Open problems from the 1970s

Results on questions first raised the 1970s, going by the earliest step each entry records.

63 AI-made results on questions first raised the 1970s, from 132 papers in the OpenAI math collection, each explained in plain English. 39 have a formal Lean proof listed; 24 are claimed in a paper and not yet machine-checked. They span 17 fields, led by algebraic and complex geometry (7), combinatorics (6) and theoretical computer science (6). The oldest question here dates back to 1970: Deterministic polynomial factorization over prime fields. Results rated Landmark include Kakeya in three and four dimensions and Fourier restriction for positively curved surfaces.

Number theory5

Algebraic and complex geometry7

  • 033Sep 10, 2026 Explained

    Iitaka subadditivity, variation, and logarithmic additivity

    Proves Campana's orbifold Iitaka subadditivity conjecture for smooth Fujiki-class-C\mathcal C manifolds with rational simple-normal-crossing boundaries. For projective fibrations f:U→Vf:U\to V of smooth complex quasi-projective varieties with connected fibers, general fiber F, and κˉ(V)≥0\bar\kappa(V)\ge0, proves Popa's inequality κˉ(U)≥κ(F)+max⁡{κˉ(V),Var(f)}\bar\kappa(U)\ge\kappa(F)+\max\{\bar\kappa(V),\mathop{\mathrm{Var}}\nolimits (f)\}, where variation measures the whole geometric generic fiber.

  • 040Sep 24, 2026 Explained

    Bloch’s conjecture for complex surfaces

    Proves Bloch's conjecture: for every smooth connected projective complex surface S with pg(S)=0p_g(S)=0, the Albanese map CH0(S)0→Alb(S)(C)\mathrm{CH}_0(S)^0\to\mathrm{Alb}(S)(\mathbb C) on integral degree-zero zero-cycles is an isomorphism. This combines the new pg=q=0p_g=q=0 theorem with the classical theorem of Bloch, Kas, and Lieberman.

    Claimed, not checked
  • 046Sep 23, 2026 Explained

    Shafarevich counterexamples in dimension two and with large fundamental group

    Constructs a smooth projective complex fourfold with large fundamental group whose universal cover contains no positive-dimensional compact analytic subvariety but is neither Stein nor holomorphically convex. A separate smooth projective complex surface already disproves unrestricted Shafarevich holomorphic convexity in dimension two.

    Claimed, not checked
  • 047Sep 23, 2026 Explained

    Zariski cancellation and affine fibrations over the complex numbers

    Constructs an integral complex affine fourfold X≇A4X\not\cong\mathbb A^4 with X×A1≅A5X\times\mathbb A^1\cong\mathbb A^5, disproving affine-space cancellation over ℂ in dimension four. It also disproves the Dolgachev–Weisfeiler affine-fibration conjecture: smooth surjections X→A1X\to\mathbb A^1 and A5→A2\mathbb A^5\to\mathbb A^2 have every residue-field fiber isomorphic to affine three-space but are not Zariski-locally trivial.

  • 059Sep 24, 2026 Explained

    Counterexamples to Zariski’s multiplicity conjecture

    Disproves Zariski's multiplicity conjecture by constructing reduced holomorphic hypersurface germs that are ambiently homeomorphic but have different multiplicities. The examples include hypersurfaces in ℂ4 with isolated critical points and multiplicities four and five.

    Claimed, not checked
  • 060Sep 24, 2026 Explained

    The Global Spherical Shell conjecture

    Every connected minimal compact complex surface of class VII with b2>0b_2\gt 0 contains a global spherical shell, proving the positive-b2 Global Spherical Shell conjecture. Such a shell is a holomorphically embedded neighborhood of the standard three-sphere in C2∖{0}\mathbb C^2\setminus\{0\} whose complement is connected.

    Claimed, not checked
  • 064Sep 24, 2026 Explained

    Topological triviality of μ-constant surface singularities

    Proves topological right-triviality for every holomorphic one-parameter family of isolated hypersurface singularities in ℂ3 with constant Milnor number, resolving the surface case of the μ-constant problem. After shrinking the parameter disk and representatives, ambient homeomorphisms vary jointly continuously, fix the origin section and preserve the defining functions.

