494g + 494g+49 in §5. The goal poses that explicit bound, for every finite graph, connected or not.

Milestones

  1. Lemma 18 (p. 18). Every BFS layering (V0,V1,… )(V_0, V_1, \dots)(V0​,V1​,…) of a planar graph GGG admits a 494949-queue layout whose vertex ordering lists V0V_0V0​, then V1V_1V1​, then V2V_2V2​, and so on.
  2. Lemma 21 (p. 19). If GGG is connected with Euler genus at most ggg and TTT is a BFS spanning tree with layering (Vi)(V_i)(Vi​), there is a connected (or empty) subgraph ZZZ with at most 2g2g2g vertices in each layer such that G−V(Z)G - V(Z)G−V(Z) is planar and sits inside a connected planar graph G+G^+G+ whose own BFS layering (Wi)(W_i)(Wi​) satisfies Wi∩(V(G)∖V(Z))=Vi∖V(Z)W_i \cap (V(G)\setminus V(Z)) = V_i \setminus V(Z)Wi​∩(V(G)∖V(Z))=Vi​∖V(Z); vertical paths of the BFS tree of G+G^+G+ restrict to vertical paths of TTT.
  3. The 4g4g4g-queue step (p. 23). If GGG has a layering with at most 2g2g2g vertices of ZZZ per layer and G−ZG - ZG−Z has a 494949-queue layout ordered layer by layer, then qn⁡(G)≤4g+49\operatorname{qn}(G) \le 4g + 49qn(G)≤4g+49.

Significance

The result. Theorem 2 settles boundedness of the queue-number for every class of graphs embeddable in a fixed surface, with a bound linear in the Euler genus. Through the connection between queue-number and track-number, the paper derives from it (§9, Theorems 54 and 58) that a graph of Euler genus ggg with nnn vertices has track-number gO(g4/7)g^{O(g^{4/7})}gO(g4/7) and a three-dimensional grid drawing of volume gO(g4/7)ng^{O(g^{4/7})} ngO(g4/7)n, linear in nnn for every fixed surface. It is also a step on the paper's route to Theorem 3 (proper minor-closed classes), since graphs on surfaces are the basic pieces of the Robertson–Seymour graph minor structure theorem. Lemma 21 is of independent use: it reduces a graph on a surface to a planar graph while controlling BFS layers.

Formalizing it. The result is proved; as far as is known it has no machine-checked proof. A formalization needs queue layouts, layerings, BFS layerings and vertical paths, and, independently of queues, a usable combinatorial theory of graphs on surfaces, which Lean's Mathlib does not have. The Euler genus definition of this mission (embedding schemes and face tracing) and Lemma 21 are reusable well beyond queue layouts.

Difficulty

The obvious reduction, deleting few vertices to make the graph planar, is not enough: a planar subgraph alone does not control how the deleted vertices interact with a queue layout. The deleted set must be thin in every BFS layer, and the planar remainder must carry a BFS layering compatible with the original one, which is what Lemma 21 provides. Its proof cuts the surface along a subgraph made of tree paths and must show that the cut graph is planar by an Euler-characteristic count over face-tracing data, and that distances from a new root agree with the old BFS distances. In Lean, the main obstacle is the surface side: Euler's formula for embedding schemes, the cutting operation on rotation systems, and the passage between the combinatorial notion of Euler genus and the drawing-based notion of planarity. The planar input, Lemma 18, is itself the whole of mission 1's argument (Theorem 15 with Lemmas 5 and 8).

Formalization scope

  • Graphs are SimpleGraph V on a finite type V : Type with decidable equality and adjacency.
  • "qn⁡(G)≤k\operatorname{qn}(G) \le kqn(G)≤k" is HasQueueLayout G k: an injective map ord : V → ℕ (the linear ordering) and an assignment of the edges of GGG (G.edgeSet, not all unordered pairs) to Fin k such that no two edges in one queue nest; nesting uses strict inequalities, so edges sharing an end never nest. Queues may be empty.
  • A layering is a layer function L : V → ℕ; a BFS layering takes one root per component. Vertical paths are nonempty lists indexed from 000 with distance d+id + id+i, d≥0d \ge 0d≥0.
  • Euler genus is combinatorial: EulerGenusLE G g asks for an embedding scheme (rotation permutation of the darts, cyclic at every vertex, and a symmetric edge signature) whose Euler genus 2c−n+m−f2c - n + m - f2c−n+m−f, computed in Z\mathbb ZZ, is at most ggg. The face count is half the number of face-tracing orbits plus the number of isolated vertices. Equivalence with footnote 2's topological definition is the Heffter–Edmonds–Ringel rotation principle and its non-orientable extension, with additivity over components; it is not part of the mission.
  • Planarity is the published RobertsonSeymour1986.GM5.IsPlanar: a crossing-free drawing in R2\mathbb R^2R2 by simple arcs. "Euler genus 000 iff planar" is a theorem connecting the two definitions, not built into either.
  • "Euler genus ggg" is read as "at most ggg" throughout; every bound is monotone in ggg. In Lemma 21, "ZZZ is connected" reads "empty or connected" (the paper takes Z=∅Z = \emptysetZ=∅ when g=0g = 0g=0), and the restriction of a vertical path may be empty.
  • Trivializing formalizations are ruled out: queues indexed on all pairs Sym2 V would deny edgeless graphs a 000-queue layout; non-strict nesting would forbid adjacent edges in one queue; a drawing that tolerates crossings would make every graph planar; a face count without halving, or without isolated vertices, would make the Euler genus too small or too large (the sanity checks confirm K3K_3K3​ has a scheme of Euler genus 000, a twisted K3K_3K3​ one of genus 111, and two isolated vertices genus 000).
  • Welcome contributions: Euler's formula for embedding schemes, face-tracing lemmas, the planar case (Lemma 18, via mission 1's results), the cutting construction of Lemma 21, and the purely combinatorial 4g4g4g-queue step.

Selected references

  • V. Dujmović, G. Joret, P. Micek, P. Morin, T. Ueckerdt, D. R. Wood, Planar graphs have bounded queue-number, J. ACM 67(4), 2020; arXiv:1904.04791v5. https://arxiv.org/abs/1904.04791 , https://doi.org/10.1145/3385731
  • L. S. Heath, F. T. Leighton, A. L. Rosenberg, Comparing queues and stacks as mechanisms for laying out graphs, SIAM J. Discrete Math. 5(3), 1992. https://doi.org/10.1137/0405031
  • L. S. Heath, A. L. Rosenberg, Laying out graphs using queues, SIAM J. Comput. 21(5), 1992. https://doi.org/10.1137/0221055
  • V. Dujmović, Graph layouts via layered separators, J. Combin. Theory Ser. B 110, 2015. https://doi.org/10.1016/j.jctb.2014.07.005
  • V. Dujmović, P. Morin, D. R. Wood, Layered separators in minor-closed graph classes with applications, J. Combin. Theory Ser. B 127, 2017. https://doi.org/10.1016/j.jctb.2017.05.006
  • B. Mohar, C. Thomassen, Graphs on Surfaces, Johns Hopkins University Press, 2001.
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Calculus of Variations·Captain: marwahaha

Generalized Cartan–Hadamard isoperimetry and Euclidean equality rigidityOpen Problem

Motivation

Sharp filling inequalities compare the mass of a cycle with the least mass needed to fill it. The selected formulation extends a Euclidean coefficient to proper CAT(0) metric spaces. The pinned manuscript supplies the research context.

Setting

Integral currents are encoded metric currents with integer-multiplicity chart decompositions and integral boundary. The input is a compactly supported n-cycle for n at least two. In the displayed coefficient, σ_n=(n+1)ω_{n+1}, where ω_{n+1} is the Euclidean volume of the unit ball in dimension n+1; this is the published sphereArea convention.

Formalization target

The selected goal is OAI.CAT0Fillings.sharp_integral_filling. Its central assertion is

∂S=T,M(S)≤M(T)(n+1)/n(n+1)σn1/n.\partial S=T,\qquad\mathbf M(S)\leq\frac{\mathbf M(T)^{(n+1)/n}}{(n+1)\sigma_n^{1/n}}.∂S=T,M(S)≤(n+1)σn1/n​M(T)(n+1)/n​.

The theorem states that, for a proper metric space X with its Borel σ-algebra that is CAT(0), meaning there is a choice of geodesic parametrization segment(x,y,t) from x to y (with segment(x,y,0)=x, segment(x,y,1)=y, and dist(segment(x,y,s),segment(x,y,t))=|s−t|·dist(x,y) for s,t in [0,1]) satisfying the comparison inequality dist(segment(o,x,s),segment(o,y,t))² ≤ (s·d(o,x) − t·d(o,y))² + s·t·(d(x,y)² − (d(o,x) − d(o,y))²), the following filling property holds for every integer n ≥ 2. Let T be an integral n-current on X, that is, a metric current (a multilinear functional on a bounded Lipschitz function and n Lipschitz functions, with locality, continuity and finite mass) that is a countable sum of disjointly supported integer-multiplicity bi-Lipschitz chart pieces and whose boundary has the same properties, and suppose T is compactly supported and a cycle, meaning its boundary is zero. Then there exists a compactly supported integral (n+1)-current S on X whose boundary is T and whose mass satisfies mass(S) ≤ c_n · mass(T)^((n+1)/n), where c_n = 1/((n+1)·(σ_n)^(1/n)), σ_n = (n+1)·ω_{n+1} is the area of the unit n-sphere and ω_{n+1} is the volume of the unit ball in Euclidean (n+1)-space. This is an admitted theorem statement, not a verified proof.

