Partial differential equations · incompressible flow · harmonic analysis

Navier–Stokes Existence and Smoothness

Collaboration beta

Does viscosity keep every permitted smooth three-dimensional incompressible flow smooth for all future time? The current source studies constraints on a hypothetical breakdown through conditional exact-core and neutral Euler profiles. It reports useful carrier, variance and value-current restrictions, while keeping their assumptions separate. A missing PDE estimate and an exhaustive transfer from arbitrary initial data to all relevant alternatives still prevent a proof of the full problem.

ν>0, u0S(3;3), u0=0: (u,p)smooth on3×[0,),tu+(u)u+p=νΔu,u=0,u(0)=u0,supt0|u(t)|22<
Clay Millennium Prize Problems
Known results and sources
Illustration: Blue and copper stream ribbons in a dark three-dimensional volume accompany the open question of smooth incompressible flow for all future time.
Illustration: Does positive viscosity preserve smoothness for every permitted three-dimensional initial flow?

Research problem

Exact mathematical statement

For every viscosity ν>0\nu>0 and every smooth, divergence-free initial velocity u0:33u_0: \mathbb R^3\to\mathbb R^3 that is rapidly decreasing with all derivatives, find smooth velocity and pressure on 3×[0,)\mathbb R^3\times[0,\infty) satisfying the unforced incompressible Navier–Stokes equations, the prescribed initial data and a uniform kinetic-energy bound:

tu+(u)u+p=νΔu,u=0,u(0)=u0,supt03|u(x,t)|2dx<.\partial_tu+(u\cdot\nabla)u+\nabla p=\nu\Delta u,\qquad\nabla\cdot u=0,\qquad u(0)=u_0,\qquad\sup_{t\ge0}\int_{\mathbb R^3}|u(x,t)|^2\,dx<\infty.

This is the whole-space existence and smoothness alternative for every permitted datum. Periodic, forced, Euler, weak-solution or restricted-data statements do not replace it. The current source reports no resolution.

Problem infographic

Problem at a glance

Illustration: Smooth three-dimensional flow, incompressibility, positive viscosity and finite energy lead to an open question: smooth flow for all future time, or finite-time breakdown. The ribbons are schematic.
Illustration: For every positive viscosity and every smooth, divergence-free initial velocity on ℝ³ that decreases rapidly with all derivatives, the unforced problem asks for global smooth velocity and pressure with the prescribed initial data and uniformly bounded kinetic energy. The source establishes neither an all-data proof nor a counterexample.

Current mathematical picture

Where work on Navier–Stokes Existence and Smoothness stands

Open problem

recorded v56 frontier for the unforced all-data whole-space existence target: retain unresolved upstream extraction, baseline-EC current/carrier routes and additional MP/positive-defect hypotheses. Preserve v6 factual scope, the inactive historical computation and all source corrections without promoting reported audits or unopened proof owners.

Leading routeDirect exact-core angular and carrier routes

This route keeps the direct angular obstruction at EC-WEAK scope and the centered local carrier identity at baseline-EC scope. Neither requires MP. Angular rank two remains possible. The centered carrier has baseline windows T=L a^(−4/3), improved under EC-WEAK to T=L/a, with fixed-L endpoint error O(1/L) and no implicit interchange of limits. A vanishing complete signed interface mean on the appropriate clock would close that core, but the required depletion is open; absolute-value replacements lose the cancellation.

Route status · Active route
Useful failureSource-reported limitation

A moment-defined characteristic frequency by itself does not supply the Fourier-support hypothesis needed for wake decoupling. The retained architecture would need a production-bearing component with enough compactness and inherited growth to enter a narrow rigidity theorem, together with a reduction of collective multiplicity and a separate treatment of the zero-viscosity corridor.

Route status · Narrowed route
Main reductionCorridor-generated active increment

The source labels the corridor-generated increment theorem as derived in Revision 6.

Evidence posture · Source-reported route statement · dependencies incomplete
Priority open bridgeV49-I

Adjudicate actual dissipative profiles after the exact MP provider, not an arbitrary Euler profile.

Task status · Ready to work on
Research-record correctionResearch-record correction

We corrected the cited passages. The mathematical claims and their status did not change.

Reader-facing record corrected; mathematics unchanged

Work mapped so far

Navier–Stokes Existence and Smoothness in numbers

6kretained lines of mathematical investigation1,196 in the current working snapshot
Argument development
5,158 · 86%
Explored or eliminated routes
149 · 2%
Computational analysis
11 · 0%
Open obligations
276 · 5%
Definitions and setup
392 · 7%
23selected mapped statements5routes investigated20open questions20contribution-ready tasks
How this is measured

This measures retained mathematical investigation, not proximity to a proof. Code, data, logs, repeated text, operational instructions, and generated presentation copy are excluded.

Argument map and routes

How the current approaches connect

Claims, reductions, open questions, active routes, and narrowed alternatives in one mathematical map.

Visible working map

Research route map

28 selected steps

Selected claims, active routes, useful failures, and open questions from the current research map. Arrows appear only for explicitly recorded relationships.