    Claimed, not checked

Real and complex analysis4

  • 072Sep 24, 2026 Explained

    Brennan's conjecture and the integral-means spectrum

    Proves Brennan's conjecture: for every conformal bijection ϕ from a simply connected plane domain onto the disk, ∣ϕ′∣s|\phi'|^s is area-integrable for 4/3<s<44/3\lt s\lt 4. The sharp universal integral-means identity is BS(t)=∣t∣−1B_{\mathcal S}(t)=|t|-1 for t ≤ −2. A strict bound Bb(−1)<1/4B_b(-1)\lt 1/4 for bounded univalent functions disproves Kraetzer's prediction at that parameter.

  • 074Sep 23, 2026 Explained

    Kakeya in three and four dimensions

    Resolves the Kakeya maximal conjecture in three dimensions and the Hausdorff-dimension conjecture in four. In three dimensions, the radius-δ tube maximal operator maps L3(R3)L^3(\mathbb R^3) to L3(S2)L^3(S^2) with norm Oε(δ−ε)O_\varepsilon(\delta^{-\varepsilon}) for every ε > 0. In four dimensions, every set containing a unit segment in every direction has Hausdorff dimension four.

    Claimed, not checked
  • 077Sep 24, 2026 Explained

    Fourier restriction for positively curved surfaces

    Proves the diagonal Fourier extension conjecture for positively curved surfaces in three dimensions. For every compact smooth positively curved surface Σ⊂R3\Sigma\subset\mathbb R^3, including surfaces with boundary, the extension operator is bounded from Lp(Σ)L^p(\Sigma) to Lp(R3)L^p(\mathbb R^3) for every p > 3.

    Claimed, not checked
  • 084Sep 25, 2026 Explained

    The geometric case of the Erdős similarity conjecture

    For every fixed q∈(0,1)q\in(0,1), constructs compact subsets of [0,1][0,1] with measure arbitrarily close to one containing no translated and nontrivially dilated copy of {qn:n≥1}\{q^n:n\ge1\}, with dilations of either sign. This resolves the geometric-progression case of the Erdős similarity conjecture for every ratio.

Convex and metric geometry1

Theoretical computer science6

  • 103Sep 23, 2026 Explained

    Exact derandomization of logarithmic space: L=RL=BPL\mathsf L=\mathsf{RL}=\mathsf{BPL}

    Proves L=RL=BPL\mathsf L=\mathsf{RL}=\mathsf{BPL}, resolving derandomization for bounded-error logarithmic-space computation. An effective compiler converts each randomized polynomial-time logarithmic-space machine deciding a language with one-sided or two-sided error into a deterministic logarithmic-space decider with explicit polynomial running-time bounds.

  • 121Sep 24, 2026 Explained

    Almost-linear approximation of edit distance

    For every fixed rational ε∈(0,1)\varepsilon\in(0,1), gives a randomized (1+ε)(1+\varepsilon) approximation to unit-cost edit distance in worst-case expected time N1+o(1)N^{1+o(1)}, with success probability at least 2/3. The strings have total length N and polynomially bounded integer symbols. This is an asymptotic guarantee at fixed accuracy.

  • 124Sep 24, 2026 Explained

    Polynomial-time scheduling on three identical machines

    Resolves the three-processor unit-job scheduling problem of Garey and Johnson: a deterministic polynomial-time algorithm minimizes makespan for nonpreemptive unit-length jobs with arbitrary precedence constraints on three identical parallel machines. For an explicitly given precedence graph, it decides deadline feasibility exactly and constructs a feasible schedule.

  • 129Sep 25, 2026 Explained

    Exponential state costs for two-way automata

    Proves exponential lower bounds both for complementing two-way nondeterministic finite automata and for simulating one-way nondeterministic automata by two-way deterministic ones. The latter resolves the Sakoda–Sipser state-succinctness conjecture over growing finite alphabets; both results rule out polynomial state bounds independent of alphabet size.