Significance and status

The goal is the CAT(0) integral-current filling inequality. Euclidean coefficient optimality is an additional reference. The manifold perimeter comparison and equality-rigidity statements in the manuscript are not separate attached targets. The target is currently Open on Prove2Me. The manuscript's mathematical argument and a machine-checked proof of the selected statement are separate deliverables.

Difficulty

The sharp coefficient must hold without a smooth manifold model, while preserving integrality, compact support and the exact boundary.

Formalization scope

The exact published goal, its hypotheses and its referenced definition blocks specify the requested formalization. The explanatory formula above is a summary; all quantifiers and additional clauses in the linked statement remain required.

Additional published targets are included as separate references:

  • OAI.SharpIntegralFillings.coefficient_optimal (Open).

Selected references

  • OpenAI, Generalized Cartan–Hadamard isoperimetry and Euclidean equality rigidity, preprint, 2026. Manuscript.
  • OpenAI, accompanying formal statements, commit adc7f1241b42. Selected goal source.
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Group Theory·Captain: marwahaha

A hyperbolic group with no geometric CAT(0) actionOpen Problem

Motivation

A linear filling inequality captures a form of large-scale negative curvature. The source asks whether a finite aspherical complex with that property must admit a geometric model of local nonpositive curvature. The source is OpenAI's September 2026 manuscript.

Setting

A finite complex has its usual barycentric realization. Asphericity means higher homotopy groups vanish. A linear disk-filling inequality bounds triangular face moves needed to fill an edge loop by a constant times its length.

Formalization targets

∃K:K finite, connected, aspherical, with linear disk filling,π1K hyperbolic with no geometric CAT(0) action.\exists K:\quad K\text{ finite, connected, aspherical, with linear disk filling},\quad\pi_1K\text{ hyperbolic with no geometric CAT(0) action}.∃K:K finite, connected, aspherical, with linear disk filling,π1​K hyperbolic with no geometric CAT(0) action.

The defined proposition MainStatement holds, namely that there exist a finite abstract simplicial complex K on vertices Fin n, with its standard barycentric realization |K| (nonnegative coordinate vectors summing to 1 supported on a face), a basepoint x in |K|, and a real constant C ≥ 0 such that all of the following hold. |K| is connected and aspherical at x, meaning every homotopy group π_{m}(|K|,x) with m ≥ 2 is trivial. K satisfies a linear disk-filling inequality: every closed edge path p that bounds some disk, where a disk is a chain of elementary moves (collapsing a repeated vertex, removing a spur a,b,a, or replacing a,b,c by a,c across a nondegenerate triangular face, which costs one) reducing p to a single vertex, admits such a disk using at most C times (length of p minus 1) triangular faces. The fundamental group G = π₁(|K|,x) is word hyperbolic in the four-point sense: for some finite generating set S and some δ ≥ 0, every a,b,c,d in G satisfy d(a,c)+d(b,d) ≤ max(d(a,b)+d(c,d), d(a,d)+d(b,c)) + 2δ, where d is word distance. G admits no geometric CAT(0) action: there is no proper cocompact isometric action of G on any nonempty proper complete metric space X (in universe u) that is CAT(0), in the sense that segments exist with the squared-distance comparison inequality. Finally, for every finite complex L whose realization is homotopy equivalent to |K|, there is no metric on |L|, inducing its given topology, that is geodesic and locally CAT(−1), meaning each point has a ball that satisfies the hyperbolic-cosine midpoint inequality cosh d(z,m) ≤ (cosh d(z,x)+cosh d(z,y))/(2cosh(d(x,y)/2)) for segment midpoints m.

The goal is OAI.HyperbolicObstruction.main.

Significance

The goal also excludes a finite homotopy-equivalent complex with a compatible geodesic locally CAT(-1) metric. It joins a finite topological model, a group-theoretic obstruction, and a metric-model consequence. 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

A large-scale hyperbolicity inequality does not directly construct a local curvature metric. Excluding all geometric actions requires more than finding a defect in the original complex’s chosen metric.

Formalization scope

Word hyperbolicity uses the four-point word-distance condition. Excluded CAT(0) actions are on nonempty proper complete spaces. The final metric must induce the finite realization’s existing topology; changing that topology is not permitted.

The shared definitions are supplied by HyperbolicObstruction. 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 hyperbolic group with no geometric CAT(0) action, preprint, September 2026. Manuscript.
  • OpenAI, accompanying Lean statement. Pinned source.
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Group Theory·Captain: wurtle

Quasi-isometric recognition of virtually polycyclic groupsResearch Paper

Motivation: recognizing a group from its large-scale geometry

Geometric group theory studies finitely generated groups through their word metrics, which are well defined up to quasi-isometry. A basic question is which algebraic properties are quasi-isometry invariants: if a group HHH "looks like" a group PPP from far away, must HHH share PPP's algebraic structure? Gromov's polynomial-growth theorem (1981) answers this for virtually nilpotent groups. The next natural class is the virtually polycyclic groups — groups with a finite-index subgroup admitting a finite subnormal series with cyclic factors — which are exactly, up to finite index, the lattices in connected simply connected solvable Lie groups. Eskin, Fisher and Whyte conjectured that this class is quasi-isometrically rigid, and the question had been settled only for special families such as Sol\mathrm{Sol}Sol and certain abelian-by-abelian groups.

Background

  • 1981 — Gromov: groups of polynomial growth are virtually nilpotent, which settles the virtually nilpotent case (Publ. IHÉS 1981).
  • 2000 — Farb and Mosher pose horizontal-preservation and recognition problems for solvable groups (arXiv:math/0005184).
  • 2004 — Shalom proves that a finitely generated group quasi-isometric to an infinite polycyclic group has a finite-index subgroup with infinite abelianization (Acta Math. 2004).
  • 2007 — Eskin, Fisher and Whyte formulate the lattice-recognition conjecture and its polycyclic form (Conjecture 1.2) (PAMQ 2007).
  • 2010–2013 — Dymarz treats certain diagonalizable models (GAFA 2010); Peng handles nondegenerate unimodular split abelian-by-abelian Lie groups (G&T 2011); Eskin–Fisher–Whyte prove recognition for Sol\mathrm{Sol}Sol by coarse differentiation (Ann. of Math. 2013).
  • 2025 — Dymarz, Fisher and Xie prove a Tukia-type theorem and rigidity for SOL-like groups (Adv. Math. 2025); Le Boudec proves recognition under commability (arXiv:2510.24581); Grayevsky and Pallier treat Sol5\mathrm{Sol}_5Sol5​ (arXiv:2509.12823).
  • 2026 — An OpenAI preprint, Quasi-isometric recognition of virtually polycyclic groups (OpenAI Math Release, September 24, 2026), claims recognition for the full class. The preprint has not been peer reviewed and its theorems are not formally verified.

Setting

For finitely generated groups P,HP,HP,H with word metrics, a (K,C)(K,C)(K,C)-quasi-isometry F:P→HF:P\to HF:P→H satisfies K−1d(x,x′)−C≤d(Fx,Fx′)≤Kd(x,x′)+CK^{-1}d(x,x')-C\le d(Fx,Fx')\le Kd(x,x')+CK−1d(x,x′)−C≤d(Fx,Fx′)≤Kd(x,x′)+C and has CCC-dense image. For finitely generated groups this is equivalent to a coarse equivalence: maps f:P→Hf:P\to Hf:P→H, g:H→Pg:H\to Pg:H→P sending pairs at bounded distance (differences in a fixed finite set) to pairs at bounded distance, with g∘fg\circ fg∘f and f∘gf\circ gf∘g at bounded distance from the identities. A uniform lattice in a locally compact group SSS is a discrete subgroup Λ\LambdaΛ with S=ΛKS=\Lambda KS=ΛK for a compact KKK; a lattice is a discrete subgroup whose coset space carries an SSS-invariant probability measure.

For the height theorem: a connected simply connected Lie group GGG is real-triangulable if the adjoint representation of its Lie algebra g\mathfrak gg is simultaneously upper triangular in some real basis, with diagonal characters χ1,…,χs\chi_1,\dots,\chi_sχ1​,…,χs​. Put k=⋂jker⁡χj\mathfrak k=\bigcap_j\ker\chi_jk=⋂j​kerχj​ and W=g/kW=\mathfrak g/\mathfrak kW=g/k; the exponential height map π:G→(W,+)\pi:G\to(W,+)π:G→(W,+) is the homomorphism whose differential is the quotient map. GGG is unimodular if its left Haar measure is right invariant.

Formalization targets

Milestone: uniform bounded height (Theorem 1.4)

Let GGG be connected, simply connected, real-triangulable and unimodular, with a proper left-invariant metric and a norm on WWW. There is a finite subgroup AG≤GL(W)\mathcal A_G\le\mathrm{GL}(W)AG​≤GL(W) such that for all K≥1K\ge1K≥1, C≥0C\ge0C≥0 there is BBB with: every (K,C)(K,C)(K,C) self quasi-isometry FFF of GGG has some AF∈AGA_F\in\mathcal A_GAF​∈AG​ with

∥πF(g)−πF(1)−AF π(g)∥≤B(g∈G).\bigl\|\pi F(g)-\pi F(1)-A_F\,\pi(g)\bigr\|\le B\qquad(g\in G).​πF(g)−πF(1)−AF​π(g)​≤B(g∈G).

