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Differential Geometry·Captain: mikedeng1

A Generalisation of Steenrod's Approximation Theorem: Smoothing a Continuous Section of a Smooth Bundle with Normed-Modelled Fibre near L, Fixed off U, by a Vertical Homotopy Within Any NeighbourhoodResearch Paper

Motivation

Many constructions in differential topology and infinite-dimensional Lie theory start from a continuous object and need a smooth one: a continuous section of a smooth bundle, a continuous map into a manifold, a continuous homotopy between smooth maps. Steenrod's approximation theorem (Steenrod 1951, §6.7) says that, for finite-dimensional bundles, a continuous section can be smoothed by a small homotopy through sections, without changing it where it is already smooth. Hirsch's textbook (Hirsch 1976, Ch. 2) gives the relative version for maps between finite-dimensional manifolds.

Gauge theory and the study of principal bundles whose structure group is an infinite-dimensional Lie group (current groups, diffeomorphism groups, gauge groups) need the same statement when the typical fibre is infinite-dimensional. C. Wockel (arXiv:math/0610252, 2006) proves it for a finite-dimensional base with corners and a fibre that is a manifold modelled on a locally convex space, combining Steenrod's argument with Neeb's approximation results for maps into locally convex spaces (Neeb 2002, App. A.3). The consequences in the paper are that smooth and continuous homotopy classes of sections, and of maps from a finite-dimensional manifold into a locally convex manifold, coincide; this is used in bundle theory for infinite-dimensional structure groups (Müller–Wockel 2006, cited as [MW06] in the paper).

Setting

A manifold with corners MMM is a Hausdorff paracompact space with charts onto open subsets of the quadrant R+d={x∈Rd:xi≥0}\mathbb R^d_+ = \{x \in \mathbb R^d : x_i \ge 0\}R+d​={x∈Rd:xi​≥0} and smooth coordinate changes. A locally convex manifold NNN is a Hausdorff space with charts onto open subsets of a locally convex space and smooth coordinate changes, where smoothness of f:U→Yf : U \to Yf:U→Y means that all iterated directional derivatives exist and are continuous (Definition 0.1 of the paper).

A map π:E→M\pi : E \to Mπ:E→M is a locally trivial smooth bundle with typical fibre NNN if every point of MMM has an open neighbourhood SSS and a diffeomorphism φ:π−1(S)→S×N\varphi : \pi^{-1}(S) \to S \times Nφ:π−1(S)→S×N with pr1∘φ=π\mathrm{pr}_1 \circ \varphi = \pipr1​∘φ=π. A section is a continuous map σ:M→E\sigma : M \to Eσ:M→E with π∘σ=idM\pi \circ \sigma = \mathrm{id}_Mπ∘σ=idM​. A map is smooth on a neighbourhood of a set sss if it is smooth on some open set containing sss.

For spaces X,YX, YX,Y, C(X,Y)c.o.C(X, Y)_{c.o.}C(X,Y)c.o.​ is the space of continuous maps with the compact-open topology, generated by the sets ⌊C,W⌋={f:f(C)⊆W}\lfloor C, W\rfloor = \{f : f(C) \subseteq W\}⌊C,W⌋={f:f(C)⊆W} with CCC compact and WWW open.

Formalization targets

Goal: Theorem 0.11 (Generalised Steenrod Approximation Theorem)

Let MMM be finite-dimensional and connected, π:E→M\pi : E \to Mπ:E→M a locally trivial smooth bundle with typical fibre NNN, σ\sigmaσ a continuous section, L⊆ML \subseteq ML⊆M closed, U⊆MU \subseteq MU⊆M open, and σ\sigmaσ smooth on a neighbourhood of L∖UL \setminus UL∖U. Then for every open O⊇σ(M)O \supseteq \sigma(M)O⊇σ(M) there are a section τ\tauτ and a homotopy HHH with

