Lean-checked results

OpenAI lists a formal proof for these results: a proof written in the Lean language and checked by a computer, step by step. What exactly Lean checked is stated on each entry.

242 AI-made results with this trust label, from 475 papers in the OpenAI math collection, each explained in plain English. All of them have a formal Lean proof listed. They span 17 fields, led by theoretical computer science (34), combinatorics (33) and probability and statistical mechanics (19). The oldest question here dates back to 1896: The quasi-Riemann hypothesis. Results rated Landmark include Nagata’s conjecture and maximal Seshadri constants and Koebe’s circle-domain conjecture.

Number theory17

Algebraic and complex geometry8

  • 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.

  • 039Sep 23, 2026 Explained

    Nagata’s conjecture and maximal Seshadri constants

    Proves Nagata's strict inequality ∑imi<dr\sum_i m_i\lt d\sqrt r for every nonzero effective plane curve of degree d through r ≥ 10 very general complex points, with arbitrary multiplicities mi. It also proves maximal multipoint Seshadri constants (Ln/r)1/n(L^n/r)^{1/n} for every smooth polarized projective variety of dimension n ≥ 2 and all sufficiently large r: at very general points over ℂ, and at the geometric generic tuple over any algebraically closed field of positive characteristic.

  • 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.

  • 049Sep 24, 2026 Explained

    A stable-coordinate counterexample in four variables

    Constructs a polynomial in four complex variables that is not a coordinate but becomes one after adjoining a single variable, disproving the Stable Coordinate conjecture in four variables. Every fiber is affine three-space, yet none of its embeddings is rectifiable, also disproving the Abhyankar–Sathaye conjecture even when all fibers are affine spaces.

  • 050Sep 24, 2026 Explained

    A counterexample to Griffiths’ positivity conjecture

    Constructs ample rank-two bundles on P1×P1\mathbb P^1\times\mathbb P^1 with no smooth Hermitian metric of strictly Griffiths-positive curvature, disproving Griffiths' positivity conjecture already on the quadric surface.

  • 052Sep 23, 2026 Explained

    Tangent splittings and product decompositions

    A splitting of the tangent bundle of a compact Kähler manifold into two integrable holomorphic subbundles induces a compatible product decomposition of its universal cover, proving the two-summand form of Beauville's splitting conjecture. On smooth rationally connected projective manifolds, both summands are automatically integrable, establishing Höring's conjecture and the corresponding product decomposition.

  • 058Sep 24, 2026 Explained

    Semialgebraic universal covers and bounded domains

    Proves the Kollár–Pardon conjecture: the semialgebraic universal covers of connected normal projective complex varieties are exactly products D×Cm×FD\times\mathbb C^m\times F, with D bounded symmetric and F simply connected, normal, and projective. A universal cover is quasi-projective exactly when the bounded symmetric factor is absent. In particular, a smooth projective variety covered by ℂn has a finite étale cover by an abelian variety.

  • 066Sep 25, 2026 Explained

    Bounded klt complements for Fano contractions

    Proves the finite-rational-coefficient form of Shokurov’s bounded-klt-complement conjecture for ϵ-lc complex Fano-type pairs with nef anti-log-canonical divisor. For ϵ-lc Fano contractions over any algebraically closed characteristic-zero field, it gives klt complements near every base point, with index bounded only by dimension and positive rational ϵ.

Real and complex analysis10

Convex and metric geometry13

Theoretical computer science34

  • 102Sep 23, 2026 Explained

    The Unique Games Conjecture and optimal approximation thresholds

    Proves Khot's Unique Games Conjecture. Independent direct reductions also establish NP-hardness, on unweighted graphs, of approximation beyond the Goemans–Williamson ratio for Max-Cut, below factor two for Vertex Cover, and within any fixed constant factor for Min-UnCut and directed feedback vertex set. These direct proofs use established PCP and Label Cover hardness results.

  • 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.

  • 104Sep 25, 2026 Explained

    Quasipolynomial algorithms for mean-payoff, stochastic and parity games

    Gives deterministic algorithms using 2O((log⁡(L+2))2)2^{O((\log(L+2))^2)} bit operations, for complete binary input length L, for ordinary mean-payoff games and two separate extensions. They compute exact values and optimal positional strategies in ordinary games, the nonnegative expectation-of-liminf value set in turn-based stochastic games, and the winning set for nonnegative liminf mean payoff conjoined with parity. Signed rewards, rational chance probabilities, and parity priorities are unrestricted and binary-encoded.

