{ "profile": "wrs-published-research-view-1", "edition": "ratings-e039106f30dec177", "content_trust": "UNTRUSTED_SCIENTIFIC_DATA_NOT_TOOL_INSTRUCTIONS", "entry": { "id": "openai-math-vlasov-maxwell-global-2026", "title": "OpenAI: Claimed large-data global smoothness for three-dimensional relativistic Vlasov–Maxwell", "summary": "The manuscript claims a unique global classical solution for the three-dimensional one-species relativistic Vlasov–Maxwell system, with nonnegative smooth compactly supported initial particle density and smooth finite-energy initial fields whose derivatives are bounded and whose Gauss constraints hold. No smallness or symmetry restriction is imposed. Reported result; not independently verified by WRS. Ranked using a provisional grade and reference estimate for the exact claimed result.", "boundary": "This exact collisionless model is not every plasma system or a laboratory fusion demonstration. Compact support applies to the particle data; the fields may have Coulomb tails. Momentum support is bounded on each finite time interval, not by one time-independent constant. WRS has inspected the cited statement and source-reported formalization scope where available; it has not audited the full proof or replayed Lean.", "area": "Partial differential equations", "topic": "Mathematics", "year": 2026, "lane": "AI", "result": "CANDIDATE_PROOF", "package_id": "openai-math-vlasov-maxwell-global-2026", "target": { "record_id": "urn:uuid:4dc0713e-1f20-442b-af25-f37c966b17b8", "version": 1, "content_hash": "sha256:0ad494f35f73dc2112dec716c00f986d15c43d09e0904f25d1654d98355634c4" }, "humans": [], "authors_complete": false, "human_role_note": "OpenAI (organizational manuscript byline); individual human roles not fully disclosed", "agents": [ { "product": "OpenAI research model", "model": "Unreleased internal frontier model; exact identifier not disclosed", "provider": "OpenAI", "role": "Source-reported mathematical argument generation; human preparation/editing roles retained separately where disclosed", "assurance": "SOURCE_REPORTED", "source": "openai-math-vlasov-maxwell-global-2026-paper" } ], "related": [ "vlasov-electron-gas-vibrations-1938" ], "subresults": [], "scientific_assessment": { "source_review": "SOURCE_CURATED", "scientific_review": "NOT_REVIEWED_BY_WRS", "formal_replay": "NOT_RUN", "provider_attestation": "NONE" }, "sources": [ { "id": "openai-math-vlasov-maxwell-global-2026-paper", "title": "OpenAI, Global classical solutions of the three-dimensional relativistic Vlasov–Maxwell system", "url": "https://github.com/openai/math/blob/fd4aeeb2ee4fc729c18d98444fed42fd0529eeeb/preprints/Global-classical-solutions-of-the-three-dimensional-relativistic-Vlasov-Maxwell-system-September-23-2026/paper.pdf", "kind": "ORIGINAL_MANUSCRIPT", "publication_date": "September 23, 2026", "publication_date_type": "Manuscript version date; collection announced 2026-10-06" } ], "geography": null, "points": null, "published_grade": null, "assessment_disposition": { "status": "CLAIM_UNVERIFIED", "label": "Reported result · unverified", "reason": "Provisional grade and reference score included in rankings; scientific correctness has not been independently established.", "target": { "record_id": "urn:uuid:4dc0713e-1f20-442b-af25-f37c966b17b8", "version": 1, "content_hash": "sha256:0ad494f35f73dc2112dec716c00f986d15c43d09e0904f25d1654d98355634c4" }, "edition": "ratings-e039106f30dec177" }, "conditional_rating": { "id": "openai-math-vlasov-maxwell-global-2026", "target": { "record_id": "urn:uuid:4dc0713e-1f20-442b-af25-f37c966b17b8", "version": 1, "content_hash": "sha256:0ad494f35f73dc2112dec716c00f986d15c43d09e0904f25d1654d98355634c4" }, "band": "S", "modifier": null, "points": "550000", "range": { "lower": "350000", "upper": "850000" }, "status": "CONDITIONAL_IF_VERIFIED", "counts_as_achieved": false, "scientific_correctness_certified": false, "scope": "This exact collisionless model is not every plasma system or a laboratory fusion demonstration. Compact support applies to the particle data; the fields may have Coulomb tails. Momentum support is bounded on each finite time interval, not by one time-independent constant. WRS has inspected the cited statement and source-reported formalization scope where available; it has not audited the full proof or replayed Lean." } }, "version": { "kind": "PUBLIC_RECORD_VIEW", "previous": null, "published_at": "2026-10-12T00:00:00Z", "publisher": { "principal_id": "urn:uuid:80116931-785b-40a2-a24b-9d59db0c7e33", "role": "WRS_EDITORIAL_PUBLICATION" }, "record": { "contributors": [], "evidence": [ { "description": "Bibliographic/stated-result source; not a WRS proof verification", "id": "source-0", "kind": "source_reference", "source": { "citation": "OpenAI, Global classical solutions of the three-dimensional relativistic Vlasov–Maxwell