How statement and proof provenance work
The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.
- Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
- AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
- AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.
These labels describe origin, not correctness: citations and verification chips remain separate evidence.
Fixed softening does not guarantee finite extensive free energy
Statement refuted
Fix . For each box , let , let be its canonical partition function, and set . The per-particle free-energy density is (in joules), and the per-volume free-energy density is (in joules per cubic metre). Here a “finite extensive free-energy density” means that the chosen normalized sequence has a finite real thermodynamic-limit value. The claim refuted is that a fixed positive softening length guarantees such a finite limit for every sequence of unscaled self-gravitating boxes whose volumes are bounded above and below by positive multiples of . The counterexample below has both and .
Facts & Assumptions
Given: The softened Newtonian pair potential with fixed and the growing-box hypotheses in Point collapse and unscaled gravity nonextensivity.
For boxes containing a fixed positive-volume cube, the softened unscaled model has along the concentration sequence, so its free energy per particle tends to . (Point collapse and unscaled gravity nonextensivity)
Counterexample
Fix , take , and set for every integer . Then , , and , so this is a bounded-box sequence satisfying the softened concentration hypotheses in [F1].
Clause 2 of [F1] gives , hence . Since , also . Neither normalization has a finite real thermodynamic-limit value along this sequence, contradicting the claimed guarantee.