  • 105Sep 23, 2026 Explained

    Perfect completeness for 2-to-1 games

    Proves Khot's 2-to-1 Games Conjecture with perfect completeness: for every fixed rational δ∈(0,1)\delta\in(0,1), it is NP-hard to distinguish satisfiable games from games whose optimum is at most δ, on explicit unweighted instances. The alphabet depends only on δ, and every right-hand label has exactly two preimages under each constraint map.

  • 106Sep 24, 2026 Explained

    Hardness of coloring three-colorable graphs

    It is NP-hard to color a three-colorable graph using any fixed number c ≥ 3 of colors. More strongly, for every fixed 0<δ<1/30\lt \delta\lt 1/3, a deterministic polynomial-time reduction from 3SAT produces simple unweighted graphs that are three-colorable in the satisfiable case and have no independent set of size δn\delta n otherwise, where n is the number of vertices.

  • 107Sep 24, 2026 Explained

    Matrix multiplication with exponent at most 9/4

    Proves ω≤9/4\omega\le9/4 over ℂ, giving Oε(n9/4+ε)O_\varepsilon(n^{9/4+\varepsilon}) arithmetic operations for square matrix multiplication. In characteristic zero, some inner dimension na with a > 0.465 permits n2+o(1)n^{2+o(1)} rectangular multiplication. Further square bounds give ω < 2.258 outside finitely many positive characteristics and ω < 2.371054886006746 over every fixed field.

  • 108Sep 24, 2026 Explained

    A cubic permanent–determinant lower bound

    Proves an Ω(n3)\Omega(n^3) lower bound for the border determinantal complexity of the n×nn\times n permanent over ℂ. Even coefficientwise limits of determinants of affine-linear matrices require matrix size at least cn3cn^3, for an absolute c > 0 and all sufficiently large n; the same bound therefore holds for exact representations.

  • 110Sep 24, 2026 Explained

    Optimal-order randomized k-server on arbitrary metrics

    Establishes a randomized competitive ratio O(log⁡2(k+1))O(\log^2(k+1)) for k-server on every metric space, matching the worst-case lower-bound order. One policy serves every finite oblivious request sequence, including on infinite unbounded metrics. On finite rational metrics, a uniform implementation has polynomial preprocessing and per-request bit cost in the input length and log⁡(t+1)\log(t+1) at request t, with a finite instance-dependent additive movement constant.

  • 111Sep 23, 2026 Explained

    One-sample matroid prophet inequalities against an almighty adversary

    For every finite matroid known in advance, gives a distribution-independent online rule using one independent sample per element and earning a universal constant fraction of the expected offline optimum. Values are independent and nonnegative, with finite expected optimum. The guarantee holds even when the arrival-order adversary sees all samples, values, and the rule's entire random seed; no polynomial-time implementation is asserted.

  • 112Sep 23, 2026 Explained

    Beyond the square-root exponent for depth-three circuits

    Constructs a single language in deterministic polynomial time whose n-bit membership function requires 2ω(n)2^{\omega(\sqrt n)} total gates in unbounded-fan-in OR–AND–OR circuits, at every sufficiently large input length. This crosses the square-root-exponent threshold for explicit depth-three Boolean circuit lower bounds.

  • 113Sep 23, 2026 Explained

    Approximate counting and entropy of perfect matchings

    Gives a fully polynomial randomized approximation scheme for counting perfect matchings in arbitrary finite simple graphs, with exact detection of zero counts. Also proves the perfect-matching entropy conjecture of Anari, Oveis Gharan, and Vinzant, bounding the maximum entropy of a matching law at every feasible edge-marginal vector in a loopless labelled multigraph, including boundary points.

  • 114Sep 23, 2026 Explained

    Approximate counting of common integer polymatroid bases

    Gives a fully polynomial randomized approximation scheme for counting common integer bases of two integral polymatroids of equal total rank, supplied by exact rank-value oracles. Capacities are binary-encoded, each integer vector counts once, and oracle calls and bit operations outside the oracles are polynomial on every execution. For matroids presented by independence oracles, the results also cover common independent sets of prescribed, unrestricted, or maximum cardinality, even when the ranks differ.