28 selected steps

Scroll horizontally to explore the route

Working route overview for Navier–Stokes Existence and SmoothnessA selected map of recorded claims, active routes, useful failures, open questions, and their explicit relationships. Search, filter, zoom, or pan within this page.All-data global existence and smoothness on ℝ³ — Depends on missing premiseAll-data global existenceand smoothness on ℝ³Conditional exact-core and profile chain — Depends on missing premiseConditional exact-core andprofile chainCorridor-generated active increment — Depends on missing premiseCorridor-generated activeincrementFinite-energy response promotion — Depends on missing premiseFinite-energy responsepromotionPositive-viscosity reservoir — Depends on missing premisePositive-viscosity reservoirBaseline EC gives a joint sink current, still compatible with a critical model — Depends on missing premiseBaseline EC gives a jointsink current, stillcompatible…Baseline exact-core assumptions — Depends on missing premiseBaseline exact-coreassumptionsBranch-II logarithmic invariant — Depends on missing premiseBranch-II logarithmicinvariantCanonical Euler profiles need the exact provider and positive retained defect — Depends on missing premiseCanonical Euler profilesneed the exact provider andpositive…Complete signed carrier on the correct two clocks — Depends on missing premiseComplete signed carrier onthe correct two clocksCritical moments and capacity retain sign and radius gaps — Depends on missing premiseCritical moments andcapacity retain sign andradius…Direct angular exact-core route without MP — Depends on missing premiseDirect angular exact-coreroute without MPDirect exact-core angular and carrier routes — activeDirect exact-core angularand carrier routesActual MP-derived neutral profiles — activeActual MP-derived neutralprofilesTemporal simplification and pressure order zero — activeTemporal simplification andpressure order zeroJoint value-current incompatibility at baseline EC scope — activeJoint value-currentincompatibility at baselineEC…S762 — stoppedS762V56-T01 / V56-C04 — stoppedV56-T01 / V56-C04V56-C04 / V54-C01 / V54-M01 — stoppedV56-C04 / V54-C01 / V54-M01Source-reported limitation — stoppedSource-reported limitationV46-A — OpenV46-AV46-B — OpenV46-BV46-C — OpenV46-CV46-D — OpenV46-DV46-E — OpenV46-EV46-F — OpenV46-FV46-G — OpenV46-GV49-H — OpenV49-H
Working claimActive routeOpen, active, or blocked questionUseful failure

Working overview, not proof. The map shows selected recorded relationships; more nodes or edges do not establish correctness or completion.

Active routeDirect exact-core angular and carrier routes

This route keeps the direct angular obstruction at EC-WEAK scope and the centered local carrier identity at baseline-EC scope. Neither requires MP. Angular rank two remains possible. The centered carrier has baseline windows T=L a^(−4/3), improved under EC-WEAK to T=L/a, with fixed-L endpoint error O(1/L) and no implicit interchange of limits. A vanishing complete signed interface mean on the appropriate clock would close that core, but the required depletion is open; absolute-value replacements lose the cancellation.

Route status · Active route
Active routeActual MP-derived neutral profiles

This route first needs the conditional MP construction of an actual canonical Euler profile with positive local defect. The source reports targeted MP checks rather than a full reconstruction. Compensated neutrality and rough rank deficiency do not automatically supply the regularity or conservation needed for rigidity, and a smooth special-case theorem does not close the rough profile route.

Route status · Active route
Active routeTemporal simplification and pressure order zero

The temporal route concerns the fixed core U's affine-L² variance: its lower bound uses the actual MP diagonal to contradict conservation of stationary retained profiles. The fixed-rank quantifiers remain essential; allowing rank to grow with T does not supply the requested simplification. The pressure route separately needs the additional pressure-time order-zero premise in the actual retained canonical frame and normalization. The logarithmic ceiling and fixed-rank estimates do not provide that premise or a simultaneous arbitrary-frame/rank theorem; no completed EC exclusion follows.

Route status · Active route
Active routeJoint value-current incompatibility at baseline EC scope

The joint value-current route starts from baseline EC without MP. Its prospective contradiction requires a PDE-specific annular estimate from the common origin of velocity, vorticity and pressure. Finite action, the no-atom result and the critical tail admit the recorded measure model, so those abstract estimates alone do not supply the missing bound.

Route status · Active route

Explored alternatives

Other routes

1 recorded
Narrowed routeSource-reported limitation

A moment-defined characteristic frequency by itself does not supply the Fourier-support hypothesis needed for wake decoupling. The retained architecture would need a production-bearing component with enough compactness and inherited growth to enter a narrow rigidity theorem, together with a reduction of collective multiplicity and a separate treatment of the zero-viscosity corridor.

Route status · Narrowed route

Route statements and reductions

Statements the next route can inspect and build on

Route statementConditional exact-core and profile chain

The source's conditional chain is EC-WEAK to the exact MP provider, then V49-T10 and an actual canonical neutral Euler profile with positive defect. The provider keeps the same retained sequence, frames, fields, pressure trace, carrier decomposition and limit order. Upstream extraction and closure of all remaining singularity branches are still separate requirements.

