Solid results

Results rated Solid: real progress on narrower or more technical questions.

50 AI-made results rated Solid, from 98 papers in the OpenAI math collection, each explained in plain English. 37 have a formal Lean proof listed; 13 are claimed in a paper and not yet machine-checked. They span 14 fields, led by probability and statistical mechanics (9), combinatorics (8) and mathematical physics (8). The oldest question here dates back to 1943: The joint critical Ashkin–Teller current limit.

Number theory1

Algebraic and complex geometry5

  • 035Sep 24, 2026 Explained

    Log-canonical threefold abundance in numerical dimension one

    Proves log abundance for projective log canonical threefold pairs over algebraically closed fields of characteristic p > 3 when the effective boundary is rational and the ℚ-Cartier adjoint is nef of numerical dimension one. The adjoint is semiample, without requiring the original variety to be terminal or ℚ-factorial.

    Claimed, not checked
  • 043Sep 24, 2026 Explained

    P = W for fixed-determinant SLn moduli spaces

    Proves Pk=W2k=W2k+1P_k=W_{2k}=W_{2k+1} on the full rational cohomology of smooth coprime fixed-determinant, trace-free Higgs moduli spaces and their character varieties for composite ranks over smooth projective complex curves of genus at least two. This includes variant cohomology and, together with the known prime-rank theorems, establishes the fixed-determinant P = W conjecture in every coprime rank.

    Claimed, not checked
  • 044Sep 24, 2026 Explained

    The equivariant cohomological Hikita conjecture

    Proves the equivariant cohomological Hikita correspondence for every finite quiver, including loops and multiple arrows, with arbitrary dimension and framing vectors and commuting flavor torus. When every semistable point is stable and the gauge action is free, the equivariant cohomology of the Nakajima variety is canonically the coordinate ring of the scheme-theoretic cocharacter-fixed locus of its flavor-deformed Coulomb branch.

    Claimed, not checked
  • 055Sep 24, 2026 Explained

    Gepner symmetry and large-volume stability on threefolds

    Proves Toda's Gepner conjecture for every smooth complex quintic threefold, constructing a numerical Bridgeland stability condition with the prescribed phase shift 2/5. Also constructs numerical Bridgeland stability conditions at every sufficiently large volume on all smooth projective complex threefolds with trivial canonical bundle, with the exact ordinary and square-root-Todd central charges.

    Claimed, not checked
  • 067Sep 25, 2026 Explained

    The Campana–Peternell conjecture in dimension six

    Proves the Campana–Peternell conjecture in complex dimension six: every smooth connected complex projective Fano sixfold with nef tangent bundle is rational homogeneous.

    Claimed, not checked

Convex and metric geometry1

Theoretical computer science3

Combinatorics8

Algebra2

  • 204Sep 24, 2026 Explained

    Tensor saturation for even spin groups

    Proves saturation factor one for Spin(2n)\mathop{\mathrm{Spin}}\nolimits (2n), n ≥ 2: for three dominant integral weights whose sum lies in the root lattice, an invariant at any common positive integral dilation already gives an invariant at the original weights. This resolves the type-D part of the simply-laced saturation conjecture.

    Claimed, not checked
  • 210Sep 25, 2026 Explained

    Foulkes' conjecture for sixth powers and quadratic stabilization

    Proves the sixth case of Foulkes’ conjecture: Sym6(SymbV)\mathop{\mathrm{Sym}}\nolimits ^6(\mathop{\mathrm{Sym}}\nolimits ^bV) embeds equivariantly in Symb(Sym6V)\mathop{\mathrm{Sym}}\nolimits ^b(\mathop{\mathrm{Sym}}\nolimits ^6V) for every b ≥ 6 and finite-dimensional complex V. More generally, the canonical multiplication map Symb(SymaV)→Syma(SymbV)\mathop{\mathrm{Sym}}\nolimits ^b(\mathop{\mathrm{Sym}}\nolimits ^aV)\to\mathop{\mathrm{Sym}}\nolimits ^a(\mathop{\mathrm{Sym}}\nolimits ^bV) is surjective for a ≥ 2 and b≥a(a−1)b\ge a(a-1), giving dimension-independent quadratic stabilization.

Probability and statistical mechanics9

  • 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.