τ(M)⊆O,τ smooth on a neighbourhood of L,τ∣M∖U=σ∣M∖U,\tau(M) \subseteq O,\quad \tau \text{ smooth on a neighbourhood of } L,\quad \tau|_{M \setminus U} = \sigma|_{M \setminus U},τ(M)⊆O,τ smooth on a neighbourhood of L,τ∣M∖U​=σ∣M∖U​, H:[0,1]×M→O,H(0,⋅)=σ, H(1,⋅)=τ,π∘H(t,⋅)=idM,H(t,x)=σ(x) for x∉U.H : [0,1] \times M \to O,\quad H(0,\cdot) = \sigma,\ H(1, \cdot) = \tau,\quad \pi \circ H(t, \cdot) = \mathrm{id}_M,\quad H(t,x) = \sigma(x) \text{ for } x \notin U.H:[0,1]×M→O,H(0,⋅)=σ, H(1,⋅)=τ,π∘H(t,⋅)=idM​,H(t,x)=σ(x) for x∈/U.

Milestones

  1. Remark 0.4: a connected paracompact finite-dimensional manifold with corners is σ-compact.
  2. Proposition 0.7: C∞(M,Y)C^\infty(M, Y)C∞(M,Y) is dense in C(M,Y)c.o.C(M, Y)_{c.o.}C(M,Y)c.o.​, with support control for compactly supported maps.
  3. Corollary 0.8: C∞(M,V)C^\infty(M, V)C∞(M,V) is dense in C(M,V)c.o.C(M, V)_{c.o.}C(M,V)c.o.​ for V⊆YV \subseteq YV⊆Y open.
  4. Lemma 0.9: relative smoothing of f:M→Wf : M \to Wf:M→W, W⊆YW \subseteq YW⊆Y open convex, within any compact-open neighbourhood, keeping fff off UUU.
  5. Lemma 0.10: the same for maps into a subset W⊆NW \subseteq NW⊆N diffeomorphic to an open convex subset of the model space.
  6. Sections versus fibre maps (proof of Theorem 0.11, p. 5): over a smooth trivialisation φ\varphiφ, a section σ′\sigma'σ′ is smooth near xxx if and only if pr2∘φ∘σ′\mathrm{pr}_2 \circ \varphi \circ \sigma'pr2​∘φ∘σ′ is.

Significance

The result. The theorem turns continuous sections into smooth ones by homotopies that are small (they stay in any prescribed open set OOO around the section) and relative (fixed where nothing needs changing). It yields that C∞(M,N)C^\infty(M, N)C∞(M,N) is dense in C(M,N)C(M, N)C(M,N) for the graph and compact-open topologies (Corollary 0.12), that every continuous section is homotopic to a smooth one and continuously homotopic smooth sections are smoothly homotopic (Proposition 0.13), and that smooth and continuous homotopy classes [M,N][M, N][M,N] agree (Corollary 0.14). These are the statements needed to compare smooth and topological classification of bundles with infinite-dimensional structure groups.

Formalizing it. The theorem is proved in the paper; no machine-checked version exists. Mathlib has smooth partitions of unity on finite-dimensional manifolds with corners and local-to-global smoothing for maps into convex sets, but no density of C∞(M,Y)C^\infty(M, Y)C∞(M,Y) in C(M,Y)C(M, Y)C(M,Y) for the compact-open topology, no relative smoothing lemma, and no smoothing of sections of non-vector bundles. A formalization would supply these as reusable statements about Mathlib's ContMDiff, Bundle.Trivialization and C(M, Y).

Difficulty

The obvious argument glues local smoothings with a partition of unity, as for real-valued functions. This fails for sections of a non-linear bundle: convex combinations of points of EEE, or of NNN, are meaningless, so a partition-of-unity average of local smoothings is not a section, and the smoothing cannot be done in one global step. Any stepwise replacement must keep the section inside the prescribed open set OOO, must not destroy smoothness already achieved near earlier parts of LLL, and must avoid convergence arguments, since infinitely many steps are needed on a non-compact MMM. The homotopy has to be continuous at the end where infinitely many steps accumulate. Finally, an infinite-dimensional NNN is not locally compact, so all compactness must come from MMM; this is why the base is finite-dimensional while the fibre is not.