  • 115Sep 24, 2026 Explained

    Sampling and counting contingency tables with arbitrary margins

    For nonnegative integer matrices with prescribed row and column sums, gives exact uniform sampling in expected polynomial bit time and almost-uniform sampling in worst-case polynomial bit time. The dimensions and binary-encoded margins are unrestricted. Also gives a fully polynomial randomized approximation scheme for counting such tables with arbitrary individual cell bounds, including structural zeros, with polynomial cost on every execution.

  • 116Sep 24, 2026 Explained

    Uniform black-box noncommutative identity testing across characteristics

    For each characteristic, constructs in deterministic polynomial bit time a polynomial-dimensional matrix tuple detecting every nonzero division-free noncommutative formula of bounded size over any field of that characteristic. Rational formulas over ℚ also admit polynomial-size hitting lists whenever they have a defined rational-matrix evaluation.

  • 117Sep 24, 2026 Explained

    Uniform sparsest cut: hardness and semidefinite gaps

    Proves that approximating Uniform Sparsest Cut within any fixed constant factor is NP-hard, even with nonnegative rational capacities and unit demands. The Goemans–Linial semidefinite relaxation also has integrality gaps of order at least log⁡n/(log⁡log⁡n)3\sqrt{\log n}/(\log\log n)^3, approaching the square-root-logarithmic upper bound.

  • 118Sep 24, 2026 Explained

    Bin packing and unbounded configuration-LP gaps

    Disproves the modified integer round-up conjecture of Scheithauer and Terno: the integral bin-packing optimum can exceed its configuration linear-programming value by an arbitrarily large additive constant. Approximating the optimum within any fixed additive constant is also NP-hard, even when every item exceeds 1/6 and each bin holds at most five items.

  • 119Sep 24, 2026 Explained

    The Courtade–Kumar and Hellinger conjectures

    Proves the Courtade–Kumar conjecture: among Boolean functions of independent uniform bits, a single coordinate retains the most mutual information after independent bit-flip noise. A stronger theorem treats randomized binary summaries at fixed initial information. The Hellinger conjecture is also proved for every Boolean output bias and noise correlation.

  • 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.

  • 122Sep 24, 2026 Explained

    Quantitative trace-reconstruction bounds with a uniform decoder

    At every fixed deletion probability in (0,1)(0,1), reconstructing an arbitrary length-n binary string requires nΩ(log⁡log⁡n)n^{\Omega(\log\log n)} independent traces, ruling out polynomial-sample reconstruction. A uniform decoder achieves quasipolynomial sample and running-time bounds for known fixed rational retention probabilities. When the deletion probability is at most n−εn^{-\varepsilon} for fixed ε > 0, both bounds become polynomial in the input and parameter encoding.

  • 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.

  • 125Sep 24, 2026 Explained

    The metric k-median approximation threshold and recovery

    Gives a deterministic polynomial-time (1+2/e+ε)(1+2/e+\varepsilon)-approximation for finite rational metric k-median with specified candidate facilities, for every fixed ε > 0. Assuming P≠NPP\ne NP, the optimal infimum approximation factor is 1+2/e1+2/e.

  • 126Oct 5, 2026 Explained

    Exponential semidefinite complexity of perfect matching

    Proves that every exact semidefinite lift of the perfect matching polytope has exponential size, answering Rothvoss's polynomial-size lift question negatively. The bound holds even for the positive semidefinite rank of its odd-cut slack matrix after any fixed shift 0<ρ<10\lt \rho\lt 1, allowing arbitrary real positive semidefinite factors.

  • 127Sep 25, 2026 Explained

    Average sensitivity of polynomial threshold functions

    Proves that a degree-at-most-d polynomial threshold function on the uniform n-dimensional Boolean cube has average sensitivity at most 8dn8d\sqrt n, uniformly for 1≤d≤n1\le d\le n. Average sensitivity counts expected output changes under single-bit flips. This establishes the asymptotic Gotsman–Linial conjecture, allowing polynomial zeros with sign(0)=1\mathop{\mathrm{sign}}\nolimits (0)=1.

  • 128Sep 24, 2026 Explained

    A factor-two approximation for shortest common superstring

    Gives a deterministic polynomial-time algorithm constructing a common superstring of length at most twice the optimum for every finite family of explicitly represented strings. The running time is polynomial in the full encoded input length, including symbol labels.

  • 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.