Milestone: lattice recognition (Corollary 1.2)

If a finitely generated group HHH is quasi-isometric to a lattice in a connected simply connected solvable Lie group, then a finite-index subgroup of HHH is a uniform lattice in some (possibly different) connected simply connected solvable Lie group.

Goal: quasi-isometric recognition (Theorem 1.1)

Let PPP be finitely generated and virtually polycyclic and HHH finitely generated. If HHH is quasi-isometric to PPP, then

H is virtually polycyclic,and some finite-index Γ≤H is isomorphic to a uniform lattice in a connected simply connected solvable Lie group.H\ \text{is virtually polycyclic},\quad\text{and some finite-index } \Gamma\le H \text{ is isomorphic to a uniform lattice in a connected simply connected solvable Lie group.}H is virtually polycyclic,and some finite-index Γ≤H is isomorphic to a uniform lattice in a connected simply connected solvable Lie group.

The second clause is the classical lattice realization of virtually polycyclic groups (Dekimpe's theorem, used in the source's proof of Corollary 1.2), recorded in the same formal statement. All three statements are published on the platform with status Open: no machine-checked proofs exist yet.

Significance

The result itself. Virtual polycyclicity becomes a quasi-isometry invariant among finitely generated groups, extending Gromov's theorem from nilpotent to solvable lattices and resolving the Eskin–Fisher–Whyte conjecture in its lattice form, where the ambient Lie group may change. The bounded-height theorem is a rigidity statement for quasi-isometries of an entire class of solvable Lie groups: up to bounded error and a finite group of linear symmetries, every quasi-isometry preserves height. This is the kind of control that previously required case-by-case coarse differentiation.

Formalizing it. The proof combines Lie theory, measured couplings, reduced cohomology, volume growth, Gromov's theorem and finiteness/duality results for elementary amenable groups — a long chain in which a machine check would add real confidence. Basic objects (coarse equivalences of groups, polycyclic series, uniform lattices, Lie groups with exponential maps) are reusable across geometric group theory.

Difficulty

Quasi-isometries carry no algebraic structure and can be wild at bounded scales, so the comparison group HHH cannot be assumed solvable or even amenable a priori. Shalom's argument yields only a nontrivial homomorphism to Z\mathbb ZZ, not full structure. The geometric core is height rigidity: one must show that a quasi-isometry cannot mix "up" and "down" directions of different exponential rates, uniformly over all quasi-isometries with given constants, and with a bounded (not merely sublinear) error, which is exactly what the later group-theoretic deduction needs.

Formalization scope

  • Polycyclicity is encoded by an explicit finite cyclic subnormal series; virtual polycyclicity by a finite-index polycyclic subgroup. Quasi-isometry of finitely generated groups is encoded as GroupCoarseEquivalence, with bornologous maps and errors in finite sets — equivalent to quasi-isometry of word metrics.
  • Simply connected solvable Lie groups are bundled as SimplyConnectedSolvableLieModel (finite-dimensional charted Lie group, Hausdorff, second countable, simply connected, solvable). Uniform lattices are discrete subgroups with a compact fundamental cover; finite-covolume lattices carry an invariant probability measure on the coset space.
  • In the height theorem, real-triangulability is a TriangularAdjoint basis, WWW is any normed space linearly isomorphic to the canonical quotient, and π\piπ is characterized through an exponential map. The metric is any compatible proper left-invariant metric with linear chain bounds — a quasi-isometric generalization of the source's fixed left-invariant Riemannian metric. The finite group A\mathcal AA is chosen before K,CK,CK,C.
  • Needed infrastructure: Lie algebras of Lie groups and exponential maps, Haar measure, quasi-isometries, Gromov's theorem, and the theory of elementary amenable groups.

Selected references

  • M. Gromov, Groups of polynomial growth and expanding maps, Publ. Math. IHÉS 53 (1981), 53–78. https://doi.org/10.1007/BF02698687
  • Y. Shalom, Harmonic analysis, cohomology, and the large-scale geometry of amenable groups, Acta Math. 192 (2004), 119–185. https://doi.org/10.1007/BF02392739
  • A. Eskin, D. Fisher and K. Whyte, Quasi-isometries and rigidity of solvable groups, Pure Appl. Math. Q. 3 (2007), 927–947. https://doi.org/10.4310/PAMQ.2007.v3.n4.a3
  • A. Eskin, D. Fisher and K. Whyte, Coarse differentiation of quasi-isometries II: Rigidity for Sol and lamplighter groups, Ann. of Math. 177 (2013), 869–910. https://doi.org/10.4007/annals.2013.177.3.2
  • I. Peng, Coarse differentiation and quasi-isometries of a class of solvable Lie groups II, Geom. Topol. 15 (2011), 1927–1981. https://doi.org/10.2140/gt.2011.15.1927
  • T. Dymarz, Large scale geometry of certain solvable groups, Geom. Funct. Anal. 19 (2010), 1650–1687. https://doi.org/10.1007/s00039-010-0046-y
  • T. Dymarz, D. Fisher and X. Xie, A Tukia-type theorem for nilpotent Lie groups and quasi-isometric rigidity of solvable groups, Adv. Math. 468 (2025). https://doi.org/10.1016/j.aim.2025.110202
  • K. Dekimpe, Solvable Lie algebras, Lie groups and polynomial structures, Compos. Math. 121 (2000), 183–204. https://doi.org/10.1023/A:1001738932743
  • Y. Cornulier and R. Tessera, On the vanishing of reduced 1-cohomology for Banach representations, Ann. Inst. Fourier 70 (2020), 1951–2003. https://doi.org/10.5802/aif.3363
  • OpenAI, Quasi-isometric recognition of virtually polycyclic groups, OpenAI Math Release preprint, September 24, 2026 (source of the goal; Theorem 1.1 and Corollary 1.2, p. 2; Theorem 1.4, p. 4). https://github.com/openai/math/blob/adc7f1241b42e322a6451854ab7e4b4c146bf78a/preprints/quasi-isometric-recognition-of-virtually-polycyclic-groups-September-24-2026/paper.pdf
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Group Theory·Captain: wurtle

A Modulus Proof of Cannon’s ConjectureResearch Paper

Motivation

A finitely generated group is (word-)hyperbolic if the geodesic triangles in its Cayley graph are uniformly thin, as in the hyperbolic plane. Such a group has a boundary at infinity ∂G\partial G∂G, a compact space of asymptotic directions. The fundamental group of a closed hyperbolic 3-manifold is hyperbolic with boundary the 2-sphere. Cannon's conjecture asks for the converse: if a hyperbolic group has boundary homeomorphic to S2S^2S2, does it act geometrically on hyperbolic three-space H3\mathbb H^3H3? An affirmative answer characterizes, purely in terms of coarse geometry, which groups arise from closed hyperbolic 3-manifolds; it is one of the central problems of geometric group theory and is closely tied to the geometrization program for 3-manifolds.

Timeline

  • 1981, 1980. Sullivan and Tukia show that groups of uniformly quasiconformal maps of the sphere are conjugate to Möbius groups (Sullivan, Stony Brook 1978 proceedings; Tukia, doi:10.5186/aasfm.1980.0530).
  • 1989. Pansu introduces conformal dimension of boundaries (doi:10.5186/aasfm.1989.1424).
  • 1994. Cannon's combinatorial Riemann mapping theorem recovers quasiconformal coordinates from discrete moduli (doi:10.1007/BF02398434).
  • 1998. Cannon and Swenson state the group-boundary conjecture and relate geometric actions to conformality of boundary coverings (doi:10.1090/S0002-9947-98-02107-2).
  • 1999. Cannon, Floyd and Parry reduce the problem to bounded discrete moduli of annuli at small scales (Ann. Acad. Sci. Fenn. Math., 1999).
  • 2002, 2005. Bonk and Kleiner develop quasisymmetric uniformization of metric spheres and prove the conjecture when the Ahlfors-regular conformal dimension is attained (doi:10.1007/s00222-002-0233-z, doi:10.2140/gt.2005.9.219).
  • 2012–2013. Kahn–Marković, Bergeron–Wise, Agol and Marković connect surface subgroups, cubulation and Kleinian realizations (doi:10.4007/annals.2012.175.3.4, doi:10.4171/DM/421, doi:10.1007/s00039-013-0228-5). Bourdon and Kleiner give a combinatorial-modulus criterion for uniformization (doi:10.4171/GGD/177).
  • 2015. Haïssinsky proves a virtual Kleinian criterion for cubulated hyperbolic groups with planar boundary (doi:10.1007/s00222-014-0552-x).
  • 2026. Groves, Haïssinsky, Manning, Osajda, Sisto and Walsh reduce the residually finite case to the Toral Relative Cannon conjecture (arXiv:2406.14667).

The source of this mission, an OpenAI preprint dated September 23, 2026, follows the analytic route and proves the conjecture.

Setting

Let GGG be a group with a finite symmetric generating set SSS and Cayley graph Γ(G,S)\Gamma(G,S)Γ(G,S) with graph distance ddd. GGG is hyperbolic if there is δ\deltaδ such that every point on a side of a geodesic triangle lies within d≤δd\le\deltad≤δ of the union of the other two sides. A geodesic ray based at 111 is a sequence r0=1,r1,…r_0=1,r_1,\dotsr0​=1,r1​,… with d(ri,rj)=∣i−j∣d(r_i,r_j)=|i-j|d(ri​,rj​)=∣i−j∣; two rays are equivalent if d(rn,sn)d(r_n,s_n)d(rn​,sn​) stays bounded. The boundary ∂G\partial G∂G is the set of equivalence classes with the quotient of the topology of pointwise convergence.