Formalization scope

  • Normed models. Mathlib's manifolds require a normed model space, so NNN is modelled (without boundary) on a real normed space FFF, not necessarily complete or finite-dimensional, and the total space EEE is a manifold with corners modelled on a real normed space; in Proposition 0.7, Corollary 0.8 and Lemma 0.9 the target YYY is a real normed space. On normed spaces the paper's smoothness coincides with Fréchet C∞C^\inftyC∞, Mathlib's ContMDiff … ∞ (not the analytic ω). This is the one specialisation of the paper; non-normable locally convex fibres are out of scope.
  • The base. MMM carries any finite-dimensional Mathlib model with corners III (which contains the quadrant R+d\mathbb R^d_+R+d​), with [T2Space M], and [ParacompactSpace M] (Theorem 0.11, Remark 0.4, milestone 6) or [SigmaCompactSpace M] (Proposition 0.7, Corollary 0.8, Lemmas 0.9, 0.10), as Definition 0.3 and the statements require; Theorem 0.11 adds [ConnectedSpace M]. NNN is [T2Space N].
  • Conventions. "Smooth on a neighbourhood of sss" is C∞C^\inftyC∞ on an open set containing sss (SmoothNear), not smoothness on sss itself. Spaces C(M,W)C(M, W)C(M,W) for W⊆YW \subseteq YW⊆Y or W⊆NW \subseteq NW⊆N are maps into the subtype with the compact-open topology, so neighbourhoods are taken in C(M,W)C(M, W)C(M,W). A bundle is given by smooth Bundle.Trivializations covering MMM; "WWW diffeomorphic to an open convex subset of FFF" is a partial diffeomorphism N→FN \to FN→F with source WWW and convex target. The homotopy is indexed by unitInterval and runs from σ\sigmaσ at 000 to τ\tauτ at 111. "Support" is the closed support tsupport.
  • No trivial reading. The goal must not be read with smoothness on LLL only (which is weaker for closed LLL), with OOO replaced by all of EEE, or with a trivial bundle or finite-dimensional fibre; a sanity file checks that the hypotheses are satisfiable on the product bundle R×R→R\mathbb R \times \mathbb R \to \mathbb RR×R→R.
  • What a development needs. Smooth partitions of unity on MMM (in Mathlib), local compactness and σ-compactness of MMM, the compact-open topology on C(M,W)C(M, W)C(M,W) and continuity of the operations γ↦λγ+(1−λ)f\gamma \mapsto \lambda\gamma + (1-\lambda)fγ↦λγ+(1−λ)f on it, and the gluing of sections along locally finite covers. Proofs of Proposition 0.7 and Lemma 0.9 are reusable beyond this mission; contributions proving any milestone, or the Mathlib-level density results, are welcome.

Selected references

  • C. Wockel, A Generalisation of Steenrod's Approximation Theorem, preprint arXiv:math/0610252v1, 2006. https://arxiv.org/abs/math/0610252
  • N. Steenrod, The Topology of Fibre Bundles, Princeton University Press, 1951, §6.7. https://doi.org/10.1515/9781400883875
  • M. W. Hirsch, Differential Topology, Graduate Texts in Mathematics 33, Springer, 1976, Ch. 2. https://doi.org/10.1007/978-1-4684-9449-5
  • K.-H. Neeb, Central extensions of infinite-dimensional Lie groups, Ann. Inst. Fourier 52 (2002), App. A.3 (cited as [Ne02]).
  • C. Müller, C. Wockel, Equivalences of smooth and continuous principal bundles with infinite-dimensional structure group, preprint, 2006 (cited as [MW06]).
  • J. Dugundji, Topology, Allyn and Bacon, 1966, Theorems XI.7.2–3.
8 thms1 active userReviewed
🏆Completed
Combinatorics·Captain: username