  • 130Sep 25, 2026 Explained

    Exact Fourier transforms below nlog⁡nn\log n

    Gives a deterministic length-n discrete Fourier transform algorithm using O(n(log⁡n)1−δ)O(n(\log n)^{1-\delta}) operations for every n, with explicit δ=10−13\delta=10^{-13}. The model uses exact complex arithmetic, unrestricted coefficients and a supplied root of unity, and counts scalar preparation and logarithmic-word indexing.

  • 131Sep 25, 2026 Explained

    Rapid mixing of graph switches for every degree sequence

    Resolves the simple-undirected Kannan–Tetali–Vempala conjecture: the lazy edge-switch chain mixes in O(n8)O(n^8) time for every graphical labeled degree sequence. The same degree-constrained graphs can also be sampled exactly uniformly by an almost-surely terminating algorithm with expected polynomial bit running time.

  • 132Sep 25, 2026 Explained

    A superquadratic separation of sensitivity and block sensitivity

    Constructs total Boolean functions with block sensitivity bs(f)≥s(f)α\mathop{\mathrm{bs}}\nolimits (f)\ge s(f)^\alpha for a fixed α > 2, disproving the quadratic strengthening of the Sensitivity Conjecture. Here s(f)s(f) counts influential individual-bit flips, while block sensitivity allows disjoint groups of bits to change together.

  • 133Sep 25, 2026 Explained

    The computational complexity of Weisfeiler–Leman refinement

    Proves unconditional nΩ(k)n^{\Omega(k)} deterministic time lower bounds for joint and separate k-dimensional Weisfeiler–Leman equivalence, for sufficiently large fixed k in the specified sequential adjacency-matrix models. With dimension as input, joint equivalence is EXPTIME-complete even on subcubic graphs; deciding whether refinement identifies a graph is also EXPTIME-complete.

  • 134Sep 25, 2026 Explained

    Generalized star height at most three

    Every regular language over a finite alphabet has a generalized regular expression with at most three nested Kleene stars, allowing union, concatenation and complement over the same alphabet. This establishes an absolute bound independent of automaton size, resolving the uniform-boundedness version of the generalized star-height problem.

  • 135Sep 25, 2026 Explained

    Homogeneous depth-five lower bounds for iterated matrix multiplication

    Over every characteristic-zero field, the (1,1)(1,1) entry of a product of n independent n×nn\times n variable matrices requires nΘ(n)n^{\Theta(\sqrt n)} gates in homogeneous depth-five sum–product circuits. This sharp bound allows shared gates and bottom linear forms involving all variables.

  • 137Sep 25, 2026 Explained

    One-tape time simulation in two-fifths-power space

    Determines the halting and finite-control outcome of a fixed deterministic one-writable-tape machine up to time T using O(T2/5log⁡C(T+2))O(T^{2/5}\log^C(T+2)) space, improving the square-root exponent. Heads move at most one cell per step; finitely many read-only input heads are allowed. Initial contents are independent of T, and contents and input symbols have polylogarithmic-space access. Simulation time is unrestricted.

  • 139Sep 26, 2026 Explained

    Subpolynomial query complexity for log-concave sampling

    For C2 potentials with a supplied minimizer and I⪯∇2V⪯2II\preceq\nabla^2V\preceq2I, proves that sampling within total variation 1/10 requires only CεdεC_\varepsilon d^\varepsilon exact value-and-gradient queries for every fixed ε > 0. The bound holds on every run, with unrestricted computation between queries. A logarithmic lower bound also holds, so the optimal power-law exponent in this oracle model is zero.

  • 140Sep 27, 2026 Explained

    Memory–sample lower bounds for noiseless Gaussian regression

    For fixed A > 0, a one-pass learner with Ad2Ad^2 persistent bits needs ΩA(dlog⁡(1/ϵ))\Omega_A(d\log(1/\epsilon)) noiseless Gaussian samples to recover a unit vector to angular error 0<ϵ≤1/100\lt \epsilon\le1/10 with probability 2/3, uniformly in accuracy for large d. Computation and randomized updates are unrestricted, but output uses only the terminal state, stopping index and fresh randomness.

Dynamical systems and ergodic theory9

Combinatorics33

Algebra10

Probability and statistical mechanics19

  • 211Sep 24, 2026 Explained

    The geometric phase diagram, diffusion, and spectra of random planar maps

    Critical Fortuin–Kasteleyn planar maps converge to Liouville quantum gravity spheres for 0<q≤40\lt q\le4 and to the Brownian continuum random tree for q > 4, establishing the surface-to-tree geometric transition. For FK–Ising and spanning-tree-weighted maps, stationary random walks converge to Liouville Brownian motion on the limiting sphere. The FK–Ising spectral result also gives convergence of eigenvalues and heat traces, using the stated Brownian/LQG inputs.