H3\mathbb H^3H3 is the upper half-space {x∈R3:x3>0}\{x\in\mathbb R^3: x_3>0\}{x∈R3:x3​>0} with distance arcosh⁡(1+∣x−y∣2/(2x3y3))\operatorname{arcosh}\bigl(1+|x-y|^2/(2x_3y_3)\bigr)arcosh(1+∣x−y∣2/(2x3​y3​)), and Isom⁡(H3)\operatorname{Isom}(\mathbb H^3)Isom(H3) is its full isometry group, including orientation-reversing isometries. A homomorphism ρ:G→Isom⁡(H3)\rho:G\to\operatorname{Isom}(\mathbb H^3)ρ:G→Isom(H3) gives a proper action if {g:ρ(g)K∩K≠∅}\{g:\rho(g)K\cap K\ne\varnothing\}{g:ρ(g)K∩K=∅} is finite for every compact KKK, and a cocompact action if translates of one compact set cover H3\mathbb H^3H3.

Formalization targets

Goal: Theorem 1.1

G hyperbolic, ∂G≅S2 ⟹ ∃ ρ:G→Isom⁡(H3) proper, cocompact, with ker⁡ρ finite.G\ \text{hyperbolic},\ \partial G\cong S^2\ \Longrightarrow\ \exists\,\rho:G\to\operatorname{Isom}(\mathbb H^3)\ \text{proper, cocompact, with }\ker\rho\ \text{finite}.G hyperbolic, ∂G≅S2 ⟹ ∃ρ:G→Isom(H3) proper, cocompact, with kerρ finite.

The Lean statement OAI.CannonRelease.cannon is open on the platform.

Significance

The theorem identifies hyperbolic groups with 2-sphere boundary, up to finite kernels, with uniform lattices in Isom⁡(H3)\operatorname{Isom}(\mathbb H^3)Isom(H3). For torsion-free GGG, the quotient H3/G\mathbb H^3/GH3/G is a closed hyperbolic 3-manifold, possibly nonorientable (Corollary 8.1), and the work of Kahn–Marković, Bergeron–Wise and Agol then gives virtual structure results (Corollary 8.2). It also settles the hypotheses of the reductions of Marković and of Groves et al. in full generality.

The result is proved in an OpenAI preprint; it has not been peer reviewed, and no machine-checked proof exists. A formal proof would require formal infrastructure for hyperbolic groups and their boundaries, quasiconformal analysis and combinatorial modulus, very little of which is currently in Mathlib.

Difficulty

By the Cannon–Floyd–Parry and Bourdon–Kleiner criteria, the theorem reduces to a uniform upper bound on the combinatorial 2-modulus of curve families at all scales of the boundary. The bound is easy to state but there is no a priori reason why moduli of coverings of a topological sphere should stay bounded; Bonk–Kleiner needed the extra hypothesis that the conformal dimension is attained. A proof must extract analytic control (a nonconstant limit function with controlled oscillation) from a hypothetical sequence of coverings with unbounded modulus and contradict it using only hyperbolicity and the topology of the boundary.

Formalization scope

  • CayleyData G is a finite symmetric generating set with connected SimpleGraph.mulCayley; ThinTriangles asks for one natural number δ\deltaδ working for all geodesic triangles given as walks of length equal to graph distance.
  • Rays are ℕ → G with r 0 = 1 and dist (r i) (r j) = |i-j|; the boundary is the quotient by bounded synchronous distance. GGG carries the discrete topology, rays the subspace product topology, and the boundary the quotient topology, which coincides with the visual topology for hyperbolic groups.
  • S2S^2S2 is the unit sphere in EuclideanSpace ℝ (Fin 3); H3\mathbb H^3H3 is the upper half-space with the explicit arcosh distance and subspace topology; isometries are self-homeomorphisms preserving that distance.
  • The kernel is only required to be finite, and orientation-reversing elements are allowed, matching the paper.

A complete development needs Gromov hyperbolic groups and visual metrics, approximately self-similar spheres, combinatorial modulus and the Bonk–Kleiner/Bourdon–Kleiner uniformization criterion, and the Sullivan–Tukia straightening of uniformly quasiconformal groups. Contributions formalizing Proposition 2.6 (from a round boundary action to a geometric action on H3\mathbb H^3H3) or Theorem 2.5 (the uniformization criterion) are welcome.

Selected references

  • OpenAI, A Modulus Proof of Cannon's Conjecture, preprint, September 23, 2026. https://github.com/openai/math/blob/adc7f1241b42e322a6451854ab7e4b4c146bf78a/preprints/A-Modulus-Proof-of-Cannons-Conjecture-September-23-2026/paper.pdf
  • J. W. Cannon, The combinatorial Riemann mapping theorem, Acta Math., 1994. https://doi.org/10.1007/BF02398434
  • J. W. Cannon, E. L. Swenson, Recognizing constant curvature discrete groups in dimension 3, Trans. Amer. Math. Soc., 1998. https://doi.org/10.1090/S0002-9947-98-02107-2
  • J. W. Cannon, W. J. Floyd, W. R. Parry, Sufficiently rich families of planar rings, Ann. Acad. Sci. Fenn. Math., 1999. https://www.acadsci.fi/mathematica/Vol24/cannon.pdf
  • M. Bonk, B. Kleiner, Quasisymmetric parametrizations of two-dimensional metric spheres, Invent. Math., 2002. https://doi.org/10.1007/s00222-002-0233-z
  • M. Bonk, B. Kleiner, Conformal dimension and Gromov hyperbolic groups with 2-sphere boundary, Geom. Topol., 2005. https://doi.org/10.2140/gt.2005.9.219
  • M. Bourdon, B. Kleiner, Combinatorial modulus, the combinatorial Loewner property, and Coxeter groups, Groups Geom. Dyn., 2013. https://doi.org/10.4171/GGD/177
  • V. Marković, Criterion for Cannon's conjecture, Geom. Funct. Anal., 2013. https://doi.org/10.1007/s00039-013-0228-5
  • P. Haïssinsky, Hyperbolic groups with planar boundaries, Invent. Math., 2015. https://doi.org/10.1007/s00222-014-0552-x
  • D. Groves, P. Haïssinsky, J. F. Manning, D. Osajda, A. Sisto, G. S. Walsh, Drilling hyperbolic groups, preprint, 2026. https://arxiv.org/abs/2406.14667
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Analysis·Captain: wurtle

Koebe's Circle-Domain ConjectureResearch Paper

Motivation

The Riemann mapping theorem says that every simply connected proper domain in the plane is conformally equivalent to the unit disk. For domains with more complicated complements one needs a model with many "holes". Koebe's Kreisnormierungsproblem (1908) asks whether every domain in the Riemann sphere is conformally equivalent to a circle domain, one whose complementary components are all round disks or points. Such a model would give a canonical geometric picture of an arbitrary planar domain, and it is closely tied to circle packings, Kleinian groups and the geometry of hyperbolic surfaces of genus zero.

Timeline

  • 1908. Koebe poses the problem (Nachr. Ges. Wiss. Göttingen, 1908).
  • 1920. Koebe's treatment of the finitely connected case (doi:10.1007/BF01199400).
  • 1993. He and Schramm prove the conjecture for countably connected domains (doi:10.2307/2946541).
  • 1995. Schramm introduces transboundary extremal length and treats domains bounded by points and KKK-quasicircles (doi:10.1007/BF02788827).
  • 2025. Rajala shows that arbitrary interior exhaustions can fail to have circle-domain limits and proves an exhaustion refinement theorem for countably connected domains (doi:10.1353/ajm.2025.a966291); Ntalampekos and Rajala study exhaustions of circle domains (arXiv:2312.06840).
  • 2026. Esmayli and Rajala prove uniformization for cospread domains and under a quasitripod condition (arXiv:2401.08485); Karafyllia and Ntalampekos treat spherical Gromov-hyperbolic domains (arXiv:2405.13782). Ntalampekos surveys the area (arXiv:2603.15098).

The source of this mission, an OpenAI preprint dated September 23, 2026, claims the conjecture in its unrestricted form.

Setting

The Riemann sphere is C^=C∪{∞}\widehat{\mathbb C}=\mathbb C\cup\{\infty\}C=C∪{∞}, with local coordinate zzz near finite points and 1/z1/z1/z near ∞\infty∞. A domain is a nonempty connected open subset. A map fff is conformal at ppp if it is continuous at ppp and, in these coordinates, complex differentiable at ppp with nonzero derivative. A conformal equivalence f:U→Vf:U\to Vf:U→V is a bijection that is conformal at every point of UUU and whose inverse is conformal at every point of VVV.

A closed round disk in C^\widehat{\mathbb C}C is the image of the closed unit disk under a Möbius transformation z↦(az+b)/(cz+d)z\mapsto (az+b)/(cz+d)z↦(az+b)/(cz+d), ad−bc≠0ad-bc\ne0ad−bc=0; these are closed Euclidean disks, closed half-planes together with ∞\infty∞, and complements of open disks. A circle domain is a domain each of whose complementary connected components is a closed round disk or a single point. The complement may be empty, finite, countable or uncountable.