Source-reported route statement · dependencies incomplete
Route statementBaseline exact-core assumptions

EC assumes an eternal smooth canonical Biot–Savart velocity, exact vorticity passivity and elliptic stretching relation, complete volume-preserving flow, fixed nonzero finite enstrophy and the displayed Sobolev bounds. Its velocity lies in the stated Lorentz and bounded classes, not necessarily L2. Material vector distributions are invariant, but local deformation or covariance information is not a global anti-spray estimate.

Source-reported route statement · dependencies incomplete
Route statementDirect angular exact-core route without MP

The source reports direct angular covariance and modulation results under EC-WEAK, without MP. The angular lower bound is uniform in time and constant unit axes and leaves rank two possible. For the modulation result, recentering X is absolutely continuous, X(0)=0, and its long-time averaged |X′|² is bounded. The stressed mean identity retains both fluctuation stress R=avg(w⊗w) and drift stress S=avg(w⊗(X′−c)); the external steady zero-drift theorem does not establish that stressed identity.

Source-reported route statement · dependencies incomplete
Route statementComplete signed carrier on the correct two clocks

The source derives local weighted energy and centered carrier identities with the displayed cutoff and double-zero weights. Centering removes an acceleration contribution but does not give global L2 for h_a. A difference equal to an energy derivative is not instantaneous equality. The baseline clock T=L a^(-4/3) and weak clock T=L/a keep signed interfaces and fixed-L errors; taking absolute values loses cancellation.

Source-reported route statement · dependencies incomplete
Route statementFixed-core temporal complexity and separate Euler-profile conservation

For the fixed exact-core velocity U under EC-WEAK, the source defines temporal variance using its affine L² mean and finite velocity differences. Its upper bound is O(T); the positive order-T lower bound uses the actual MP diagonal as a contradiction argument. For each fixed rank N, the centered core error obeys c_N T ≤ E_N(s,T) ≤ CT/(N+1) for T ≥ T_N, uniformly in starting time; the lower bound again uses MP. Constants, thresholds, bands and shells can depend on fixed rank. Separately, canonical EP velocities with finite temporal span, or an exact rigid orbit under the stated global weak bounds and affine-L²/no-escape hypotheses, are conservative; these are not quantitative variance estimates for an arbitrary profile. The actual band-limited core translating-pattern statements keep their own scope. There is no growing-rank lower rate or simultaneous arbitrary-frame/rank theorem. The oscillating packet model fails self-induced passivity and stretch–diffusion.

Source-reported route statement · dependencies incomplete
Route statementCanonical Euler profiles need the exact provider and positive retained defect

Canonical weak Euler profiles need not have finite energy. Positive defect is an additional retained property of the exact common provider sequence. Smooth or geometrically restricted conservation results do not close arbitrary rough profiles. Full carrier decomposition, actual-cut commutators, pressure trace, caps, limit order and positive defect may not be replaced by auxiliary cuts, a generic weak limit or an assumed common center.

Source-reported route statement · dependencies incomplete
Route statementEvery rough conservation criterion keeps its extra hypothesis

The source records conservation under spatially constant axes, suitable actual VMO alignment with strong residual, or controlled actual projectors/gradients. Weak vorticity projectors and arbitrary pointwise kernels are insufficient. An actual positive-defect frame instead forces logarithmic oscillation on the specified tested scales. This supplies a lower bound, not the missing sublogarithmic upper estimate.

Source-reported route statement · dependencies incomplete
Route statementBaseline EC gives a joint sink current, still compatible with a critical model

At baseline EC scope, a joint subsequence gives source-reported measures m, C and J with a sink identity, finite action, the small-ball bound and reciprocal annular series. Double-zero and scale tests, not absence of an origin atom alone, remove derivative-delta terms. Pressure-weighted f_t is essential. The displayed critical measure model satisfies the current constraints; a stronger PDE-driven annular bound remains missing. MP is not a premise of this route.

Source-reported route statement · dependencies incomplete
Route statementPressure time derivative being a measure remains unresolved

The source uses a gauge-safe weak Euler class, localized pressure normalization and the stated order of Bernoulli and pressure cutoffs. The external bounded-velocity result is not automatically a weak-Lorentz theorem. Positive defect forces normalized pressure variation to diverge, with no supplied rate; a log-square ceiling does not make the time derivative a measure. V54-M01 blocks a purely local implication while retaining zero defect and failing global weak canonical hypotheses.

Source-reported route statement · dependencies incomplete

More ways to contribute

Open questions

Additional prepared tasks for exploring this research frontier.

20 featured tasks
01
V49-I

Adjudicate actual dissipative profiles after the exact MP provider, not an arbitrary Euler profile.

Suggested move: Adjudicate actual dissipative profiles after the exact MP provider, not an arbitrary Euler profile.
Ready to work on
02
V49-H

Use the direct angular exact-core route without silently adding MP as an assumption.

Suggested move: Use the direct angular exact-core route without silently adding MP as an assumption.
Ready to work on
03
V55-O

Obtain an o(T) approximation at one fixed finite rank or the exact excluded orbit class; rank growing with T does not suffice.

