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Hopkins' chromatic splitting conjecture (weak and odd-prime strong forms)

Fix a prime pp, let Ln−1L_{n-1} be localization at E(n−1)E(n-1) and LK(n)L_{K(n)} localization at Morava KK-theory. Hopkins' chromatic splitting conjecture, recorded by Hovey (1995, Conjecture 4.2), describes the chromatic overlap Ln−1LK(n)Sp∧L_{n-1}L_{K(n)}S_p^\wedge. Its weak form asserts that for the pp-completion XX of a finite spectrum the canonical map Ln−1X→Ln−1LK(n)XL_{n-1}X\to L_{n-1}L_{K(n)}X has a homotopy retraction (finite-input form: Beaudry-Goerss-Henn, Conjecture 1.1.11). Its strong form prescribes an explicit splitting of Ln−1LK(n)Sp∧L_{n-1}L_{K(n)}S_p^\wedge into suspended localized spheres indexed by an exterior algebra; Beaudry disproved this at n=p=2n=p=2, and Barthel-Beaudry (2019, Conjecture 6.3) retain it at odd primes. Both forms were known through height two at odd primes. Does the canonical map split for all nn and pp, and does the overlap decompose as predicted at odd primes?

Result
Disproved(see note)
Status
Candidate (review pending)
AI contribution
AI-discovered
Method
Argument
Field
Stable homotopy theory: chromatic homotopy
Posed by
M. J. Hopkins, recorded by M. Hovey, Bousfield localization functors and Hopkins' chromatic splitting conjecture (1995), Conjecture 4.2; refined by Barthel-Beaudry (2019) and Beaudry-Goerss-Henn
Year posed
1995
Years open
31y
Solved
2026-09-27
Model
Unreleased internal OpenAI model
Vendor
OpenAI
Collaborators
—
Verification
Unreviewed
Publication
Announced
Collection
OpenAI math release (October 2026), version adc7f12
Significance
40 / 100
Disclosed cost
—
Wikipedia
No dedicated article

What was actually shown

Weak form: for the derived pp-completion X=Sp∧X=S_p^\wedge, the canonical map Ln−1X→Ln−1LK(n)XL_{n-1}X\to L_{n-1}L_{K(n)}X has no homotopy retraction at height n=pn=p for every p≥5p\ge5 and at n=p+1n=p+1 for every p≥7p\ge7; the class β1(p−1)2\beta_1^{(p-1)^2} is a nonzero kernel element (at p=5p=5, β116\beta_1^{16} in degree 608). Strong form: for p≥5p\ge5 the map L0LK(3)S→L0LK(2)LK(3)SL_0L_{K(3)}S\to L_0L_{K(2)}L_{K(3)}S is nonzero on π−3\pi_{-3}, so the height-three splitting fails even as an equivalence of E(2)E(2)-local spectra. Companions: at n=p=3n=p=3 the overlap is not in the thick subcategory generated by L0S,L1S,L2SL_0S,L_1S,L_2S; positively, for p>n+1p>n+1 the overlap has a 2n2^n-stage filtration with the predicted cofibers (nonsplit), with explicit attachments at height three. Heights below p−1p-1 remain open.

What the AI did

The OpenAI math release (github.com/openai/math, commit adc7f12) states that its results were produced by an unreleased internal OpenAI model under one fixed procedure, averaging about three hours of ChatGPT Pro thinking compute per result. This result is not among the README's stated exceptions (the Re(s) > 11/12 zero-free region write-up and the Hodge conjecture for CM abelian varieties). The manuscript is credited to OpenAI alone and names no human author. The family has five manuscripts dated 25 and 27 September 2026: two counterexample papers, one negative finite-assembly result, and two positive filtration results. The rational-obstruction manuscript ships a small exact-arithmetic support script whose coverage note says it checks only Chevalley-Eilenberg matrix arithmetic, not the main theorem.

Verification

No independent mathematician has checked this yet. Checked here: the abstracts, introductions and main theorems of the TeX sources of all five manuscripts, read against Hovey's Conjecture 4.2 and the Barthel-Beaudry and Beaudry-Goerss-Henn formulations they cite; the proofs were not refereed. The weak-splitting counterexamples (principal manuscript) use the derived p-completion of the sphere, i.e. finite input, as the conjecture requires; they rely on the Hopkins-Miller computation recorded by Heard and on Devinatz-Hopkins nilpotence. The strong-form disproof at height three uses the solid Lubin-Tate theory of Barthel, Mann, Ray, Schlank, Senger, Weinstein and Zhou (cited as 2026). The disproofs cover specific ranges of p and n only; the weak form at heights below p - 1 and at small primes is not addressed. No Lean formalization is supplied for this family.

Sources

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