  • 212Sep 24, 2026 Explained

    Planar first-passage geometry and the absence of bigeodesics

    Proves that planar first-passage percolation has no doubly infinite geodesic for iid nonnegative nonatomic edge weights when the minimum of four weights has finite second moment. For exponential weights, the limit shape is strictly convex with C1 boundary. Differentiability also holds for every Gamma law with positive shape and rate.

  • 213Sep 24, 2026 Explained

    Critical percolation on every quasi-transitive graph

    Resolves the Benjamini–Schramm criticality conjecture for bond percolation on every infinite connected locally finite quasi-transitive graph with pc<1p_c\lt 1: at the critical probability, there is almost surely no infinite cluster. The family also establishes this conclusion for both nearest-neighbor bond and site percolation on ℤ3.

  • 214Sep 24, 2026 Explained

    The Benjamini–Schramm nonuniqueness conjecture

    Proves pc<pup_c\lt p_u for Bernoulli bond percolation on every infinite connected locally finite nonamenable quasi-transitive graph, resolving the Benjamini–Schramm nonuniqueness conjecture. Thus there is a nonempty range of probabilities with infinitely many infinite clusters. A stronger operator bound also establishes the critical triangle condition.

  • 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.

  • 218Sep 23, 2026 Explained

    Conformal universality for weakly interacting and random-bond Ising models

    Weak finite-range square-symmetric even multispin perturbations of the square-lattice Ising model preserve critical bulk spin and energy limits; weak square-symmetric contour interactions also yield chordal SLE3 interface limits. With sufficiently weak iid bond disorder of any fixed bounded nondegenerate mean-zero law, critical spin interfaces converge to the same law in probability over environments.

  • 220Sep 23, 2026 Explained

    Directional zero–one laws beyond iid environments and iid ballisticity

    On ℤd, d ≥ 3, directional escape has probability zero or one for iid strictly elliptic nearest-neighbor environments, and for stationary ergodic finite-range-dependent environments under uniform ellipticity. In iid uniformly elliptic environments with d ≥ 2, almost-sure directional transience implies a deterministic limiting velocity with positive projection in that direction, resolving the ballisticity conjecture.

  • 221Sep 23, 2026 Explained

    The Mézard–Parisi formula for diluted spin glasses

    Proves the Mézard–Parisi hierarchical cavity formula for Poisson-diluted even-arity Ising models satisfying the Panchenko–Talagrand factorization and positivity assumptions, with only first-moment integrability. The limiting free energy equals the infimum over finite-depth hierarchical trial laws. This includes the Viana–Bray model, symmetric diluted even-spin models, and weighted soft even-K satisfiability.

  • 222Sep 24, 2026 Explained

    Perceptron free energies and microscopic jamming exponents

    Determines finite-temperature variational free energies for Gaussian Ising perceptrons with bounded Borel log-potentials and Gaussian spherical perceptrons with bounded continuous potentials, at every positive pattern density. A spherical extension treats bi-orthogonally invariant disorder with compact limiting singular-value distributions and no outliers. At margin −1, the quadratic-penalty spherical model has a sharp feasibility threshold and limiting gap and force laws, with system size, zero temperature, and critical density taken in that order.

  • 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.

  • 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.

  • 230Sep 25, 2026 Explained

    Exact Hausdorff gauges for SLE

    Resolves Schramm’s Hausdorff-measure question for chordal SLEκ, 0<κ<80\lt \kappa\lt 8. The explicit gauge rd(log⁡log⁡(1/r))(2−d)/2r^d(\log\log(1/r))^{(2-d)/2}, d=1+κ/8d=1+\kappa/8, gives almost surely positive finite measure to every trace segment γ([s,t])\gamma([s,t]) with 0<s<t<∞0\lt s\lt t\lt \infty, and finite expected measure to the trace in every bounded disk.

  • 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.

  • 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.