Suggested move: Obtain an o(T) approximation at one fixed finite rank or the exact excluded orbit class; rank growing with T does not suffice.
Ready to work on
04
V55-P

Use the common PDE origin of m, C and J to contradict their sink/reciprocal constraints, retaining pressure-weighted f_t; no MP assumption is needed.

Suggested move: Use the common PDE origin of m, C and J to contradict their sink/reciprocal constraints, retaining pressure-weighted f_t; no MP assumption is needed.
Ready to work on
05
V46-D

Prove rough neutral rigidity or conservation beyond the already conditional special cases.

Suggested move: Prove rough neutral rigidity or conservation beyond the already conditional special cases.
Ready to work on
06
V55-Q

Force vanishing of the complete signed centered interface along the stated clock and fixed-L sequence; h_a is not known to be globally L2.

Suggested move: Force vanishing of the complete signed centered interface along the stated clock and fixed-L sequence; h_a is not known to be globally L2.
Ready to work on
07
V46-F

Retain the stationary capacity question as a scope included by, but not closed by, the nonstationary V55-P route.

Suggested move: Retain the stationary capacity question as a scope included by, but not closed by, the nonstationary V55-P route.
Ready to work on
08
V55-N

Prove actual-frame sublogarithmic coarse direction oscillation or the stated stronger cubic-gradient bound on the tested radii.

Suggested move: Prove actual-frame sublogarithmic coarse direction oscillation or the stated stronger cubic-gradient bound on the tested radii.
Ready to work on
09
V53-L

Obtain an actual retained-profile pressure-time-derivative measure or uniform order-zero bound; logarithmic ceilings do not establish it.

Suggested move: Obtain an actual retained-profile pressure-time-derivative measure or uniform order-zero bound; logarithmic ceilings do not establish it.
Ready to work on
10
Select a production-bearing component from the corridor-generated response.Suggested move: Carry out Work Order NS-V6-B on the generated increment: split its energy into the bounded, subcritical, and critical branches, then prove joint time–space–frequency concentration or a quantified temporal multiplicity alternative.
Ready to work on
11
V53-M

Contradict persistent force or negative-power tails using dynamics, not amplitude laws alone.

Suggested move: Contradict persistent force or negative-power tails using dynamics, not amplitude laws alone.
Ready to work on
12
V46-C

Supply a nonreused physical cost across the missing radius.

Suggested move: Supply a nonreused physical cost across the missing radius.
Ready to work on
13
V46-A

Exhaust the upstream extraction or close every missing branch separately.

Suggested move: Exhaust the upstream extraction or close every missing branch separately.
Ready to work on
14
V46-B

Cancel the complete carrier, including low-time and mixed-tensor terms.

Suggested move: Cancel the complete carrier, including low-time and mixed-tensor terms.
Ready to work on
15
V51-J

Prove actual nonlinear local fractional-cofactor or force-tail regularity.

Suggested move: Prove actual nonlinear local fractional-cofactor or force-tail regularity.
Ready to work on
16
V46-G

Develop a genuinely different mathematical route when current additional-premise criteria do not close the target.

Suggested move: Develop a genuinely different mathematical route when current additional-premise criteria do not close the target.
Ready to work on
17
V46-E

Construct and control actual nested signed-corridor capacity; unsigned annular budgets do not suffice.

Suggested move: Construct and control actual nested signed-corridor capacity; unsigned annular budgets do not suffice.
Ready to work on
18
V51-K

Turn correctly scaled intrinsic motion into a physical nonreuse cost, not repeated normalized bounds.

Suggested move: Turn correctly scaled intrinsic motion into a physical nonreuse cost, not repeated normalized bounds.
Ready to work on
19
Unify spatial, frequency, and temporal production multiplicity.Suggested move: Construct a positive localized spacetime production measure, select bounded derivative-mass cylinders with a fixed measure share, and either obtain a finite-energy bubble or contradict the global energy and packet budgets.
Ready to work on
20
Rule out the narrow viscous or Euler profiles produced by the reduction.Suggested move: Prove rigidity only for the source-generated profile classes—including the required inherited equality or finite-interval enstrophy change—while testing steady fields, traveling fields, separated packets, derivative leakage, and coordinate normalization.
Ready to work on

Sourced mathematical context

The known mathematical landscape

Context collected Aug 7, 2026
Current statusOpen problem

Clay Mathematics Institute continues to label the problem Unsolved. Global Leray weak solutions, two-dimensional regularity, partial regularity, conditional continuation criteria, numerical scenarios, averaged-model blowup, and weak-solution nonuniqueness do not establish any of Fefferman's smooth-data global-regularity or breakdown alternatives.

[1][3]
External progress

What the literature has established

Selected external milestones in reverse chronological order, with their evidence posture.