Formalization targets

Goal: Theorem 1.1 (circle-domain uniformization)

∀ G⊂C^ domain∃ Ω circle domain, ∃ f:G→ conformal Ω bijective.\forall\,G\subset\widehat{\mathbb C}\ \text{domain}\quad\exists\,\Omega\ \text{circle domain},\ \exists\,f:G\xrightarrow{\ \text{conformal}\ }\Omega\ \text{bijective}.∀G⊂C domain∃Ω circle domain, ∃f:G conformal ​Ω bijective.

Lean: OAI.Problem047.koebe_circle_domain, open on the platform.

Significance

The theorem would complete the existence half of Koebe's problem with no restriction on the number, size or geometry of the complementary components. The paper derives a consequence for hyperbolic geometry (Corollary 8.1): every complete hyperbolic surface of genus zero is isometric to the boundary of the convex hull of a closed set in ∂∞H3\partial_\infty\mathbb H^3∂∞​H3 whose components are round disks or points. Combined with the exhaustion theorem of Ntalampekos and Rajala, it also gives convergent finitely connected approximations for every proper domain. Uniqueness up to Möbius maps is a different question (the He–Schramm rigidity conjecture), addressed in the companion mission on removable boundaries.

The result is claimed in an OpenAI preprint that has not been peer reviewed; no machine-checked proof exists. Mathlib has neither the Riemann mapping theorem in full generality nor finitely connected circle-domain uniformization, so a formal proof would build substantial reusable complex-analytic infrastructure.

Difficulty

The standard approach uniformizes finitely connected approximations, whose complements are finitely many round disks, and passes to a limit. The difficulty is control at the limit: with possibly uncountably many complementary components, a limiting component can be strictly larger than the round disk obtained by following one approximating disk, or can be a non-round continuum for which no disk was followed at all. Rajala showed that arbitrary exhaustions can indeed fail to produce circle-domain limits, so the approximations must be chosen with care, and all components must be controlled simultaneously, not one at a time.

Formalization scope

  • Sphere := OnePoint ℂ; Möbius maps are Matrix.GeneralLinearGroup (Fin 2) ℂ acting on it.
  • IsConformalAt f p: ContinuousAt f p and a nonzero HasDerivAt of fff in the charts chart p, chart (f p) (identity coordinate at finite points, z↦1/zz\mapsto1/zz↦1/z at ∞\infty∞).
  • IsConformalEquivalence f U V: fff conformal on UUU, MapsTo f U V, and a conformal g on VVV with MapsTo g V U that is a two-sided inverse.
  • IsCircleDomain V: open, IsConnected (hence nonempty), and every connectedComponentIn Vᶜ p is a singleton or IsRoundClosedDisk (a Möbius image of the closed unit disk).
  • The goal quantifies over all open connected U; there is no countability or regularity assumption on the complement.

A complete development needs finitely connected uniformization, normal families on the sphere, Dirichlet energy and extremal length, and component correspondence for limits. Contributions formalizing the named intermediate results (Theorem 3.1 finite transfer, Theorem 4.3 compatible barrier lemma, Theorem 5.1 positive-law alternative, Theorem 7.5 retained-test transfer) or the classical He–Schramm countable case are welcome.

Selected references

  • OpenAI, Koebe's Circle-Domain Conjecture, preprint, September 23, 2026. https://github.com/openai/math/blob/adc7f1241b42e322a6451854ab7e4b4c146bf78a/preprints/Koebes-Circle-Domain-Conjecture-September-23-2026/paper.pdf
  • P. Koebe, Über die Uniformisierung beliebiger analytischer Kurven (Dritte Mitteilung), Nachr. Ges. Wiss. Göttingen, 1908.
  • P. Koebe, Abhandlungen zur Theorie der konformen Abbildung VI, Math. Z., 1920. https://doi.org/10.1007/BF01199400
  • Z.-X. He, O. Schramm, Fixed points, Koebe uniformization and circle packings, Ann. of Math., 1993. https://doi.org/10.2307/2946541
  • O. Schramm, Transboundary extremal length, J. Analyse Math., 1995. https://doi.org/10.1007/BF02788827
  • K. Rajala, Uniformization of planar domains by exhaustion, Amer. J. Math., 2025. https://doi.org/10.1353/ajm.2025.a966291
  • D. Ntalampekos, K. Rajala, Exhaustions of circle domains, IMRN, 2025. https://doi.org/10.1093/imrn/rnaf296
  • B. Esmayli, K. Rajala, Conformal uniformization of domains bounded by quasitripods, Duke Math. J., 2026. https://doi.org/10.1215/00127094-2025-0035
  • C. Karafyllia, D. Ntalampekos, Uniformization of Gromov hyperbolic domains by circle domains, Duke Math. J., 2026. https://doi.org/10.1215/00127094-2025-0076
  • D. Ntalampekos, Uniformization problems in the plane: A survey, preprint, 2026. https://arxiv.org/abs/2603.15098
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Analysis·Captain: wurtle

Removable Boundaries and Rigidity of Circle DomainsResearch Paper

Motivation

A circle domain is a domain in the Riemann sphere whose complementary components are round disks or points. Koebe asked in 1908 whether every domain is conformally equivalent to a circle domain (existence). A second question is rigidity: when is that circle-domain model unique up to Möbius transformations? For finitely and countably connected domains the model is unique, but for domains with uncountably many boundary components uniqueness can fail, and the boundary geometry decides. He and Schramm conjectured that a circle domain is rigid exactly when its boundary is conformally removable. Rigidity is what makes the circle-domain model canonical, and it connects conformal geometry with removability questions for quasiconformal and Sobolev maps.

Timeline

  • 1993. He and Schramm prove uniformization and rigidity for countably connected circle domains (doi:10.2307/2946541).
  • 1994. He and Schramm prove rigidity when the boundary has σ\sigmaσ-finite linear measure, and conjecture that rigidity is equivalent to conformal removability of the boundary (doi:10.1007/BF01231761).
  • 2000. Jones and Smirnov relate removability for continuous Sobolev functions to quasiconformal removability (doi:10.1007/BF02384320).
  • 2016. Younsi proves that conformal rigidity is equivalent to quasiconformal rigidity and studies the removability formulations (doi:10.1016/j.aim.2016.08.039).
  • 2020. Ntalampekos and Younsi prove rigidity under square integrability of the quasihyperbolic distance, covering Hölder and John circle domains (doi:10.1007/s00222-019-00921-1).
  • 2023–2024. Ntalampekos proves rigidity when point components are countably negligible for extremal distance (CNED) and continuous Sobolev extension across closed CNED sets (doi:10.1090/tran/8923, doi:10.1007/s00029-024-00951-5).
  • 2025. Rajala constructs a rigid circle domain with non-removable boundary, so rigidity does not imply removability (doi:10.1112/plms.70081).

The source of this mission, an OpenAI preprint dated September 23, 2026, claims the remaining implication: removability implies rigidity.

Setting

The Riemann sphere C^=C∪{∞}\widehat{\mathbb C}=\mathbb C\cup\{\infty\}C=C∪{∞} has local coordinates zzz and 1/z1/z1/z. A map is conformal at ppp if it is continuous there and complex differentiable with nonzero derivative in these coordinates; a conformal equivalence f:Ω→Ω′f:\Omega\to\Omega'f:Ω→Ω′ is a bijection, conformal on Ω\OmegaΩ, with conformal inverse. A Möbius transformation is z↦(az+b)/(cz+d)z\mapsto(az+b)/(cz+d)z↦(az+b)/(cz+d) with ad−bc≠0ad-bc\neq0ad−bc=0. A closed round disk is the Möbius image of the closed unit disk. A circle domain is a nonempty connected open set whose complementary components are closed round disks or points.

A compact E⊂C^E\subset\widehat{\mathbb C}E⊂C is conformally removable if every orientation-preserving homeomorphism of C^\widehat{\mathbb C}C that is conformal on C^∖E\widehat{\mathbb C}\setminus EC∖E is Möbius. A circle domain Ω\OmegaΩ is conformally rigid if every conformal equivalence from Ω\OmegaΩ onto another circle domain is the restriction of a Möbius transformation.

Formalization targets

Goal: Theorem 1.1

Ω,Ω′ circle domains,  ∂Ω conformally removable,  f:Ω→Ω′ conformal equivalence ⟹ ∃M Mo¨bius: f=M∣Ω.\Omega,\Omega'\ \text{circle domains},\ \ \partial\Omega\ \text{conformally removable},\ \ f:\Omega\to\Omega'\ \text{conformal equivalence}\ \Longrightarrow\ \exists M\ \text{Möbius}:\ f=M|_\Omega.Ω,Ω′ circle domains,  ∂Ω conformally removable,  f:Ω→Ω′ conformal equivalence ⟹ ∃M Mo¨bius: f=M∣Ω​.

Lean: OAI.Problem047.removability_implies_rigidity, open on the platform. The complement may have any cardinality, and no boundary extension of fff is assumed.

Significance

Together with Rajala's counterexample to the converse, the theorem would settle the He–Schramm rigidity conjecture: removability is sufficient but not necessary. It subsumes the earlier sufficient conditions (σ\sigmaσ-finite length, Hölder/John domains, CNED point sets) whenever those boundaries are removable. The intermediate Theorem 5.1, a continuous Sobolev extension theorem across compact totally disconnected conformally removable sets, is of independent interest. The result is claimed in an OpenAI preprint that has not been peer reviewed, and no machine-checked proof exists.