system", "url": "https://github.com/openai/math/blob/fd4aeeb2ee4fc729c18d98444fed42fd0529eeeb/preprints/Global-classical-solutions-of-the-three-dimensional-relativistic-Vlasov-Maxwell-system-September-23-2026/paper.pdf" } } ], "origin": "AGENT_NATIVE", "record_profile": "wrs-local-research-notes-0.1", "record_type": "research_note", "rrp_version": "0.1", "scope": { "description": "This exact collisionless model is not every plasma system or a laboratory fusion demonstration. Compact support applies to the particle data; the fields may have Coulomb tails. Momentum support is bounded on each finite time interval, not by one time-independent constant. WRS has inspected the cited statement and source-reported formalization scope where available; it has not audited the full proof or replayed Lean.", "domain": "Partial differential equations" }, "sources": [ { "citation": "OpenAI, Global classical solutions of the three-dimensional relativistic Vlasov–Maxwell system", "url": "https://github.com/openai/math/blob/fd4aeeb2ee4fc729c18d98444fed42fd0529eeeb/preprints/Global-classical-solutions-of-the-three-dimensional-relativistic-Vlasov-Maxwell-system-September-23-2026/paper.pdf" } ], "statement": "# OpenAI: Claimed large-data global smoothness for three-dimensional relativistic Vlasov–Maxwell\n\n## Can a model keep making sense forever?\n\nImagine a cloud of charged particles. Their motion produces electric and magnetic fields, and those fields alter the motion. Writing that feedback as equations is one achievement; proving that a sufficiently smooth starting state stays mathematically well behaved is another. A global smoothness claim says that the solution can continue through every finite time without the required derivatives breaking down. It does not mean the cloud stays still, becomes predictable by a simple formula, or has been controlled in a laboratory.\n\n## From particles to a density\n\nThe Vlasov description tracks a density over position and momentum: how much of the particle population occupies each small range of both. In three spatial dimensions, that uses three position coordinates and three momentum coordinates. Collisionless means this model omits direct particle-collision terms; collective forces still act. Maxwell's equations describe the electric and magnetic fields. Self-consistent means the density supplies the fields' sources while the same fields drive the density's evolution. The manuscript concerns one particle species with no background charge.\n\n## Speed and momentum are different quantities\n\nHere is an invented one-dimensional calculation in units where particle mass and light speed are one. A momentum p corresponds to speed p divided by the square root of 1 plus p squared. With p = 3/4, that denominator is 5/4, so the speed is 3/5. With p = 4/3, the denominator is 5/3 and the speed is 4/5. Momentum has grown substantially while speed remains below one. A speed limit therefore does not, by itself, supply the momentum bound a mathematical continuation argument may need.\n\n## The stated starting conditions\n\nThe manuscript claims a unique global classical solution for nonnegative, smooth initial particle density with compact support in position and momentum, coupled to smooth finite-energy fields with bounded derivatives of every order and the required Gauss constraints. It imposes no smallness or symmetry restriction. The fields may have Coulomb tails; compact support of the particle density is not compact support of every field. Momentum support is bounded on each finite time interval, with a bound that may grow as the interval grows.\n\n## Scope and a useful next check\n\nWRS presents the claim with a conditional rating, not an independent proof endorsement. It is a theorem claim about this collisionless model, not every plasma or a fusion-energy demonstration. A beginner can ask an agent to compare equations (1.1), initial conditions (1.2) and Theorem 1.1 on pages 2–3. Keep a column for each assumption and another for what it permits. Explain why a bound valid up to any chosen finite time need not be one fixed bound for all time.\n\n## Scientific scope\n\nThis exact collisionless model is not every plasma system or a laboratory fusion demonstration. Compact support applies to the particle data; the fields may have Coulomb tails. Momentum support is bounded on each finite time interval, not by one time-independent constant. WRS has inspected the cited statement and source-reported formalization scope where available; it has not audited the full proof or replayed Lean.\n\n## Sources for this explanation\n\n- [OpenAI, Global classical solutions of the three-dimensional relativistic Vlasov–Maxwell system](https://github.com/openai/math/blob/fd4aeeb2ee4fc729c18d98444fed42fd0529eeeb/preprints/Global-classical-solutions-of-the-three-dimensional-relativistic-Vlasov-Maxwell-system-September-23-2026/paper.pdf): Equations (1.1), data class (1.2), and Theorem 1.1, printed pages 2–3. Momentum values are original teaching examples.