  1. PreprintHou, Wang, and Yang claim a computer-assisted proof of nonuniqueness for unforced Leray–Hopf solutions. Their compactly supported L^2 initial datum is singular at the origin, and the checked source remains a preprint, so the result does not resolve a Clay smooth-data alternative.[10]
  2. Computational resultHou published high-resolution numerical evidence of potentially singular behavior in an axisymmetric scenario, explicitly as potential numerical evidence rather than a proof of singularity.[9]
  3. Peer reviewedAlbritton, Brué, and Colombo proved nonuniqueness of Leray solutions with the same forcing and zero initial data; forced weak nonuniqueness is distinct from Clay's smooth-solution alternatives.[8]
  4. Peer reviewedTao proved finite-time blowup for an averaged three-dimensional Navier–Stokes equation retaining energy cancellation, demonstrating a barrier to arguments based only on coarse energy structure rather than blowup for the true equation.[7]
12 cited sources7 related results or reductionsReferences

Mathematical neighborhood

Related results and reusable starting points

Current focusExistence and Smoothness of the Navier–Stokes Equation
Weaker or relaxed formGlobal Leray weak existence

Global Leray weak solutions exist in three dimensions, but weak existence permits insufficient regularity and does not supply the uniqueness or smoothness demanded by the target.

[4]
Solved special caseTwo-dimensional incompressible Navier–Stokes

The corresponding two-dimensional incompressible regularity problem is classically solved, but the proof does not control three-dimensional vortex stretching.

[3]
Dependency or reductionPartial regularity and critical continuation criteria

Partial-regularity and critical-norm criteria sharply constrain any singularity; proving the required critical control for all smooth initial data would rule out blowup, but that bound remains unavailable.

[5][6]
Related problemAveraged Navier–Stokes blowup model

Blowup in an averaged model shows that energy cancellation alone cannot prove regularity, but the averaged equation is not the original Navier–Stokes equation.

[7]
Related problemForced weak-solution nonuniqueness

Forced Leray-solution nonuniqueness concerns weak solutions and nonzero forcing, so it is a neighboring phenomenon rather than a smooth-data blowup or global-regularity result.

[8]
Related problemUnforced Leray–Hopf weak-solution nonuniqueness

The recent unforced Leray–Hopf nonuniqueness claim uses singular L^2 initial data and remains a computer-assisted preprint; it does not address the official smooth-data alternatives.

[10]
Related problemNumerical singularity scenarios

High-resolution numerical potentially singular scenarios can guide analysis, but finite numerical resolution neither proves blowup nor certifies global regularity.

[9]

Formal and computational footholds

Existing statements, libraries, computations, and datasets that can shorten the next serious attempt.

  • computation · not independently reproducedPotentially singular axisymmetric Navier–Stokes computation

    Published high-resolution computation supports a potentially singular scenario but is not a mathematical certificate and was not independently rerun for this collection.

    [9]
  • software · not independently reproducedHou–Wang–Yang weak-nonuniqueness code

    Public code accompanies the computer-assisted preprint on unforced Leray–Hopf weak nonuniqueness. ProofAtlas did not run it, and its singular-data weak-solution target is not the Clay statement.

    [10][11]
  • dataset · source linked; not reproduced by ProofAtlasJohns Hopkins Turbulence Databases

    Large direct-numerical-simulation datasets and query software support empirical turbulence study, but finite-resolution data do not certify global regularity or blowup.

    [12]

Formalization opportunities

Lean work can make these reusable foundations precise without being presented as a proof of the core problem.

  • Formalization targetA statement-aligned formalization of Fefferman's exact R^3 and periodic alternatives, including the official smoothness, decay, energy, pressure, and forcing hypotheses.
  • Formalization targetDistributions, weak derivatives, Bochner and Sobolev spaces, divergence-free vector fields, and nonlinear PDE solution concepts on R^3 and T^3.
  • Formalization targetLocal and global regularity, pressure reconstruction, energy inequalities, and checked continuation or blowup criteria.
  • Formalization targetA verified bridge distinguishing smooth classical solutions, suitable weak solutions, and Leray–Hopf solutions so neighboring nonuniqueness results cannot be mistaken for a Clay solution.

Later mathematical changes

What changed after the initial research map

Later recorded revisions that changed the mathematics, without inventing a date or an AI attribution.

Retain the v56 all-data Navier–Stokes frontier with distinct EC and MP-dependent routes, corrected affine/scaling/pressure scope, open source work and the preserved v6 history.Retain the v56 all-data Navier–Stokes frontier with distinct EC and MP-dependent routes, corrected affine/scaling/pressure scope, open source work and the preserved v6 history.

Changed the research frontierLater mathematical revision

Private recorded successor preparation; no public priority claim

The initial argument structure appears separately. Uploads, model runs, and presentation changes do not count as mathematical updates.

Research-record corrections

What changed in the research record

These notes describe corrections to cited passages, highlighted tasks, or connections between claims. The mathematical claims and their status did not change.

Research-record correctionWe corrected the cited passages. The mathematical claims and their status did not change.

Corrected the research recordCorrection note

Cited passages corrected
Research-record correctionWe corrected the cited passages. We removed a duplicate or outdated task or route step. We updated the highlighted open task or route. The mathematical claims and their status did not change.

Corrected the research recordCorrection note

Correction details
Research-record correctionWe corrected supporting details in the research record. The mathematical claims and their status did not change.