Difficulty

Removability is a statement about homeomorphisms of the whole sphere, while rigidity starts from a map defined only on the domain. The obvious route, extending fff to a homeomorphism of the sphere and then invoking removability, fails: a point component of the complement of Ω\OmegaΩ may correspond to a disk component of Ω′\Omega'Ω′ and vice versa, so the coordinates of fff need not extend continuously, and nothing a priori controls boundary behaviour at uncountably many point components whose union can have positive area.

Formalization scope

  • Sphere := OnePoint ℂ, Möbius maps are Matrix.GeneralLinearGroup (Fin 2) ℂ acting on it; conformality uses the charts zzz and 1/z1/z1/z with HasDerivAt and a nonzero derivative.
  • IsCircleDomain: open, IsConnected, and every connectedComponentIn of the complement is a singleton or a Möbius image of the closed unit disk.
  • IsConformallyRemovable E: IsCompact E and every homeomorphism h : Sphere ≃ₜ Sphere that is homotopic to the identity (orientation preserving) and conformal on Eᶜ equals some Möbius map everywhere.
  • The boundary is frontier U; the conclusion is ∃ M, ∀ p ∈ U, f p = M • p.
  • The shared definitions are those of the Koebe circle-domain mission of the same family.

A complete development needs the theory of conformal maps on the sphere, Sobolev functions and Dirichlet energy in the plane, the measurable Riemann mapping theorem (used for the conductivity deformation), and component correspondence. Contributions formalizing Theorem 5.1 (continuous Sobolev extension), Proposition 6.2 (common point traces), or the He–Schramm countable case are welcome.

Selected references

  • OpenAI, Removable Boundaries and Rigidity of Circle Domains, preprint, September 23, 2026. https://github.com/openai/math/blob/adc7f1241b42e322a6451854ab7e4b4c146bf78a/preprints/Removable-Boundaries-and-Rigidity-of-Circle-Domains-September-23-2026/paper.pdf
  • Z.-X. He, O. Schramm, Fixed points, Koebe uniformization and circle packings, Ann. of Math., 1993. https://doi.org/10.2307/2946541
  • Z.-X. He, O. Schramm, Rigidity of circle domains whose boundary has σ-finite linear measure, Invent. Math., 1994. https://doi.org/10.1007/BF01231761
  • M. Younsi, Removability, rigidity of circle domains and Koebe's conjecture, Adv. Math., 2016. https://doi.org/10.1016/j.aim.2016.08.039
  • D. Ntalampekos, M. Younsi, Rigidity theorems for circle domains, Invent. Math., 2020. https://doi.org/10.1007/s00222-019-00921-1
  • D. Ntalampekos, Rigidity and continuous extension for conformal maps of circle domains, Trans. Amer. Math. Soc., 2023. https://doi.org/10.1090/tran/8923
  • D. Ntalampekos, CNED sets: countably negligible for extremal distances, Selecta Math., 2024. https://doi.org/10.1007/s00029-024-00951-5
  • P. W. Jones, S. K. Smirnov, Removability theorems for Sobolev functions and quasiconformal maps, Ark. Mat., 2000. https://doi.org/10.1007/BF02384320
  • K. Rajala, Rigid circle domains with non-removable boundaries, Proc. Lond. Math. Soc., 2025. https://doi.org/10.1112/plms.70081
  • OpenAI, Koebe's Circle-Domain Conjecture, preprint, September 23, 2026.
2 thms1 active userReviewed
Dynamical SystemsSymplectic Geometry·Captain: Mazecto

Hryniewicz's Criterion: Disk-like Global Sections of Dynamically Convex Reeb Flows on S³Research Paper

Motivation

A global surface of section reduces a flow on a closed 3-manifold to an area-preserving map of a surface. It is a compact embedded surface whose boundary consists of periodic orbits, whose interior is transverse to the flow, and which every other trajectory hits infinitely often in forward and backward time. Poincaré introduced the idea for the restricted three-body problem. Once a section is a disk, results on area-preserving disk maps (Brouwer, Franks) give periodic orbits and other structure for the whole flow.

For Hamiltonian flows on star-shaped energy surfaces in R4\mathbb{R}^4R4, equivalently Reeb flows on the tight 3-sphere, it is natural to ask which periodic orbits bound such a disk. Hryniewicz's criterion answers this for dynamically convex flows, with no genericity assumption. The answer is purely topological: a periodic orbit bounds a disk-like global section exactly when it is unknotted with self-linking number −1-1−1. The criterion is used in celestial mechanics: Joung and van Koert apply it to validated periodic orbits of the restricted three-body problem (arXiv:2407.19159).

Timeline.

  • 1998. Hofer, Wysocki and Zehnder prove that every dynamically convex contact form on S3S^3S3 has some periodic orbit P0P_0P0​, with Conley–Zehnder index 333, that bounds a disk-like global section. That disk is a page of an open book adapted to the flow. Strictly convex energy surfaces in R4\mathbb{R}^4R4 are dynamically convex (Ann. of Math. 148).
  • 2008/2012. Hryniewicz proves the "unknotted, self-linking −1-1−1" characterization in the non-degenerate case (arXiv:0812.4076).
  • 2010/2011. Hryniewicz and Salomão treat non-degenerate tight contact forms on S3S^3S3. Two extra conditions appear there: μCZ≥3\mu_{CZ}\ge 3μCZ​≥3, and linking with every orbit of index 222 (arXiv:1006.0049).
  • 2011/2014. Hryniewicz removes non-degeneracy for dynamically convex forms (arXiv:1105.2077, Theorem 1.7). In the same paper, Theorem 1.8 shows that any orbit coming from a fixed point of the first-return map of a disk-like section is again such a binding.
  • 2012. Albers, Fish, Frauenfelder, Hofer and van Koert use this circle of ideas to get disk-like sections in the planar circular restricted three-body problem (arXiv:1103.3881).

Setting

Use coordinates x=(q1,p1,q2,p2)x=(q_1,p_1,q_2,p_2)x=(q1​,p1​,q2​,p2​) on R4\mathbb{R}^4R4, the Liouville form λ0=12∑j(qj dpj−pj dqj)\lambda_0=\tfrac12\sum_j (q_j\,dp_j-p_j\,dq_j)λ0​=21​∑j​(qj​dpj​−pj​dqj​) and the symplectic form ω0=dλ0=∑jdqj∧dpj\omega_0=d\lambda_0=\sum_j dq_j\wedge dp_jω0​=dλ0​=∑j​dqj​∧dpj​.

Let H:R4→RH:\mathbb{R}^4\to\mathbb{R}H:R4→R be smooth and set S=H−1(1)S=H^{-1}(1)S=H−1(1). Assume that every ray from the origin meets SSS exactly once, and that it crosses SSS transversally:

dH(x) x>0(x∈S).dH(x)\,x>0\qquad(x\in S).dH(x)x>0(x∈S).

Then SSS is a strictly star-shaped hypersurface diffeomorphic to S3S^3S3. Every contact form on S3S^3S3 that matters below arises this way, up to diffeomorphism (see Formalization scope).

The Hamiltonian vector field XHX_HXH​ is defined by ιXHω0=−dH\iota_{X_H}\omega_0=-dHιXH​​ω0​=−dH. With this sign, λ0(XH)=12 dH(x) x>0\lambda_0(X_H)=\tfrac12\,dH(x)\,x>0λ0​(XH​)=21​dH(x)x>0 on SSS. So XH∣SX_H|_SXH​∣S​ is a positive multiple of the Reeb vector field of the contact form λ0∣S\lambda_0|_Sλ0​∣S​, and its orbits are the Reeb orbits reparametrized. A periodic orbit P=(x,T)P=(x,T)P=(x,T) is a solution with x(T)=x(0)x(T)=x(0)x(T)=x(0) and T>0T>0T>0. It is prime when TTT is its least positive period. The contact structure is ξ=ker⁡λ0∣S\xi=\ker\lambda_0|_Sξ=kerλ0​∣S​.

  • Conley–Zehnder index. Fix the global frame of ξ\xiξ given by the quaternionic rotations of ∇H\nabla H∇H. Along PPP, the linearized flow restricted to ξ\xiξ is a path φ:[0,1]→Sp(1)\varphi:[0,1]\to Sp(1)φ:[0,1]→Sp(1) with φ(0)=I\varphi(0)=Iφ(0)=I. The winding interval I(φ)I(\varphi)I(φ) collects the total rotations of all nonzero vectors, measured in turns. Then μCZ(P)\mu_{CZ}(P)μCZ​(P) is the lower semicontinuous index of Hryniewicz's §2.1.1. In particular,
μCZ(P)≥3  ⟺  min⁡I(φ)>1,\mu_{CZ}(P)\ge 3 \iff \min I(\varphi)>1,μCZ​(P)≥3⟺minI(φ)>1,

that is, every nonzero transverse vector turns by more than one full turn.