Continuous graph homomorphisms for Zd\mathbb Z^dZd-actions: Theorem 1.4 and Proposition 7.1Research Paper

Continuous colorings of lattice actions

A graph homomorphism sends vertices of one graph to another while preserving adjacency. Requiring this map to be continuous makes graph coloring sensitive to topology: each color must occupy an open and closed region. For integer lattice actions, the resulting questions connect finite graph structure with continuous dynamics. The results considered here give an algebraic sufficient condition on a finite target graph that works in every finite lattice dimension. They are Theorem 1.4 and Proposition 7.1 of Ruijun Wang's Continuous graph homomorphisms of higher dimensional abelian group actions, a 2026 research preprint.

Actions, graphs, and reduced walks

Fix an integer d≥1d\ge1d≥1. The integer lattice is G=ZdG=\mathbb Z^dG=Zd, with standard generators eie_iei​. Each generator has one coordinate equal to one and all other coordinates zero. An action of GGG on a space XXX assigns maps x↦g⋅xx\mapsto g\cdot xx↦g⋅x satisfying 0⋅x=x0\cdot x=x0⋅x=x and (g+h)⋅x=g⋅(h⋅x)(g+h)\cdot x=g\cdot(h\cdot x)(g+h)⋅x=g⋅(h⋅x). A continuous action uses the discrete topology on GGG. It is free when g⋅x=xg\cdot x=xg⋅x=x implies g=0g=0g=0.

A Polish space has a topology induced by a complete separable metric. It is zero-dimensional when its topology has a basis of clopen sets, meaning sets that are both open and closed. The standard Schreier graph on XXX joins xxx to ei⋅xe_i\cdot xei​⋅x for each generator, with adjacency understood symmetrically.

Let HHH be a finite simple graph on a vertex set VVV, equipped with the discrete topology. A continuous homomorphism is a continuous function c:X→Vc:X\to Vc:X→V such that

H.Adj⁡(c(x),c(ei⋅x))for every x∈X and i.H.\operatorname{Adj}(c(x),c(e_i\cdot x)) \quad\text{for every }x\in X\text{ and }i.H.Adj(c(x),c(ei​⋅x))for every x∈X and i.

Write UniversalTarget⁡(d,H)\operatorname{UniversalTarget}(d,H)UniversalTarget(d,H) when such a map exists for every free continuous lattice action on every zero-dimensional Polish space.

A closed walk starts and ends at the same vertex, and its length counts edges. Repetitions are allowed. The reduced homotopy group Π1∗(H,b)\Pi_1^*(H,b)Π1∗​(H,b) identifies based closed walks under cancellation of a spur and cancellation of a closed four-walk, with these relations compatible with concatenation. Its identity is the constant walk. These conventions agree with Section 2.

Formalization targets

Theorem 1.4 assumes an odd closed walk whose reduced class has trivial square:

(∃b∈V, ∃γ:b⇝b,∣γ∣ odd,[γ]2=1)⟹∀d≥1, UniversalTarget⁡(d,H).\bigl(\exists b\in V,\ \exists\gamma:b\leadsto b,\quad |\gamma|\text{ odd},\quad[\gamma]^2=1\bigr) \Longrightarrow \forall d\ge1,\ \operatorname{UniversalTarget}(d,H).(∃b∈V, ∃γ:b⇝b,∣γ∣ odd,[γ]2=1)⟹∀d≥1, UniversalTarget(d,H).

The source statement appears in Section 1.