  • 229Sep 25, 2026 Explained

    Exact three- and four-state reconstruction thresholds and four-state tree capacity

    Proves the exact reconstruction threshold dλ2>1d\lambda^2\gt 1, with nonreconstruction at equality, for three-state symmetric and four-state ferromagnetic broadcasting on regular trees (d ≥ 2) and observed Poisson trees (mean d > 1 and d > 0, respectively), with Poisson advantage averaged without conditioning on survival. The three-state theorem allows both signs of λ and gives the exact weak-recovery threshold for the symmetric three-community stochastic block model.

  • 231Sep 25, 2026 Explained

    The free uniform spanning forest is a factor of IID

    On every infinite connected locally finite simple unweighted graph, the free uniform spanning forest is a factor of independent vertex labels, by one isomorphism-equivariant rule using no root. Translation-invariant strongly Rayleigh binary processes on every countable group, including invariant determinantal processes with Hermitian positive-contraction kernels, are also factors of IID.

  • 232Oct 6, 2026 Explained

    Gaussian fields and interfaces for triangular-lattice Lipschitz heights

    Proves Gaussian free field limits on bounded smooth simply connected domains for triangular-lattice height models: uniform odd heights with increments 0,±20,\pm2 and two-arc boundary values ±1\pm1, and zero-boundary integer Lipschitz heights weighted by fixed x∈[1/2,1]x\in[1/\sqrt2,1]. Uniform real Lipschitz heights also converge to a Gaussian field; at a tuned opposite-boundary amplitude, their interface converges to chordal SLE4, establishing Schramm’s real-field/interface predictions.

    Claimed, not checked
  • 233Oct 6, 2026 Explained

    The joint critical Ashkin–Teller current limit

    Identifies the joint scaling limit of Ashkin–Teller heights and both complete current-cluster collections throughout the critical line, including the four-state Potts endpoint. In bounded Jordan domains with admissible lattice approximations and wired primal/free dual boundaries, the height converges to the predicted Gaussian free field, and the clusters to canonical recursive sets of that same field, retaining every nesting depth.

    Claimed, not checked
  • 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.

  • 236Sep 26, 2026 Explained

    The exact factor-of-IID threshold for free Ising spins on trees

    Determines when the free zero-field ferromagnetic Ising state on the infinite d-regular tree is a factor of independent vertex labels: exactly when tanh⁡β≤(d−1)−1/2\tanh\beta\le(d-1)^{-1/2}, including equality, for d ≥ 3 and β ≥ 0. The construction uses no root and is almost surely equivariant for each fixed tree automorphism, resolving the ferromagnetic case of Lyons's question.

  • 238Sep 26, 2026 Explained

    Optimal logarithmic mixing of the Thorp shuffle

    Proves that the Thorp shuffle randomizes N=2dN=2^d labeled cards in Θ(log⁡N)\Theta(\log N) physical shuffles, settling its optimal mixing order for power-of-two deck sizes. Convergence is in total variation from the worst initial ordering and concerns the entire permutation, not just individual card positions.

  • 239Oct 3, 2026 Explained

    Sharp singularity rates for symmetric random sign matrices

    Determines the sharp exponential singularity rate of symmetric random sign matrices with independent entries on and above the diagonal. Uniform signs give Pr⁡(det⁡An=0)=(1/2+o(1))n\Pr(\det A_n=0)=(1/2+o(1))^n; for fixed bias p∈(0,1)∖{1/2}p\in(0,1)\setminus\{1/2\}, the rate is (p2+(1−p)2+o(1))n(p^2+(1-p)^2+o(1))^n. In the biased case, agreeing rows attain this rate.

    Claimed, not checked

Mathematical logic1

Mathematical physics8

  • 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.

  • 266Sep 24, 2026 Explained

    Exactly three mutually unbiased bases in dimension six

    Proves N(6)=3N(6)=3, resolving Zauner's dimension-six mutually unbiased bases conjecture: three such bases exist in ℂ6, but four cannot. The exclusion is a complete certified computation under the stated binary64 arithmetic and compiler conditions. An independent companion proves the Matolcsi–Ruzsa–Weiner Fourier-vanishing conjecture for order-six complex Hadamard matrices outside Tao's cubic equivalence class.