Corrected the research recordCorrection note

Correction details

The initial argument structure appears separately. Uploads, model runs, and presentation changes do not count as mathematical updates.

Detailed research inventory

Claims, milestones, and routes in the current map

This view highlights the mathematical statements most useful for following the current route.

21 standing statements2 proposed statements20 open questions1 narrowed routes
Statements by mathematical role23 selected mapped statements
  • lemma18 of 2318
  • reduction4 of 234
  • theorem candidate1 of 231
Selected mathematical clusters1 mathematical clusters
v56 recorded research frontierCurrent governing-source route and work inventory, with retained factual predecessors and open historical obligations. The full target remains unresolved.67 displayed rows · 5 routes included
  • retained route statementQuasi-record production selectionintermediate
  • retained route statementSupported wake decouplingintermediate
  • retained route statementBranch-II logarithmic invariantintermediate
  • retained route statementPositive-viscosity reservoirintermediate
  • retained route statementFinite-energy response promotionintermediate
  • retained route statementCorridor-generated active incrementintermediate
  • Useful failureSource-reported limitationreported failure
  • Research targetSelect a production-bearing component from the corridor-generated response.open
  • Research targetUnify spatial, frequency, and temporal production multiplicity.open
  • Research targetRule out the narrow viscous or Euler profiles produced by the reduction.open
  • retained route statementAll-data global existence and smoothness on ℝ³
  • retained route statementConditional exact-core and profile chainintermediate
  • retained route statementSupply a missing PDE estimate and exhaust upstream alternativesintermediate
  • retained route statementRetained v6 corridor facts and unresolved assemblyintermediate
  • retained route statementExact identities do not make the singularity alternatives exhaustiveintermediate
  • retained route statementBaseline exact-core assumptionsintermediate
  • retained route statementOrdinary weak endpoint survives the stronger tail exclusionsintermediate
  • retained route statementDirect angular exact-core route without MPintermediate
  • retained route statementComplete signed carrier on the correct two clocksintermediate
  • retained route statementCritical moments and capacity retain sign and radius gapsintermediate
  • retained route statementFinite-energy differences are not finite-energy velocityintermediate
  • retained route statementFixed-core temporal complexity and separate Euler-profile conservationintermediate
  • retained route statementCanonical Euler profiles need the exact provider and positive retained defectintermediate
  • retained route statementEvery rough conservation criterion keeps its extra hypothesisintermediate
  • retained route statementBaseline EC gives a joint sink current, still compatible with a critical modelintermediate
  • retained route statementLocal fractional cofactor regularity is an extra conservation premiseintermediate
  • retained route statementPressure time derivative being a measure remains unresolvedintermediate
  • Recorded relationshipA full-data proof needs exhaustive extraction from every possible singularity, closure of every resulting alternative, and continuation. The conditional EC-WEAK→MP→actual positive-defect-profile chain is one component; neither that chain nor its conditional endpoint estimates establish the missing exhaustion and supercritical closure.supports · reported by source
  • Recorded relationshipRetain the v6 quasi-record/superproduction premise at its own frequency and physical-budget scope when locating the inherited corridor. The v56 governing source keeps the upstream alternatives unclosed; this premise does not prove the existence of an exhaustive canonical EC extraction.supports · reported by source
  • Recorded relationshipRetain wake decoupling only for an actually Fourier-supported projected component. Moment-defined characteristic frequency is not that hypothesis; current upstream branch discussion does not erase the original support requirement.supports · reported by source
  • Recorded relationshipRetain the earlier branch-two logarithmic invariant at its displayed branch scope as context for the v56 upstream program. A branch-specific growth record does not close intermediate inefficiency, infrared transport, dispersed profiles or other explicitly retained alternatives.supports · reported by source
  • Recorded relationshipRetain the earlier positive-viscosity reservoir premise at its exact physical-scale and budget hypotheses. The later source still requires a physical nonreuse argument; repeated normalized estimates do not imply cumulative real expenditure.supports · reported by source
  • Recorded relationshipRetain the earlier finite-energy response-promotion statement only with its original finite-energy and response hypotheses. The current EC and outer-profile velocity classes need not be finite-energy, so that retained result cannot be applied merely from weak critical bounds.supports · reported by source
  • Recorded relationshipRetain the earlier corridor-generated increment at the stated corridor and parameter order. It remains context for one inherited route, not a replacement for exhaustive branch reduction or the actual signed cancellation/depletion estimate left open by v56.supports · reported by source
  • Recorded relationshipUnder the exact-core hypotheses, the source derives its low-amplitude obstruction and the complete fixed-cutoff carrier identity. Ordinary weak membership is an additional assumption for the two-sided critical-tail alternative; the carrier identity itself uses EC alone. Weak-critical and supercritical survivors remain uncontradicted, and its limits fix the cutoff before long-time averaging.supports · reported by source
  • Recorded relationshipThe direct angular obstruction requires EC-WEAK and its displayed low-frequency normalization, without an MP prerequisite. Its lower bound is uniform in time and constant unit axes; a new depletion estimate would contradict that bound, but rank two remains possible. The independent modulation statement also requires EC-WEAK and the specified absolutely continuous recentering with bounded averaged squared speed. Its mean identity retains fluctuation and drift stresses, which the external zero-drift input does not provide.supports · reported by source