  • 138Sep 26, 2026 Explained

    Subset Sum in O(20.49n)O(2^{0.49n}) time

    Gives a uniform randomized classical algorithm for worst-case Subset Sum in ordinary O(20.49n)O(2^{0.49n}) word-RAM time on polynomial-bit inputs, where n counts the integers. The time bound holds on every execution and success probability is at least 2/3 on every input. Inputs may repeat positive integers; words have O(n+b)O(n+b) bits for maximum input bit length b.

    Claimed, not checked
  • 142Oct 4, 2026 Explained

    Deterministic polynomial factorization over prime fields

    Gives a uniform deterministic algorithm that completely factors every nonzero dense degree-n polynomial over a prime field 𝔽p, including multiplicities, in bit complexity polynomial in (n+1)log⁡p(n+1)\log p. The prime is supplied in binary. No randomness, integer-factorization or primitive-root oracle, or GRH assumption is required.

    Claimed, not checked

Dynamical systems and ergodic theory2

Combinatorics6

  • 162Sep 23, 2026 Explained

    Counterexamples to Ryser’s covering conjecture

    Disproves Ryser's covering conjecture by constructing intersecting (q+1)(q+1)-partite, (q+1)(q+1)-uniform hypergraphs with covering number q+1q+1, rather than the predicted bound q, for every sufficiently large prime q. A separate construction over extension fields also disproves Gyárfás's monochromatic tree-cover conjecture.

  • 164Sep 23, 2026 Explained

    Hindman’s finite sums and products conjecture

    Proves Hindman's finite sums and products conjecture: every finite coloring of the positive integers contains sets of any prescribed finite size whose nonempty subset sums and nonempty subset products all have one common color.

    Claimed, not checked
  • 171Sep 23, 2026 Explained

    The hypercube Ramsey conjecture

    Resolves the Burr–Erdős hypercube Ramsey conjecture: the two-color Ramsey number of the n-dimensional cube is Θ(2n)\Theta(2^n). Thus every red-blue coloring of a complete graph on a universal constant times the cube's number of vertices contains a monochromatic copy of the cube.

    Claimed, not checked
  • 172Sep 23, 2026 Explained

    Classification of finite Euclidean Ramsey configurations

    Classifies finite point configurations that occur monochromatically, at their original scale, in every finite coloring of sufficiently high-dimensional Euclidean space. The characterization is an algebraic condition over the coordinate field. It also disproves the Leader–Russell–Walters conjecture that every such configuration is a subset of a finite transitive set.

  • 182Sep 24, 2026 Explained

    Power savings for intersective polynomial differences and prime arguments

    For every fixed intersective integer polynomial h of degree k ≥ 2 with positive leading coefficient, proves that a subset of {1,…,N}\{1,\ldots,N\} avoiding nonzero values h(1),h(2),…h(1),h(2),\ldots as differences has size Oh(N1−ck)O_h(N^{1-c_k}), with ck>0c_k\gt 0 depending only on degree. Here intersective means having a root modulo every modulus. For prime arguments, a power saving also holds when h has a unit root modulo every modulus, with exponent allowed to depend on h.

  • 183Sep 25, 2026 Explained

    Power savings for planar halving lines and k-sets

    Improves the planar halving-line bound to O(n4/3−ε)O(n^{4/3-\varepsilon}) for sets with no three collinear and an absolute ε > 0. More generally, an n-point set with no three collinear has O(n(k+1)1/3−ε0)O(n(k+1)^{1/3-\varepsilon_0}) strictly separable k-subsets for 1≤k≤n/21\le k\le n/2, with an absolute ε0>0\varepsilon_0\gt 0. The constants and positive exponents are nonquantitative.

Algebra5

Probability and statistical mechanics5

  • 215Sep 23, 2026 Explained

    Canonical O(3)O(3) continuum limit and exact O(4)O(4) mass asymptotics

    Constructs the canonical continuum limit of the two-dimensional nearest-neighbor O(3)O(3) model: a non-Gaussian local relativistic theory with a unique vacuum and a positive mass gap. For the square-lattice O(4)O(4) model, determines the exact leading asymptotic of the full transfer gap, mlat(β)∼32eπ/4−1/2β e−πβm_{\mathrm{lat}}(\beta)\sim32e^{\pi/4-1/2}\sqrt\beta\,e^{-\pi\beta}. The family also proves exponential spin-correlation decay for two-dimensional nearest-neighbor O(n)O(n) models with n ≥ 3 at every positive temperature.