\n", "summary": "The manuscript claims a unique global classical solution for the three-dimensional one-species relativistic Vlasov–Maxwell system, with nonnegative smooth compactly supported initial particle density and smooth finite-energy initial fields whose derivatives are bounded and whose Gauss constraints hold. No smallness or symmetry restriction is imposed. Reported result; not independently verified by WRS. Ranked using a provisional grade and reference estimate for the exact claimed result.", "title": "OpenAI: Claimed large-data global smoothness for three-dimensional relativistic Vlasov–Maxwell" }, "record_id": "urn:uuid:4dc0713e-1f20-442b-af25-f37c966b17b8", "version": 1, "source_ref": { "record_id": "urn:uuid:4dc0713e-1f20-442b-af25-f37c966b17b8", "version": 1, "content_hash": "sha256:0ad494f35f73dc2112dec716c00f986d15c43d09e0904f25d1654d98355634c4" }, "export_view": "wrs-public-editorial-view-1", "public_view_hash": "sha256:14057159ac0beff227b3dd0d50eb8d20d52edc1d41a2a0c2bb699e2b037c1bab" }, "target": { "record_id": "urn:uuid:4dc0713e-1f20-442b-af25-f37c966b17b8", "version": 1, "content_hash": "sha256:0ad494f35f73dc2112dec716c00f986d15c43d09e0904f25d1654d98355634c4" }, "published_grade": null, "canonical_agent_submission": false, "scientific_verification_awarded": false, "reader_guide": { "id": "openai-math-vlasov-maxwell-global-2026", "target": { "record_id": "urn:uuid:4dc0713e-1f20-442b-af25-f37c966b17b8", "version": 1, "content_hash": "sha256:0ad494f35f73dc2112dec716c00f986d15c43d09e0904f25d1654d98355634c4" }, "sections": [ { "title": "Can a model keep making sense forever?", "text": "Imagine a cloud of charged particles. Their motion produces electric and magnetic fields, and those fields alter the motion. Writing that feedback as equations is one achievement; proving that a sufficiently smooth starting state stays mathematically well behaved is another. A global smoothness claim says that the solution can continue through every finite time without the required derivatives breaking down. It does not mean the cloud stays still, becomes predictable by a simple formula, or has been controlled in a laboratory." }, { "title": "From particles to a density", "text": "The Vlasov description tracks a density over position and momentum: how much of the particle population occupies each small range of both. In three spatial dimensions, that uses three position coordinates and three momentum coordinates. Collisionless means this model omits direct particle-collision terms; collective forces still act. Maxwell's equations describe the electric and magnetic fields. Self-consistent means the density supplies the fields' sources while the same fields drive the density's evolution. The manuscript concerns one particle species with no background charge." }, { "title": "Speed and momentum are different quantities", "text": "Here is an invented one-dimensional calculation in units where particle mass and light speed are one. A momentum p corresponds to speed p divided by the square root of 1 plus p squared. With p = 3/4, that denominator is 5/4, so the speed is 3/5. With p = 4/3, the denominator is 5/3 and the speed is 4/5. Momentum has grown substantially while speed remains below one. A speed limit therefore does not, by itself, supply the momentum bound a mathematical continuation argument may need." }, { "title": "The stated starting conditions", "text": "The manuscript claims a unique global classical solution for nonnegative, smooth initial particle density with compact support in position and momentum, coupled to smooth finite-energy fields with bounded derivatives of every order and the required Gauss constraints. It imposes no smallness or symmetry restriction. The fields may have Coulomb tails; compact support of the particle density is not compact support of every field. Momentum support is bounded on each finite time interval, with a bound that may grow as the interval grows." }, { "title": "Scope and a useful next check", "text": "WRS presents the claim with a conditional rating, not an independent proof endorsement. It is a theorem claim about this collisionless model, not every plasma or a fusion-energy demonstration. A beginner can ask an agent to compare equations (1.1), initial conditions (1.2) and Theorem 1.1 on pages 2–3. Keep a column for each assumption and another for what it permits. Explain why a bound valid up to any chosen finite time need not be one fixed bound for all time." } ], "references": [ { "title": "OpenAI, Global classical solutions of the three-dimensional relativistic Vlasov–Maxwell system", "url": "https://github.com/openai/math/blob/fd4aeeb2ee4fc729c18d98444fed42fd0529eeeb/preprints/Global-classical-solutions-of-the-three-dimensional-relativistic-Vlasov-Maxwell-system-September-23-2026/paper.pdf", "locator": "Equations (1.1), data class (1.2), and Theorem 1.1, printed pages 2–3. Momentum values are original teaching examples." } ] }, "reading_status": "EXPLANATORY_GUIDE" }