  • Dynamical convexity. The flow is dynamically convex if μCZ(P)≥3\mu_{CZ}(P)\ge 3μCZ​(P)≥3 for every periodic orbit PPP in SSS, prime or multiply covered.
  • Disk-like global surface of section. A smoothly embedded closed disk D⊂SD\subset SD⊂S such that ∂D=x(R)\partial D=x(\mathbb{R})∂D=x(R) for a periodic orbit PPP, XHX_HXH​ is transverse to D∖∂DD\setminus\partial DD∖∂D, and every trajectory not contained in ∂D\partial D∂D meets DDD at arbitrarily large positive and negative times. Then PPP bounds DDD.
  • Unknotted. PPP is unknotted if x(R)x(\mathbb{R})x(R) is the boundary of some smoothly embedded closed disk in SSS.
  • Self-linking number. Push xxx off itself along the global frame of ξ\xiξ to a disjoint loop x′x'x′. Then
sl⁡(P)=lk⁡(x,x′)∈Z,\operatorname{sl}(P)=\operatorname{lk}(x,x')\in\mathbb{Z},sl(P)=lk(x,x′)∈Z,

the linking number in S≅S3S\cong S^3S≅S3, with SSS oriented as the boundary of the star-shaped domain it bounds. This agrees with Hryniewicz's Definition 1.5, which uses a section of ξ\xiξ over a spanning disk.

Formalization targets

Goal: Hryniewicz's criterion (Theorem 1.7, first sentence)

For every dynamically convex strictly star-shaped SSS and every prime periodic orbit Pˉ\bar PPˉ:

Pˉ bounds a disk-like global surface of section  ⟺  Pˉ is unknotted and sl⁡(Pˉ)=−1.\bar P \text{ bounds a disk-like global surface of section} \iff \bar P \text{ is unknotted and } \operatorname{sl}(\bar P)=-1.Pˉ bounds a disk-like global surface of section⟺Pˉ is unknotted and sl(Pˉ)=−1.

The statement fixes no constants and no non-degeneracy, and it covers every dynamically convex star-shaped surface.

Stronger: adapted open book (Theorem 1.7, second sentence)

If Pˉ\bar PPˉ is unknotted with sl⁡(Pˉ)=−1\operatorname{sl}(\bar P)=-1sl(Pˉ)=−1, then S∖xˉ(R)S\setminus \bar x(\mathbb{R})S∖xˉ(R) fibres smoothly over R/Z\mathbb{R}/\mathbb{Z}R/Z. Every fibre is the interior of a disk-like global surface of section whose oriented boundary is Pˉ\bar PPˉ.

Further: new bindings from fixed points (Theorem 1.8)

Let D0D_0D0​ be any disk-like global section. Every periodic orbit through a fixed point of the first-return map of D0∖∂D0D_0\setminus\partial D_0D0​∖∂D0​ is unknotted, has self-linking number −1-1−1, and so bounds the page of an adapted open book.

Significance

The result. The criterion turns a dynamical question into a topological check. It does not depend on whether the orbit is degenerate, and degenerate orbits are what one meets at bifurcations and on symmetric levels. Every periodic orbit in a strictly convex energy surface that is unknotted with sl⁡=−1\operatorname{sl}=-1sl=−1 is a binding, so the flow is organised by many open books at once. Theorem 1.8 makes this concrete: the Hamiltonian flow twists around two different bindings, ∂D0\partial D_0∂D0​ and ∂D1\partial D_1∂D1​. In applications, numerically validated orbits become analytic global sections without a separate non-degeneracy check (Joung–van Koert, Theorems 1.2 and 1.5).

Formalizing it. The theorem is proved, in a 50-page paper that relies on Hofer–Wysocki–Zehnder's theory of pseudo-holomorphic curves in symplectizations. It has no machine-checked proof. Mathlib has no Conley–Zehnder index, no self-linking number, no linking number of curves in S3S^3S3, and no global surfaces of section. A Lean statement fixes every sign and orientation convention involved: the sign of XHX_HXH​, the orientation of SSS, which push-off defines sl⁡\operatorname{sl}sl, and the index of degenerate orbits. Each of these is easy to get wrong in prose. Formal proofs of the parts that use no holomorphic curves are valuable on their own: the necessity direction, the description of the index by winding intervals, and the explicit ellipsoid examples.

Difficulty

The obvious route is to approximate the contact form by non-degenerate forms λk→λ\lambda_k\to\lambdaλk​→λ that keep Pˉ\bar PPˉ as an orbit, and then apply the non-degenerate theorems. This fails. The λk\lambda_kλk​ need not be dynamically convex. They can have orbits of very high action with μCZ=2\mu_{CZ}=2μCZ​=2 that are not linked with Pˉ\bar PPˉ, so the Hryniewicz–Salomão criterion does not apply to λk\lambda_kλk​ (Hryniewicz, p. 4). The families of planes that would give the pages for λk\lambda_kλk​ have to be controlled directly as k→∞k\to\inftyk→∞, and this is not a formal limit argument.

A second obstruction is genuinely global. A disk spanning Pˉ\bar PPˉ and transverse to the flow in its interior is easy to produce when sl⁡(Pˉ)=−1\operatorname{sl}(\bar P)=-1sl(Pˉ)=−1. Showing that every trajectory returns to it is the whole content of the theorem, and no local or perturbative argument gives it.

For the formalization, nothing in the proof of sufficiency avoids finite-energy pseudo-holomorphic planes: Fredholm theory, asymptotic analysis, bubbling-off and compactness all enter. None of this exists in Lean.

Formalization scope

  • Ambient space. R4\mathbb{R}^4R4 is Fin 4 → ℝ with coordinates ordered (q1,p1,q2,p2)(q_1,p_1,q_2,p_2)(q1​,p1​,q2​,p2​). λ0\lambda_0λ0​, ω0\omega_0ω0​ and XHX_HXH​ are defined explicitly, with the sign conventions above.
  • Energy surfaces. Star-shaped surfaces are smooth (ContDiff ℝ ⊤) functions HHH with the ray condition and dH(x)x>0dH(x)x>0dH(x)x>0 on H−1(1)H^{-1}(1)H−1(1). The Reeb flow of a general dynamically convex form on S3S^3S3 reduces to this case, up to diffeomorphism and positive time change: such a form is tight (Hofer–Wysocki–Zehnder), and every tight form on S3S^3S3 comes from a star-shaped hypersurface (Eliashberg 1992). That reduction is not part of the targets. Hryniewicz makes the same reduction (§3, first paragraph).
  • Flow. The flow is the flow of XHX_HXH​, not of the Reeb field. All notions in the targets are invariant under positive time change. Periodic orbits are solutions of x˙=XH(x)\dot x=X_H(x)x˙=XH​(x) on all of R\mathbb{R}R. "Prime" means the recorded period is least.
  • Index. μCZ≥3\mu_{CZ}\ge 3μCZ​≥3 is encoded by the winding-interval condition in the global quaternionic frame, with degenerate orbits included. Multiply covered orbits are included in dynamical convexity.
  • Disks. Disks are smooth embeddings of the closed unit disk (injective, with injective differential up to the boundary). The return condition demands hits at arbitrarily large positive and negative times.
  • Ruling out vacuous encodings. A version without the two-sided return condition, with a dynamical-convexity predicate that no surface satisfies, or with sl⁡\operatorname{sl}sl that is not a linking number of the push-off, proves a different theorem. The ellipsoid milestone below is a non-vacuity check on the definitions.
  • Infrastructure. A complete development needs the following.
    • Reusable beyond this mission: the Conley–Zehnder index of paths in Sp(1)Sp(1)Sp(1), the linking number of disjoint loops in S3S^3S3 (or in R3\mathbb{R}^3R3 after stereographic projection), and global flows of vector fields on compact level sets.
    • Specific to this proof: contact topology of spanning disks (characteristic foliations, elimination of singularities), and finite-energy planes in R×S3\mathbb{R}\times S^3R×S3 with their Fredholm, asymptotic and compactness theory.
  • Contributions welcome. The definition layer, the index and linking-number libraries, the ellipsoid examples, Lemma 2.1, the necessity direction, Lemma 3.12, and any sub-step of the holomorphic-curve argument stated as an independent lemma.

Selected references

  • H. Hofer, K. Wysocki, E. Zehnder, The dynamics on three-dimensional strictly convex energy surfaces, Ann. of Math. 148 (1998), 197–289. https://doi.org/10.2307/120994
  • U. L. Hryniewicz, Fast finite-energy planes in symplectizations and applications, Trans. Amer. Math. Soc. 364 (2012), 1859–1931. https://arxiv.org/abs/0812.4076
  • U. L. Hryniewicz, P. A. S. Salomão, On the existence of disk-like global sections for Reeb flows on the tight 3-sphere, Duke Math. J. 160 (2011), 415–465. https://arxiv.org/abs/1006.0049
  • U. L. Hryniewicz, Systems of global surfaces of section for dynamically convex Reeb flows on the 3-sphere, J. Symplectic Geom. 12 (2014), 791–862. https://arxiv.org/abs/1105.2077
  • U. L. Hryniewicz, P. A. S. Salomão, Global surfaces of section for Reeb flows in dimension three and beyond, Proc. ICM 2018 (extended version). https://arxiv.org/abs/1712.01925
  • P. Albers, J. W. Fish, U. Frauenfelder, H. Hofer, O. van Koert, Global surfaces of section in the planar restricted 3-body problem, Arch. Ration. Mech. Anal. 204 (2012), 273–284. https://arxiv.org/abs/1103.3881
  • C. Joung, O. van Koert, Computational symplectic topology and symmetric orbits in the restricted three-body problem, Nonlinearity 38 (2025), 025015. https://arxiv.org/abs/2407.19159
  • Y. Eliashberg, Contact 3-manifolds twenty years since J. Martinet's work, Ann. Inst. Fourier 42 (1992), 165–192. https://doi.org/10.5802/aif.1288
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Analysis·Captain: Tamas Fulop

Moving Sofa ProblemOpen Problem

Motivation

The question of the largest area that can be moved around a corner has been studied since the late 1960s. Leo Moser posed it in 1966, and F. H. Hammersley gave the lower bound π/2+2/π≈2.2074\pi/2+2/\pi\approx2.2074π/2+2/π≈2.2074 and the upper bound 22≈2.8282\sqrt{2}\approx2.82822​≈2.828 in 1968. Joseph Gerver constructed a shape of area approximately 2.21952.21952.2195 in 1992 and described four constants AAA, BBB, φ\varphiφ, θ\thetaθ satisfying four equations, from which the shape is built. Dan Romik rewrote those equations in exact form as equations (1)-(4) in 2018 and reported high-precision values of the constants. Jineon Baek proved in 2024 that Gerver's shape is optimal: no larger shape can be moved around the corner. The proof was autoformalized in Lean 4 by Dean Cureton and AI agents in 2026, as the repository deancureton/MovingSofa, building on Dawid Trela's formalization of Gerver's constants and motion, Jonathan Ho's Brunn-Minkowski development, the Jordan-curve developments of R. Kirov and the TauCeti project, and Google DeepMind's formal-conjectures statement.