The main target, Proposition 7.1, permits any finite order:

(∃b∈V, ∃γ:b⇝b,∣γ∣ odd,∃N>0, [γ]N=1)⟹∀d≥1, UniversalTarget⁡(d,H).\bigl(\exists b\in V,\ \exists\gamma:b\leadsto b,\quad |\gamma|\text{ odd},\quad\exists N>0,\ [\gamma]^N=1\bigr) \Longrightarrow \forall d\ge1,\ \operatorname{UniversalTarget}(d,H).(∃b∈V, ∃γ:b⇝b,∣γ∣ odd,∃N>0, [γ]N=1)⟹∀d≥1, UniversalTarget(d,H).

Here NNN is a positive integer; it need not be the least exponent. The square-trivial case follows by taking N=2N=2N=2. The stronger statement is given in Section 7.1.

Mathematical significance and completion status

These results turn one finite algebraic witness into a conclusion covering all the spaces, actions, and positive dimensions specified above. Once a graph satisfies the hypothesis, an individual action requires no additional dynamical condition beyond the stated assumptions. The conclusion concerns finite discrete targets and the standard generating set.

Both results are established in the cited paper. Complete local Lean proofs now cover their full universal statements. The local project build and kernel audit have passed, and the final declarations use only Lean's standard logical axioms. Prove2Me has accepted the complete uploaded proof dependency graph. Both original headline theorem identities now have status Proved.

The completed development supplies reusable statements and checked infrastructure for lattice actions, reduced graph walks, finite probability distributions, and continuous graph homomorphisms. These components support inspection and reuse beyond the two headline results.

Why continuity requires attention

Choosing a homomorphism separately on each orbit does not ensure continuity across nearby points of the space. Freeness identifies each orbit with a lattice once an origin has been chosen, but does not supply continuously chosen origins across all orbits. A proof must therefore establish continuity of the resulting vertex map itself. Restricting attention to one action, one dimension, or an orbitwise map would leave the stated universal conclusion unresolved.

Formalization scope

The lattice is represented by Fin d→Z\mathrm{Fin}\ d\to\mathbb ZFin d→Z, actions use additive notation, and standard adjacency includes both orientations of each generator edge. Reduced homotopy is an inductively generated relation on genuine Mathlib graph walks; powers are repeated concatenations. The target vertex type is arbitrary and finite, with its discrete topology.

Source spaces and target vertex types have independent universe parameters. Empty source spaces are allowed. No connectivity assumption is imposed on the target, and no separate nonemptiness hypothesis is added. The odd-walk witness already forces target nonemptiness. Neither a carrier-construction assumption nor an approximation condition appears in either final theorem.

Finite order refers to the class of the walk, rather than its length. An odd walk can revisit vertices and traverse edges repeatedly, so the hypothesis does not require an embedded cycle. All four-walk relations are included, including those with repeated vertices. The conclusion asserts existence of a continuous adjacency-preserving function; it asserts neither uniqueness nor injectivity. These distinctions matter when comparing a formal declaration with the source: replacing arbitrary closed walks by simple cycles or adding connectedness would change the objects quantified over. The recorded statements retain the wider walk convention used in the paper.

Further contributions can reuse the infrastructure or establish related variants while preserving these conventions. Any changed statement should distinguish its additional hypotheses and its altered conclusion from the two results recorded here.

Selected references

Ruijun Wang, Continuous graph homomorphisms of higher dimensional abelian group actions, arXiv preprint arXiv:2609.39824v1, 2026. Version and source; Theorem 1.4; definitions; Proposition 7.1.

17 thms1 active userReviewed
Geometry & 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.
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Geometry & 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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Geometry & 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.
9 thms1 active userReviewed
Geometry & 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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🏆Completed
Dynamical SystemsMathematical Physics·Captain: lisamegawatts

Winding Dynamics I: Homotopy Conservation and Reset BalanceTextbook

Motivation

Phase winding is an integer attached to a circle-valued field on a closed spatial cycle. It distinguishes configurations that cannot be continuously deformed into one another while remaining circle-valued and spatially continuous. In oscillator and spin models this integer is often described informally as conserved by smooth evolution, while changes of winding are attributed to phase slips, vortices, singularities, or branch-cut crossings. The purpose of this mission is to turn that informal division into an exact Lean interface.