  • Recorded relationshipStarting from EC, the source constructs a weighted local centered carrier with the required double zero. The retained identity must control the complete old carrier, its commutators and mixed tensors. The centered field need not lie in global L², so this construction does not replace the uncentered global value-current route.supports · reported by source
  • Recorded relationshipThe EC moment route distinguishes the fixed signed component h=e·f with zero-mean Hardy source e·g=−Δh from the scalar-magnitude signed Radon measure κ=−Δ|f|. The latter is the finite-mass strain contribution minus the angular/zero-set measure and may have a singular zero-set part; it is not an L¹ density. The combined scalar critical-moment obstruction forces at least one of these two contributions to have infinite critical moment, not both, and supplies neither a separately useful signed flux nor a productive physical radius. Returning these moment obstructions to actual productive radii remains an additional requirement.supports · reported by source
  • Recorded relationshipThe temporal variance and best fixed-rank approximation error are quantities of the fixed core U, centered in its affine L² space; no absolute finite velocity energy is assumed. Their quantitative lower bounds use the actual MP diagonal to obtain a stationary or finite-temporal-span canonical EP limit, whose conservation contradicts the retained residual drop. They are not variance bounds for an arbitrary positive-defect profile in an arbitrary frame. Rank-dependent constants and thresholds remain fixed before the long-window limit, with no growing-rank lower rate or simultaneous arbitrary-frame/rank optimization theorem.supports · reported by source
  • Recorded relationshipThe conditional EC-WEAK → MP step must supply one common actual-field subsequence with its pressure, traces, cap structure and defect measure. Positive local defect is an additional output of that actual construction. Its nested limits cannot be replaced by unrelated compactness extractions, and the source does not supply an unconditional profile construction.supports · reported by source
  • Recorded relationshipUnder baseline EC, the source defines a joint measure/current from the uncentered velocity on a common subsequence, with its sink and small-ball estimates. The dynamic identity must retain the pressure-weighted f_t term and the common double-zero/first-jet hypotheses. These identities neither require MP nor establish the missing PDE-specific annular bound.supports · reported by source
  • DerivationThe governing source separates partial or conditional routes from exhaustive target closure. The conjecture would require every displayed premise and every remaining branch to be discharged. This is an informal dependency record, not a verified derivation.proposed
  • Research targetV46-Aopen
  • Research targetV46-Bopen
  • Research targetV46-Copen
  • Research targetV46-Dopen
  • Research targetV46-Eopen
  • Research targetV46-Fopen
  • Research targetV46-Gopen
  • Research targetV49-Hopen
  • Research targetV49-Iopen
  • Research targetV51-Jopen
  • Research targetV51-Kopen
  • Research targetV53-Lopen
  • Research targetV53-Mopen
  • Research targetV55-Nopen
  • Research targetV55-Oopen
  • Research targetV55-Popen
  • Research targetV55-Qopen
  • Useful failureS762reported failure
  • Useful failureV56-T01 / V56-C04reported failure
  • Useful failureV56-C04 / V54-C01 / V54-M01reported failure
  • Narrowed routeSource-reported limitationA moment-defined characteristic frequency by itself does not supply the Fourier-support hypothesis needed for wake decoupling. The retained architecture would need a production-bearing component with enough compactness and inherited growth to enter a narrow rigidity theorem, together with a reduction of collective multiplicity and a separate treatment of the zero-viscosity corridor.
  • Active routeDirect exact-core angular and carrier routesThis route keeps the direct angular obstruction at EC-WEAK scope and the centered local carrier identity at baseline-EC scope. Neither requires MP. Angular rank two remains possible. The centered carrier has baseline windows T=L a^(−4/3), improved under EC-WEAK to T=L/a, with fixed-L endpoint error O(1/L) and no implicit interchange of limits. A vanishing complete signed interface mean on the appropriate clock would close that core, but the required depletion is open; absolute-value replacements lose the cancellation.
  • Active routeActual MP-derived neutral profilesThis route first needs the conditional MP construction of an actual canonical Euler profile with positive local defect. The source reports targeted MP checks rather than a full reconstruction. Compensated neutrality and rough rank deficiency do not automatically supply the regularity or conservation needed for rigidity, and a smooth special-case theorem does not close the rough profile route.
  • Active routeTemporal simplification and pressure order zeroThe temporal route concerns the fixed core U's affine-L² variance: its lower bound uses the actual MP diagonal to contradict conservation of stationary retained profiles. The fixed-rank quantifiers remain essential; allowing rank to grow with T does not supply the requested simplification. The pressure route separately needs the additional pressure-time order-zero premise in the actual retained canonical frame and normalization. The logarithmic ceiling and fixed-rank estimates do not provide that premise or a simultaneous arbitrary-frame/rank theorem; no completed EC exclusion follows.
  • Active routeJoint value-current incompatibility at baseline EC scopeThe joint value-current route starts from baseline EC without MP. Its prospective contradiction requires a PDE-specific annular estimate from the common origin of velocity, vorticity and pressure. Finite action, the no-atom result and the critical tail admit the recorded measure model, so those abstract estimates alone do not supply the missing bound.
How to interpret these counts

A statement may be a lemma, conditional reduction, special case, documented limitation, or open target. These counts describe the work's structure; they do not estimate distance to a proof.