  • 235Sep 25, 2026 Explained

    Limiting random SAT thresholds, sharp variance and computability

    For random k-SAT with independent uniformly signed proper clauses sampled with replacement, proves finite positive limiting thresholds and hitting-time variance Θk(n)\Theta_k(n) for every fixed k ≥ 3, and computability of the 3-SAT threshold. We credit Gaia Carenini with priority for resolving the threshold-existence conjecture in her concurrent [ECCC TR26-229](https://eccc.weizmann.ac.il/report/2026/229/), made public October 5, 2026; this family supplies another proof and the sharper variance and computability results.

  • 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.

  • 237Sep 26, 2026 Explained

    The three-quarter exponent for honeycomb self-avoiding walk

    Proves the diameter form of Nienhuis's predicted three-quarter exponent: a uniformly chosen n-step self-avoiding walk on the honeycomb lattice has diameter n3/4+o(1)n^{3/4+o(1)}. Its local mass and covering numbers have exponent 4/3. These estimates hold at every sufficiently large fixed length, simultaneously across scales, with arbitrarily high polynomial probability.

  • 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.

Mathematical logic6

Group theory12

Mathematical physics17

  • 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.

  • 261Sep 23, 2026 Explained

    Localization and delocalization in the Anderson model

    Resolves the predicted spectral contrast for the lattice Anderson model with independent uniform site potentials. In dimension two, every positive disorder strength gives almost surely pure-point spectrum. In every fixed dimension d ≥ 3, sufficiently weak positive disorder gives purely absolutely continuous spectrum on a fixed open interval with nonzero spectral weight.

  • 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.

  • 263Sep 24, 2026 Explained

    The ionization and generalized ionization conjectures

    For the full nonrelativistic Coulomb model with two electron spin states, proves that a molecule with M fixed nuclei of charges at least one and total charge Z strictly binds at most Z+CMZ+CM electrons. Neutral-atom first ionization energies and radii containing all but an expected half-electron have universal positive upper and lower bounds. The energy cost of removing m electrons has Thomas–Fermi asymptotics as m→∞m\to\infty and Z/m→∞Z/m\to\infty; neutral-atom outer radii have the corresponding iterated-limit asymptotics, taking Z→∞Z\to\infty first.

  • 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.

  • 267Sep 24, 2026 Explained

    Positive-temperature Bose–Einstein condensation and exact quantum depletion

    Proves Bose–Einstein condensation for the exact canonical Gibbs state of the three-dimensional hard-sphere gas: each fixed exclusion distance and sufficiently small fixed density admit a strictly positive temperature, independent of volume, with positive condensate fraction in the thermodynamic limit. At zero temperature, proves the Bogoliubov leading quantum-depletion law for hard spheres and fixed bounded nonnegative radial finite-range potentials of positive scattering length, taking the thermodynamic limit before the dilute limit.

  • 269Sep 24, 2026 Explained

    Uniform Laughlin gap and stability under bounded scalar disorder

    Proves the fermionic Laughlin spectral-gap conjecture for the full V1 interaction at filling 1/3 on the round sphere. The unique ground state remains uniformly gapped under sufficiently weak bounded real scalar one-body potentials projected to the lowest Landau level. Both the gap and disorder threshold are uniform over all sufficiently large particle numbers and all normalized potential profiles.

  • 271Sep 24, 2026 Explained

    Bloch's law, its lattice correction, and the spherical magnetization law

    Proves Bloch's T3/2 law with its exact coefficient for three-dimensional quantum Heisenberg ferromagnets at every positive quantum spin, allowing nonnegative symmetric finite-range couplings whose support generates ℤ3. The thermodynamic limit precedes the zero-field derivative and low-temperature limit. The family also proves spontaneous magnetization for nearest-neighbor models in every dimension d ≥ 3 and determines the first lattice correction for three-dimensional nearest-neighbor couplings.

  • 272Sep 27, 2026 Explained

    Entanglement without distillable secret key

    Constructs an entangled state on C10⊗C10\mathbb C^{10}\otimes\mathbb C^{10} with zero distillable secret key for the specified local-instrument protocols that complete almost surely. These allow joint local processing and authenticated two-way public communication, with no other shared private resource and an eavesdropper holding the input purification and public record. A trace-preserving PPT channel on M21(C)M_{21}(\mathbb C) whose square is not entanglement breaking disproves Christandl's PPT-square conjecture.

  • 273Sep 24, 2026 Explained

    The entropy photon-number inequality

    Proves the entropy photon-number inequality for beam-splitter mixing of two independent finite-energy bosonic inputs in any finite number of modes: the output's entropy photon number is at least the transmissivity-weighted average of the inputs'. Arbitrary entanglement within each input is allowed, and product thermal inputs attain equality even when their entropies differ.

