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The spacetime Penrose inequality with charge and original-data rigidity
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Abstract
Under the stated energy, decay, and trapping hypotheses, we prove the sharp charged spacetime Penrose upper-area inequality for one-ended three-dimensional initial data with source-free electric and magnetic fields. The theorem allows arbitrary second fundamental form, nonzero ADM momentum, and disconnected boundary. Writing m for invariant ADM mass, Q for total charge magnitude, and rA for the minimum-enclosing-area radius, the bound is m ≥ Q and $r_A\le m+\sqrt{m^2-Q^2}$. The polynomial mass bound $m\ge(r_A+Q^2/r_A)/2$ is asserted only when $r_A\gt Q$. When m > Q, equality under the stated connected, outermost, outer-area-minimizing future-horizon hypotheses identifies the original data as a smooth spacelike slice of dyonic Reissner–Nordström, including smooth attachment at the future horizon.
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Collected automatically by AI tools (Claude Opus 5.5 and GPT-6 Astra, 2026-10-23) and not checked by a person. May be wrong or incomplete. Report an error.
Comments and discussion
- Hubert Bray, Tuan Dolmen, Marcus Khuri and David Schmidt, Proof of the Penrose Conjecture for Maximally Parameterized Initial Data Sets, Appendix C (arXiv:2610.20559v1, 2026-10-14). Appendix C discusses checking OpenAI's Penrose series. [family-level]
- UnstableReserves (@UnstableReserve), post on X (2026-10-13). Summarizes this paper's charged inequality, with equality "only for a single Reissner–Nordström hole", and reports the poster's own exact two-hole computations ("watch the common horizon pinch off"), with gap asymptotics described as derived but not proved.
Formalization
- OpenAI, Spacetime Penrose inequalities: enclosing area, charge, rotation, and anti-de Sitter extensions — Lean scope (release scope documentation, 2026). The family's only formalization covers the end-replacement construction and the Schwarzschild equality examples of the companion CKS/Bondi paper; this paper's charged inequality and rigidity theorem are not formalized. [family-level]
Possibly relevant literature (found by the agent, not checked)
- T. Dolmen, The Penrose inequality with charge for 2-convex initial data sets (arXiv:2607.29447, 31 Jul 2026). Proves a sharp charged Penrose inequality for Einstein–Maxwell data under Dong's 2-convexity condition and a connected outermost horizon with area at least 4πq², with Reissner–Nordström rigidity; this corresponds to this paper's charged upper-area bound and dyonic Reissner–Nordström rigidity under different hypotheses.
- E. Ng, The suboptimal Penrose inequality for charged initial data sets (arXiv:2609.22418, 18 Sep 2026). Proves a charged Penrose-type bound with a non-sharp constant for three-dimensional Einstein–Maxwell data with zero magnetic field, a non-sharp counterpart of this paper's main inequality.
News and blogs
- Carlos Toledo, OpenAI's math release: what it claims beyond what it checks (audit, 2026-10-10). Finding G3 distinguishes family 260's supporting Lean results from its headline inequalities. [family-level]
Elsewhere
- VibeMathed: Problem record
- Emergent Mind: family 260
Independent sites; their content is not reviewed here.
Cite
@misc{OAI:The-spacetime-Penrose-inequality-with-charge-and-original-data-rigidity-October-5-2026,
author = {{OpenAI}},
title = {{The spacetime Penrose inequality with charge and original-data rigidity}},
howpublished = {OpenAI Math Release preprint
\href{https://github.com/openai/math/blob/main/preprints/The-spacetime-Penrose-inequality-with-charge-and-original-data-rigidity-October-5-2026/paper.pdf}{OAI:The-spacetime-Penrose-inequality-with-charge-and-original-data-rigidity-October-5-2026}},
year = {2026}
}Lean formalization
OpenAI provides Lean files for this family: lean/docs/260.md. The Lean statements have not been checked by people against the paper's claims.
Family 260: 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.
Other papers in this family:
- A Charged Reduction of the Spacetime Penrose Inequality in Spatial Dimensions at Least Four · October 5, 2026
- Spacetime Penrose inequalities: enclosing area, charge, and rigidity · October 5, 2026
- The Kerr–Newman Penrose Inequality for Axisymmetric Electrovacuum Exteriors · October 5, 2026
- Electromagnetic tails and the Kerr–Newman Penrose inequality · October 5, 2026
- The nonmaximal anti-de Sitter Penrose Inequality and original-data rigidity · October 5, 2026
- The Penrose inequality for maximal asymptotically hyperbolic initial data · October 5, 2026
- A local Penrose inequality for conformal perturbations of Schwarzschild–anti-de Sitter data · October 5, 2026
- The spacetime Penrose inequality and enclosing area · September 27, 2026
- Conformal flow and the Riemannian Penrose inequality with minimizing frontiers · September 27, 2026
- Equality and rigidity in the spacetime Penrose inequality · September 27, 2026
- Boundary graph deformations for the spacetime Penrose inequality · September 27, 2026
- Area-controlled end replacement and the Bondi Penrose inequality in the CKS class · September 27, 2026