  • 275Sep 24, 2026 Explained

    QMA-hardness of continuum Coulomb energy

    Proves QMA-hardness of approximating the electronic Coulomb energy infimum in three dimensions, minimizing over the full spinful fermionic continuum space. Deterministic polynomial-time reductions work even with only unit-charge nuclei at distinct rational positions, polynomially many electrons and an energy-threshold separation of at least one.

  • 276Sep 24, 2026 Explained

    Classical capacity of generalized amplitude damping

    Determines the unassisted classical capacity of every qubit generalized amplitude-damping channel, including all damping and thermal parameters. An explicit one-variable optimization gives the capacity, attained by independent two-state signal ensembles with collective decoding. Holevo capacity, minimum output entropy and regularized classical capacity are additive when tensoring with any finite-dimensional quantum channel.

  • 277Sep 25, 2026 Explained

    Threshold repetition for entangled games

    Proves exponential threshold repetition for every finite two-player one-round game: if its entangled value is v < 1, the probability of winning at least a fraction v+δv+\delta of k independent repetitions decays exponentially in k, for 0<δ<1−v0\lt \delta\lt 1-v. Arbitrary joint finite-dimensional entangled strategies and correlated question distributions are allowed.

  • 278Sep 25, 2026 Explained

    Failure of Kohn–Sham ensemble representation

    Constructs a three-electron Coulomb molecule with two equal positive-integer-charge nuclei whose absolute ground-state density has no noninteracting ground-state ensemble representation by a single real spin-independent local potential in L3/2(R3)+L∞(R3)L^{3/2}(\mathbb R^3)+L^\infty(\mathbb R^3). This disproves Kohn–Sham ensemble representability for that potential class; the required nuclear charge is specified nonnumerically.

    Claimed, not checked
  • 279Sep 25, 2026 Explained

    Exact quantum factoring over a fixed finite gate set

    Gives a polynomial-time uniform quantum circuit family that outputs the complete prime factorization of every integer with probability one. Both gate count and qubit count are polynomial in the input length, and one fixed finite gate set suffices.

  • 281Sep 25, 2026 Explained

    QAOA attains the SK optimum in the thermodynamic-first limit

    Proves that QAOA approaches the ground-state energy of the Gaussian zero-field Sherrington–Kirkpatrick model when system size tends to infinity before circuit depth. For every accuracy, finite depth and deterministic angles independent of size and disorder achieve the required limiting expected energy per spin. This also yields leading-order optimal expected MaxCut values on large-degree random regular graphs, with size tending to infinity before degree.

Operator algebras1

  • 297Sep 24, 2026 Explained

    A ZFC counterexample to Naimark's problem

    Gives an alternative to [Tanaka's ZFC construction](https://arxiv.org/abs/2609.26930v1) of a unital infinite-dimensional simple complex C∗-algebra with a faithful tracial state and exactly one nonzero irreducible representation up to unitary equivalence. Thus the unrestricted compact-operator characterization fails without additional set-theoretic assumptions; the counterexample is nonseparable.

Topology2

Functional analysis2

Differential geometry4

Partial differential equations3

  • 373Sep 25, 2026 Explained

    Nonattainment of the three-marginal Coulomb Monge problem

    An optimal three-particle Coulomb configuration need not be a deterministic function of the first particle, even for smooth identical spatial densities. The Monge and Kantorovich infima agree, but the Monge infimum is not attained. The same phenomenon occurs for every inverse-power Riesz exponent in each dimension at least two, with a suitable density in each case.

  • 374Sep 25, 2026 Explained

    Sharp one-third stability of Brenier maps

    For uniform source measure ρ on a compact convex body with interior in dimension at least two, quadratic optimal transport maps satisfy ∥Tμ−Tν∥L2(ρ)≤CW2(μ,ν)1/3\|T_\mu-T_\nu\|_{L^2(\rho)}\le C W_2(\mu,\nu)^{1/3} uniformly over targets in a fixed compact set. The exponent is sharp, even for three-atom targets, disproving Letrouit's conjectured square-root bound.

  • 376Sep 27, 2026 Explained

    Universal computation in forced Navier–Stokes flows

    Constructs viscous incompressible flows starting from rest on a fixed flat three-dimensional domain that perform universal computation under smooth external forcing. A terminating compiler turns a Turing machine and input into a finite program for the force, so a designated particle reaches a fixed region exactly when the machine halts. The viscosity is fixed, positive and computable.

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