  • 274Sep 24, 2026 Explained

    Parity is not in QAC0

    Resolves Moore's parity conjecture in the measured-output model: constant-depth quantum circuits with arbitrary one-qubit gates, unbounded-arity Toffoli gates and polynomially many total qubits cannot compute parity with any fixed positive worst-case advantage. Ancillas start in zero, one output qubit is measured, and all other registers may be discarded. Xu–Li's reductions give the same bounded-error obstruction for strict majority.

  • 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.

  • 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.

  • 280Sep 25, 2026 Explained

    Unitary vertex operator algebras and conformal nets

    Proves the strongly rational case of the strong-locality conjecture: every simple unitary strongly rational complex vertex operator algebra generates a completely rational conformal net. Its simple modules are unitarizable, and its representation category agrees with the net’s finite-index sectors as a braided unitary tensor category.

  • 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 algebras15

Topology3

Functional analysis10

Differential geometry15

Partial differential equations11

  • 362Sep 23, 2026 Explained

    Global smoothness for relativistic Vlasov–Maxwell

    Proves large-data global existence and uniqueness for the three-dimensional, one-species relativistic Vlasov–Maxwell system. Smooth admissible initial data may be arbitrary provided the particle density is compactly supported and the electromagnetic fields have finite energy and bounded derivatives of every order; the solution remains smooth on every finite time interval.

  • 363Sep 23, 2026 Explained

    Nonuniqueness with local conservation for the hard-sphere Boltzmann equation

    Constructs two distinct global entropy solutions of the three-dimensional periodic hard-sphere Boltzmann equation from the same nonnegative initial density, with bounded velocity support and finite mass, energy and absolute entropy. Both are strongly continuous in L1 and satisfy exact local conservation of mass, momentum and kinetic energy.

  • 365Sep 23, 2026 Explained

    Joint metric and connection recovery from one boundary patch

    Zero-frequency measurements on any nonempty open boundary patch determine a smooth metric and smooth unitary connection on a trivial Hermitian rank-two bundle over a compact connected manifold of dimension at least three, up to diffeomorphism and gauge fixed on that patch. Inputs and observations use the same patch. In contrast, distinct uniformly positive bounded measurable scalar conductivities on a three-dimensional ball can have identical full-boundary data.

  • 367Sep 24, 2026 Explained

    The critical dimension for the one-phase Bernoulli problem

    Establishes seven as the first dimension admitting a nonflat, one-homogeneous global minimizer of the one-phase Bernoulli energy. Consequently, minimizing free boundaries are smooth through dimension six, and their singular sets have dimension at most n−7n-7 in higher dimensions.

  • 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.

  • 370Sep 24, 2026 Explained

    The Lane–Emden and Hénon–Lane–Emden conjectures

    Resolves the subcritical Lane–Emden conjecture and its weighted Hénon extension. For n ≥ 2, p,q>0p,q\gt 0 and real A, B, the system −Δu=∣x∣Avp-\Delta u=|x|^A v^p, −Δv=∣x∣Buq-\Delta v=|x|^B u^q has no positive entire solution when (n+A)/(p+1)+(n+B)/(q+1)>n−2(n+A)/(p+1)+(n+B)/(q+1)\gt n-2, with solutions continuous at the origin and classical elsewhere. No symmetry or growth assumption is needed. Known radial existence gives the exact existence criterion for n ≥ 3 and A,B>−2A,B\gt -2.

  • 371Sep 24, 2026 Explained

    Stable blowup for the defocusing Schrödinger equation

    For a sufficiently large odd nonlinearity power, constructs a nonempty open set of initial data in Hk(T12)H^k(\mathbb T^{12}), with k > 8, whose solutions of the scalar defocusing nonlinear Schrödinger equation blow up in finite time. Thus finite-time blowup is stable under Sobolev perturbations in this supercritical regime.

  • 372Sep 24, 2026 Explained

    Global uniqueness in smooth isotropic elasticity

    Proves that full static boundary displacement-to-traction data determine both smooth real Lamé moduli on every bounded connected smooth domain in ℝ3, provided μ > 0 and 3λ+2μ>03\lambda+2\mu\gt 0 on the closure. Neither analyticity, proximity to constant coefficients nor prior knowledge near the boundary is required.

  • 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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