  • 216Sep 24, 2026 Explained

    Critical and near-critical XY scaling and BKT universality

    For the square-lattice nearest-neighbor cosine XY model, proves critical axis correlations Cβc(r)∼Ar−1/4(log⁡r)1/8C_{\beta_c}(r)\sim Ar^{-1/4}(\log r)^{1/8} and the Berezinskii–Kosterlitz–Thouless essential singularity βc−βlog⁡ξ(β)→B\sqrt{\beta_c-\beta}\log\xi(\beta)\to B, with A,B>0A,B\gt 0 after the free-box thermodynamic limit. For finite square-symmetric interactions containing nearest neighbors, discrete Gaussian heights converge to Gaussian fields throughout the rough phase, including its threshold, along geometric torus sizes. Critical center-magnetization and spin-field conclusions retain their stated height, renormalization, and field-input assumptions.

    Claimed, not checked
  • 227Sep 24, 2026 Explained

    Critical SK autocorrelation processes and dynamics across the temperature transition

    For zero-field Gaussian SK heat-bath dynamics with rate-one updates per spin, proves worst-start cutoff on the log⁡n\log n scale for fixed 0≤β<10\le\beta\lt 1, mixing time n2/3+o(1)n^{2/3+o(1)} at β = 1, and stretched-exponential mixing from a Gibbs-sampled fixed starting configuration for β > 1, in probability over disorder. At criticality, rescaled stationary and quench autocorrelation processes have universal random limits for Gaussian and Rademacher disorder; the quench limit relaxes to the stationary limit.

  • 228Sep 24, 2026 Explained

    Continuum phase transitions for radial pair potentials

    Constructs stable distance-dependent pair interactions for three-dimensional classical particles with a first-order phase transition: the canonical free energy has a derivative jump at one inverse temperature throughout an open density interval. One potential has a divergent repulsive core; another is bounded and continuous with an integrable power-law tail, realizing the type of transition sought in Simon's continuum problem.

  • 234Sep 25, 2026 Explained

    All-temperature pressure of orthogonally invariant Ising spin glasses

    Gives an exact variational formula for the limiting pressure of orthogonally invariant Ising spin glasses at every fixed temperature, both almost surely and in expectation. The coupling matrix is a Haar-random rotation of a deterministic spectrum converging to a compactly supported law, with extreme eigenvalues converging to its support edges. The zero-field ground-state energy follows as temperature tends to zero.

Mathematical logic1

Group theory3

Mathematical physics3

  • 260Sep 27, 2026 Explained

    Spacetime Penrose inequalities: enclosing area, charge, rotation, and anti-de Sitter extensions

    Proves the sharp enclosing-area spacetime Penrose inequality for smooth one-ended asymptotically flat initial data in every spatial dimension n ≥ 3, under dominant energy, weak future trapping, positive enclosing area, and the stated decay assumptions. It bounds invariant ADM mass below using minimum enclosing area, with equality rigidity under additional horizon hypotheses. Charged upper-area bounds treat dyonic three-dimensional data; the higher-dimensional purely electric extension uses the matched neutral theorem.

  • 262Sep 23, 2026 Explained

    Sharp finite-matrix Lieb–Thirring inequalities and all equality cases

    Proves the sharp one-dimensional Lieb–Thirring inequality for 1/2<γ<3/21/2\lt \gamma\lt 3/2 and arbitrary finite-matrix potentials W ≥ 0 with ∫tr(Wγ+1/2)<∞\int\mathop{\mathrm{tr}}\nolimits (W^{\gamma+1/2})\lt \infty: the optimal constant is the scalar one-bound-state value, independent of matrix size. All equality cases are direct sums, in one constant unitary basis, of scalar sech2 solitons with independent scales and centers, and zero channels.