The continuum and finite-lattice settings must be separated. A jointly continuous field on a spatial circle really does provide a homotopy of circle maps, so its degree is invariant. A finite list of continuously moving vertex phases does not by itself determine a continuous field on the geometric realization of the lattice. Principal shortest-arc interpolation becomes ambiguous at antipodal bonds, and the corresponding discrete winding can jump even though every vertex phase remains continuous. The mission therefore treats winding as a first integral only on the regular sector and records every failure of regularity through an integer reset ledger.

This distinction is relevant to circle-valued reductions of the Kuramoto model, the finite XY model, and Lohe-type dynamics. Kuramoto's original synchronization model concerns coupled phase oscillators, while Lohe's non-Abelian extension replaces phases by group-valued variables. A model-specific conservation theorem is justified only after the dynamics has been connected to an actual circle-valued spatial loop or to the registered finite principal-branch interface.

Setting

A circle loop is a continuous map from a closed parameter interval to S1S^1S1 whose two endpoints agree. Its winding number is the integer obtained from the endpoint of a lift to the universal cover R→S1\mathbb R\to S^1R→S1. When the loop's basepoint moves during a deformation, the loop is normalized by the inverse of its value at the chosen spatial basepoint; this produces a based loop without changing its winding.

A continuous Circle-field segment is a jointly continuous map

U:[t0,t1]×S1⟶S1.U:[t_0,t_1]\times S^1\longrightarrow S^1.U:[t0​,t1​]×S1⟶S1.

Each time slice UtU_tUt​ is a spatial loop. Such a segment has no branch-cut convention: it is intrinsic topological data.

For a finite directed edge system (including a finite periodic lattice), a state assigns a real lift to every vertex. Each oriented edge receives an integer principal turn. A state is branch regular when no stored edge is antipodal. A coherent finite reset ledger stores successive principal-turn cochains TiT_iTi​ and defines the reset ki=Ti+1−Tik_i=T_{i+1}-T_iki​=Ti+1​−Ti​. For a certified closed integer cycle CCC, the pairing ⟨ki,C⟩\langle k_i,C\rangle⟨ki​,C⟩ is its registered winding jump.

A Kuramoto, XY, or Lohe consumer must supply the missing model-specific data. For a continuum consumer this is a jointly continuous circle-valued field. For a finite consumer it is a continuous vertex trajectory together with branch regularity away from registered events. A Lohe consumer additionally needs a continuous Circle readout or invariant Circle carrier; preservation of a rotor constraint alone does not provide that reduction.

Formalization targets

Continuous-field conservation

For every jointly continuous Circle-field segment, the two endpoint loops have equal winding:

wind⁡(Ut1)=wind⁡(Ut0).\operatorname{wind}(U_{t_1})=\operatorname{wind}(U_{t_0}).wind(Ut1​​)=wind(Ut0​​).

The statement must cover moving loop basepoints through explicit normalization. Winding is defined directly from Mathlib's exponential covering map as the floor of the zero-based lift endpoint divided by 2π2\pi2π.

Branch-regular finite conservation

For every finite directed principal-phase trajectory on a preconnected time domain that remains branch regular, every registered integer-chain winding is constant:

WC(t1)=WC(t0).W_C(t_1)=W_C(t_0).WC​(t1​)=WC​(t0​).

Continuity of the vertex phases alone is not a sufficient hypothesis and must not appear as a replacement for branch regularity or spatial interpolation.