Research outlook

Conditions that would advance the current route

Priority open bridgeAdjudicate actual dissipative profiles after the exact MP provider, not an arbitrary Euler profile.

1 approach has already been tested and narrowed. The task above is the current priority within the larger open route.

Evidence needed nextConcrete conditions for progress

A result can change the outlook by closing the bridge, narrowing its scope, or showing that the route cannot work.

  • Supply the missing mathematical implication with all stated source hypotheses and retained boundary cases.
  • Retain exact evidence for an independent source-fidelity and mathematical review; a model, calculation or branch-only result does not complete the full target.

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Research contextPrepared context for any AI agent

Does viscosity keep every permitted smooth three-dimensional incompressible flow smooth for all future time? The current source studies constraints on a hypothetical breakdown through conditional exact-core and neutral Euler profiles. It reports useful carrier, variance and value-current restrictions, while keeping their assumptions separate. A missing PDE estimate and an exhaustive transfer from arbitrary initial data to all relevant alternatives still prevent a proof of the full problem.

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Sources and references12 cited works · next context review by Nov 7, 2026

The mathematical context was checked on Aug 7, 2026. Status can be refreshed sooner after a material result or claim.

  1. 1
    Navier-Stokes Equationmaintained problem list · Clay Mathematics Institute · Clay Mathematics Institute · accessed Aug 7, 2026
  2. 2
    The Millennium Prize Problemsmaintained problem list · Clay Mathematics Institute · Clay Mathematics Institute · accessed Aug 7, 2026
  3. 3
    Existence and Smoothness of the Navier–Stokes Equationoriginal source · Charles L. Fefferman · Clay Mathematics Institute · 2006 · accessed Aug 7, 2026
  4. 4
    Sur le mouvement d’un liquide visqueux emplissant l’espacepeer reviewed result · Jean Leray · Acta Mathematica · 1934 · DOI 10.1007/BF02547354 · accessed Aug 7, 2026
  5. 5
    Partial regularity of suitable weak solutions of the Navier-Stokes equationspeer reviewed result · Luis Caffarelli, Robert Kohn, Louis Nirenberg · Communications on Pure and Applied Mathematics · 1982 · DOI 10.1002/cpa.3160350604 · accessed Aug 7, 2026
  6. 6
    L3,∞-solutions of Navier–Stokes equations and backward uniquenesspeer reviewed result · Luis Escauriaza, Gregory Seregin, Vladimír Šverák · Russian Mathematical Surveys · 2003 · DOI 10.1070/RM2003v058n02ABEH000609 · accessed Aug 7, 2026
  7. 7
    Finite time blowup for an averaged three-dimensional Navier–Stokes equationpeer reviewed result · Terence Tao · Journal of the American Mathematical Society · 2016 · DOI 10.1090/jams/838 · accessed Aug 7, 2026
  8. 8
    Non-uniqueness of Leray solutions of the forced Navier-Stokes equationspeer reviewed result · Dallas Albritton, Elia Brué, Maria Colombo · Annals of Mathematics · 2022 · DOI 10.4007/annals.2022.196.1.3 · accessed Aug 7, 2026
  9. 9
    Potentially Singular Behavior of the 3D Navier–Stokes Equationspeer reviewed result · Thomas Y. Hou · Foundations of Computational Mathematics · 2023 · DOI 10.1007/s10208-022-09578-4 · accessed Aug 7, 2026
  10. 10
    Nonuniqueness of Leray-Hopf solutions to the unforced incompressible 3D Navier-Stokes Equationpreprint · Thomas Hou, Yixuan Wang, Changhe Yang · arXiv · 2025; revised 2026 · ARXIV 2509.25116 · accessed Aug 7, 2026
  11. 11
    Code for 3D Navier–Stokes nonuniquenesssoftware or dataset · Hou Group · GitHub · accessed Aug 7, 2026
  12. 12
    Johns Hopkins Turbulence Databasessoftware or dataset · Johns Hopkins University · Johns Hopkins University · accessed Aug 7, 2026

Important qualifications

  • The Navier–Stokes literature is enormous; this record selects statement-shaping milestones rather than attempting completeness.
  • The target is Fefferman's Clay formulation for three-dimensional incompressible flow on R^3 or the three-torus, not every Navier–Stokes model or solution concept.
  • Recent manuscripts claiming full resolution outside authoritative review were not treated as status evidence.
  • The Hou–Wang–Yang weak-nonuniqueness result remains at preprint posture and was not independently reproduced.
  • Negative formalization findings reflect a scoped search and are not proofs of nonexistence.
  • No packet source or submitted mathematical claim was read or used as authority.

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