Timeline: Moser poses the problem (1966); Hammersley gives the π/2+2/π≈2.2074\pi/2+2/\pi\approx2.2074π/2+2/π≈2.2074 lower bound and the 22≈2.8282\sqrt{2}\approx2.82822​≈2.828 upper bound (1968); Gerver exhibits the 2.21952.21952.2195 shape and its differential equations (1992); Romik gives the exact equations and numerics (2018); Baek proves optimality (2024, arXiv:2411.19826); Cureton et al. complete a Lean 4 proof of optimality, existence and uniqueness of the constants, and movability of Gerver's shape (2026).

Setting

Work in the plane R2\mathbb{R}^2R2. The hallway is (−∞,1]×[0,1]∪[0,1]×(−∞,1](-\infty,1]\times[0,1]\cup[0,1]\times(-\infty,1](−∞,1]×[0,1]∪[0,1]×(−∞,1], the union of its horizontal and vertical sides. A moving sofa is a nonempty closed connected set sss in the horizontal side together with a continuous path mmm of plane isometries indexed by the unit interval, starting at the identity, keeping the image of sss inside the hallway at all times, and ending with the image inside the vertical side. Motions take values in the full isometry group E(2)E(2)E(2); continuity together with m(0)=idm(0)=\mathrm{id}m(0)=id forces the path to lie in the orientation-preserving component. The sofa constant is the supremum, in the extended nonnegative reals, of the areas volume(s)\mathrm{volume}(s)volume(s) over all moving sofas. The supremum is finite, at least 11/511/511/5, and attained.

Gerver's shape is defined from a rotation path. For constants AAA, BBB, φ\varphiφ, θ\thetaθ, let rrr be the piecewise function with breakpoints φ\varphiφ, θ\thetaθ, π/2−θ\pi/2-\thetaπ/2−θ, π/2−φ\pi/2-\varphiπ/2−φ from Romik's Theorem 2, let xxx and yyy be its cosine and sine integrals, and let ppp be the associated translation path. The sofa for those constants is the intersection over angles in [0,π/2][0,\pi/2][0,π/2] of the correspondingly rotated and translated hallways, with the endpoints using the horizontal and vertical sides. The four equations ABphiThetaSpec cut out the constants. They have exactly one solution with 0≤φ≤θ≤π/40\le\varphi\le\theta\le\pi/40≤φ≤θ≤π/4 and 0≤A0\le A0≤A, 0≤B0\le B0≤B. The same Lean development uses the identical notation as the formal statements, so prose and code read as one document.

Formalization targets

Goal: optimality of Gerver's sofa

For every AAA, BBB, φ\varphiφ, θ\thetaθ satisfying ABphiThetaSpec,

sofaConstant=volume(gerversSofaWith(A,B,φ,θ)).\mathrm{sofaConstant} = \mathrm{volume}(\mathrm{gerversSofaWith}(A,B,\varphi,\theta)).sofaConstant=volume(gerversSofaWith(A,B,φ,θ)).

The goal leaves unfixed which solution of the spec is used; by uniqueness all choices give the same shape up to the proved identification, so this is the stable form of Baek's Theorem 1.1. It asserts that the supremum equals the area of Gerver's shape, hence that no moving sofa has larger area and that the supremum is attained.

Supporting targets

∃! (A,B,φ,θ), ABphiThetaSpec(A,B,φ,θ).\exists!\,(A,B,\varphi,\theta),\ \mathrm{ABphiThetaSpec}(A,B,\varphi,\theta).∃!(A,B,φ,θ), ABphiThetaSpec(A,B,φ,θ). ∀ A,B,φ,θ, ABphiThetaSpec(A,B,φ,θ)  ⟹  ∃ m, IsMovingSofa(gerversSofaWith(A,B,φ,θ),m).\forall\,A,B,\varphi,\theta,\ \mathrm{ABphiThetaSpec}(A,B,\varphi,\theta)\implies \exists\,m,\ \mathrm{IsMovingSofa}(\mathrm{gerversSofaWith}(A,B,\varphi,\theta),m).∀A,B,φ,θ, ABphiThetaSpec(A,B,φ,θ)⟹∃m, IsMovingSofa(gerversSofaWith(A,B,φ,θ),m).

The first is Gerver's Theorem 2 in Romik's equation form on the closed domain. The second says every such shape admits a hallway motion. Together they supply the constants and the witness that the supremum is attained. The live mission records a root sketch composing the upper-bound half (every moving sofa is bounded by Gerver's area) with the movability witness into the supremum equality.

Significance

The result itself closes a problem open since 1966. It identifies the maximum area, shows the maximum is attained by an explicit shape, and determines that shape from four equations whose solution is unique. Consequences include the numerical enclosure 11/5≤volume≤∞11/5\le\mathrm{volume}\le\infty11/5≤volume≤∞ proved by interval arithmetic, the finiteness of the supremum, and the reduction of future improvements to the analysis of the functional QQQ on caps. Without it the exact maximum remains unknown.

Formalizing it adds a machine-checked proof that makes no classical area assumption: the Green-type curve-area identity and the Minkowski-type mixed-area facts quoted by the paper are proved, the paper's 11 proof gaps and 33 misprints are repaired, and the numerical certificate is kernel-checked. The hallway, motion, cap, convex-body, and surface-measure infrastructure is reusable for related isoperimetric and kinematic formalizations. Status honesty: the underlying paper proof is complete and has been formalized in the source repository; on this platform the three statements above are open targets awaiting proofs, and the uniqueness of the maximizer up to rigid motion remains open and is not part of this mission.

Difficulty

The obvious argument bounds the area of an arbitrary sofa by the area of a circumscribed cap, but caps need not satisfy the injectivity condition that makes the functional QQQ an upper bound, and QQQ need not be concave on the full space of caps. Maximizing sequences of polygons need not converge to a sofa, and limits need not be connected or attain the supremum. The naive idea of taking a supremum over all connected closed sets and extracting a convergent subsequence fails until compactness of motions, closedness of the moving-sofa predicate, and a balanced maximum with rotation angle π/2\pi/2π/2 are established. Each step fails for general sets and only holds after the polygon approximation and monotonization constructions.

Formalization scope

Lean represents the plane as EuclideanSpace ℝ (Fin 2) with its standard orientation, hallway sides as explicit sets, motions as I → E(2) where E(2) is ℝ² ≃ᵃⁱ[ℝ] ℝ² with the topology induced from continuous maps, and area as MeasureSpace.volume. The supremum is in ℝ≥0∞. Statements target the c5ea003 (Lean v4.30.0) environment, an older supported revision against which the development was verified locally. The spec uses non-strict inequalities, which makes uniqueness stronger than the strict-inequality literature form. The functions rrr, xxx, yyy, ppp take the constants as explicit arguments rather than reading global chosen constants, so the definition bundle stays independent of the existence proof; given uniqueness this implies the source statements. Boundedness and measurability are not assumed; every moving sofa is proved compact in the source development. A submission that drops closedness or connectedness, that allows a discontinuous motion, or that hard-codes the numerical value 2.21952.21952.2195 instead of proving equality with the volume of the defined shape, does not satisfy the statements. Contributions welcome: direct proofs of the three targets, sharper enclosures of the volume, and reusable hallway and motion lemmas. Out of scope: uniqueness up to congruence, the 11/511/511/5 certificate details beyond the stated lower bound, and the 20 unformalized numbered environments listed in the source NOTES.md that none of the three targets depends on.

Selected references

  • Jineon Baek, Optimality of Gerver's Sofa, arXiv:2411.19826, 2024. https://arxiv.org/abs/2411.19826
  • Joseph L. Gerver, On moving a sofa around a corner, Geometriae Dedicata 42 (1992), 267-283.
  • Dan Romik, Differential equations and exact solutions in the moving sofa problem, Experimental Mathematics 27 (2018), 316-330. https://arxiv.org/abs/1606.08111
  • Dean Cureton et al., MovingSofa: Autoformalization of Baek's solution, 2026. https://github.com/deancureton/MovingSofa
  • Google DeepMind, formal-conjectures, FormalConjectures/Wikipedia/MovingSofa.lean at ddfbaf90. https://github.com/google-deepmind/formal-conjectures
  • Dawid Trela, GerverSofaLean v1.1.0. https://github.com/dawidmtrela-dotcom/GerverSofaLean
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