  • 264Sep 23, 2026 Explained

    Strong cosmic censorship near two-ended Kerr data

    Proves local strong cosmic censorship near each fixed rotating subextremal Kerr bridge. A dense Gδ subset of a weighted smooth neighborhood of smooth complete two-ended asymptotically flat vacuum data has full maximal globally hyperbolic developments with no future continuous nondegenerate extension whose weak connection is locally square-integrable. No symmetry is imposed; extensions need not satisfy the vacuum equations.

    Claimed, not checked

Operator algebras2

Topology5

  • 308Sep 23, 2026 Explained

    Finite Smith–Toda complexes at every height

    For every n ≥ 0, constructs a finite Smith–Toda spectrum at a prime p depending on n, with Brown–Peterson homology BP∗/(p,v1,…,vn)BP_*/(p,v_1,\ldots,v_n) and the canonical comodule structure. Thus Smith–Toda complexes exist at every height when the prime may vary; an explicit example realizes V(4)V(4) at p = 1009.

    Claimed, not checked
  • 309Sep 24, 2026 Explained

    The Kervaire invariant problem at the prime three

    Resolves the odd-primary Kervaire invariant problem at the prime three: exactly the standard classes with indices 0, 2, and 3 survive in the mod-three Adams spectral sequence, in stems 10, 106, and 322. Each surviving detection coset contains an element of exact additive order three.

    Claimed, not checked
  • 310Sep 24, 2026 Explained

    Quillen's conjecture in rational homology

    Proves the rational-homology form of Quillen's conjecture for every finite group and every prime. If the largest normal p-subgroup of G is trivial, the poset of nontrivial elementary abelian p-subgroups has nonzero augmented reduced rational homology and is therefore not contractible.

    Claimed, not checked
  • 315Sep 25, 2026 Explained

    The four-dimensional Singer conjecture

    Proves that the L2-Betti numbers of the universal cover of every closed connected aspherical topological four-manifold vanish outside degree two. More generally, the same conclusion holds for every finite connected aspherical integral Poincaré complex of formal dimension four, proving the four-dimensional Singer conjecture in this wider class.

    Claimed, not checked
  • 316Sep 25, 2026 Explained

    Curtis’s conjecture

    Proves Curtis’s conjecture: the positive-degree mod-two stable Hurewicz image of the sphere is spanned by the images of the Hopf-invariant-one classes η, ν, σ and the Kervaire-invariant-one classes that exist.

    Claimed, not checked

Functional analysis2

Differential geometry3

Partial differential equations3

  • 364Sep 23, 2026 Explained

    Kinetic limits and fluctuations over the Boltzmann lifespan

    Derives the nonlinear Boltzmann equation from three-dimensional grand-canonical Newtonian gases throughout every regular kinetic interval with uniform Gaussian decay. Stable finite-range radial potentials may have attractive wells and a singular repulsive core; initial pair exclusion and spatially summable Gaussian density and gradient bounds are assumed. A companion gives finite-dimensional hard-sphere Gaussian fluctuations, centered at the exact microscopic expectation and governed by the linear fluctuating Boltzmann equation.

    Claimed, not checked
  • 369Sep 24, 2026 Explained

    The hot spots conjecture for simply connected planar domains

    Proves a strict form of Burdzy's simply connected hot spots conjecture. On every smooth bounded simply connected planar domain, each nonzero eigenfunction for the first positive Neumann eigenvalue has no interior critical point, so all global extrema lie on the boundary. Eigenvalue multiplicity is allowed.

  • 375Sep 26, 2026 Explained

    De Giorgi's conjecture in dimension eight

    Proves De Giorgi's conjecture at its sharp dimension-eight endpoint: every entire C2 solution u:R8→(−1,1)u:\mathbb R^8\to(-1,1) of Δu=u3−u\Delta u=u^3-u that is strictly increasing in one direction depends on only one linear coordinate. A stronger theorem classifies all stable entire solutions v:R7→[−1,1]v:\mathbb R^7\to[-1,1] as constant wells or planar transitions, without an energy-growth assumption.

    Claimed, not checked

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