Exact reset balance

For a finite coherent ledger with steps i=0,…,N−1i=0,\ldots,N-1i=0,…,N−1, endpoint winding change equals the sum of the reset periods:

WC(TN)−WC(T0)=∑i=0N−1⟨ki,C⟩.W_C(T_N)-W_C(T_0) =\sum_{i=0}^{N-1}\langle k_i,C\rangle.WC​(TN​)−WC​(T0​)=i=0∑N−1​⟨ki​,C⟩.

The conservation theorem is the empty-ledger or zero-period special case. The statement is an exact integer identity and does not assert an energy lower bound, vortex separation, or a thermodynamic-limit result.

Dynamics adapters

The generic dynamics adapter requires a jointly continuous ambient-state segment, a registered carrier containing it, closed spatial profiles, and a continuous readout from that carrier to the Circle. Kuramoto/XY or Lohe consumers must separately prove those hypotheses for their model. A second fence states that a global continuous readout from a simply connected carrier maps every loop to a nullhomotopic Circle loop; nonzero Lohe winding therefore requires a separately registered non-simply-connected carrier, such as a preserved U(1)U(1)U(1) orbit, or a different explicit interface.

Significance

The resulting theorem family makes precise the statement that winding obstructs unwinding. In the intrinsic continuum setting, winding cannot change while the field remains a continuous S1S^1S1-valued map. In the finite principal-branch setting, winding is piecewise constant and every change has an exact integer certificate. This separates a topological conservation law from the physical or analytic question of how much energy is needed to realize a certificate.

For formalization, the mission supplies a reusable boundary between topology and dynamics. A dynamics development can establish continuity and carrier preservation without reimplementing covering-space winding. A lattice development can consume the same integer through reset cochains without claiming that a vertex-only path is a homotopy of spatial loops. Later energy-barrier, vortex, and transport results can depend on the reset balance rather than on an informal conservation principle.

Difficulty

The principal difficulty is that several superficially similar notions of continuity have different consequences. Continuity in time of finitely many vertex phases is continuity into the configuration torus (S1)V(S^1)^V(S1)V, which is connected and does not preserve a principal-edge winding sector. Continuity of a map on time times the geometric spatial cycle is stronger. A formal statement that confuses them would make the desired theorem false.

There are two additional interface risks. First, the canonical Circle lift is based, whereas a physical phase field normally has a moving value at the chosen spatial origin. Second, the current Lohe development establishes algebraic identities and infinitesimal rotor preservation, not a global continuous flow in a selected Circle subgroup. These distinctions remain visible in the theorem hypotheses.

Formalization scope

The mission targets Lean 4.30 with Mathlib revision c5ea00351c28e24afc9f0f84379aa41082b1188f, matching the cited LeanProofs development. It reuses Mathlib's unit interval, continuous maps, path homotopies, Circle covering map, local constancy, and finite sums. The continuum statement concerns spatial S1S^1S1 only. The finite theorem is graph-generic: it uses finite oriented edges, integer edge cochains, certified closed integer cycles, coherent successive reset states, and branch regularity on a preconnected time domain.

The scope excludes ODE or PDE existence and uniqueness, preservation of a Circle carrier by a particular Lohe vector field, extraction of a coherent reset ledger from a physical event trajectory, arbitrary graph interpolation, accumulating reset times, thermodynamic limits, and energetic barriers. Those may be attached later through explicit interfaces. No theorem claims global winding conservation for an unrestricted finite vertex trajectory, and no theorem identifies group-valued Lohe motion with Circle motion without a declared continuous readout.

Selected references

  • Monumental Systems, CircleFundamentalGroupWindingV1, LeanProofs commit b656238b73d5f0f74515f6574a1dcb4e0216129f, 2026. https://github.com/MonumentalSystems/LeanProofs/blob/b656238b73d5f0f74515f6574a1dcb4e0216129f/LeanProofs/Rosetta/CircleFundamentalGroupWindingV1.lean#L81
  • Monumental Systems, FiniteTorusPrincipalResetEventV1, LeanProofs commit b656238b73d5f0f74515f6574a1dcb4e0216129f, 2026. https://github.com/MonumentalSystems/LeanProofs/blob/b656238b73d5f0f74515f6574a1dcb4e0216129f/LeanProofs/StatMech/FiniteTorusPrincipalResetEventV1.lean#L152-L167
  • Monumental Systems, CircleWindingTranslationHolonomyV1, LeanProofs commit b656238b73d5f0f74515f6574a1dcb4e0216129f, 2026. https://github.com/MonumentalSystems/LeanProofs/blob/b656238b73d5f0f74515f6574a1dcb4e0216129f/LeanProofs/Rosetta/CircleWindingTranslationHolonomyV1.lean#L107
  • Y. Kuramoto, “Self-entrainment of a population of coupled non-linear oscillators,” in International Symposium on Mathematical Problems in Theoretical Physics, Lecture Notes in Physics 39, 1975, pp. 420–422. https://doi.org/10.1007/BFb0013365
  • M. A. Lohe, “Non-Abelian Kuramoto models and synchronization,” Journal of Physics A: Mathematical and Theoretical 42 (2009), 395101. https://doi.org/10.1088/1751-8113/42/39/395101
  • A. Hatcher, Algebraic Topology, Chapter 1, Cambridge University Press, 2002. https://pi.math.cornell.edu/~hatcher/AT/ATch1.pdf
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Dynamical SystemsMathematical Physics·Captain: lisamegawatts

Winding Proto-Time I: Neutral Clock CoreTextbook

Motivation

A real lift of a circle-valued phase records both a principal representative and an integer sheet. This packet isolates the neutral arithmetic of that lifted reading before any physical interpretation as time, dynamics, causality, or a preferred vacuum.

Setting

A clock candidate is a function from an arbitrary event type to the real universal cover of the circle. Principalization separates each real value into a representative modulo 2π2\pi2π and an integer sheet. Real origin shifts, integral deck shifts, and orientation reversal are treated as distinct transformations.

Formalization targets

The intended packet covers principal-ledger reconstruction, the conditional strict order induced by an injective or monotone lift, affine-origin and deck freedom, orientation reversal, an adapter from separately established circle winding to an integer clock turn, and a scalar power-law integrability boundary.

The exact target statements remain subject to reconciliation with the immutable LeanProofs source before this private draft is submitted. In particular, no arithmetic quotient identity may be presented as the full Circle winding adapter, and no scalar integrability theorem may be interpreted as a PDE blow-up result.

Significance

This separates universal-cover bookkeeping from later consumers. A subsequent packet may connect the ledger to reset cochains, null-pair torsors, or dynamics only through explicit adapters.

Difficulty

The main risks are sign conventions at the principal cut, degeneracy on empty event types, confusion between the continuous real origin action and the integral deck action, and circular definitions that manufacture winding from the desired clock integer.

Formalization scope

The development targets Lean 4.30 and Mathlib revision c5ea00351c28e24afc9f0f84379aa41082b1188f. It makes no claim of monotone physical time, dynamical selection, causal order, global foliation, PDE existence, singularity formation, or a canonical origin or orientation.

Selected references

  • Monumental Systems, WindingProtoTimeV1Targets, LeanProofs commit b656238b73d5f0f74515f6574a1dcb4e0216129f, 2026. https://github.com/MonumentalSystems/LeanProofs/blob/b656238b73d5f0f74515f6574a1dcb4e0216129f/LeanProofs/Rosetta/WindingProtoTimeV1Targets.lean
  • Monumental Systems, CircleFundamentalGroupWindingV1, LeanProofs commit b656238b73d5f0f74515f6574a1dcb4e0216129f, 2026. https://github.com/MonumentalSystems/LeanProofs/blob/b656238b73d5f0f74515f6574a1dcb4e0216129f/LeanProofs/Rosetta/CircleFundamentalGroupWindingV1.lean
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