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.
Counterexample: the proper-time integrand of a spacelike curve is not real
Statement refuted
False claim: the formula assigns an elapsed clock time to every regular curve of the model.
The claim is refuted by a straight spacelike line: its tangent is spacelike at every point, so is negative and the square root is not a real number. A spacelike interval is not elapsed clock time; the geometric spacing along the curve is its spacelike length, a different quantity.
Facts & Assumptions
Given: An event , a spacelike vector and the straight curve , in the oriented time-oriented affine Minkowski model.
Causal classification (Timelike, null, spacelike and causal vectors of a Lorentz vector space): is spacelike when and timelike when .
Inertial charts (Inertial frames and inertial charts of the affine Minkowski model): in an inertial chart the matrix of is , so for one has .
Curves (Curves, regular causal curves and future timelike worldlines in affine Minkowski space): the curve has constant tangent and is a future timelike worldline only when is future timelike.
Proper time (Proper time along a future timelike worldline): the proper-time integrand is and the construction is restricted to future timelike worldlines; for a spacelike tangent the quantity is negative.
Counterexample
In an inertial chart with let : then , so is spacelike by [L1].
The curve has constant tangent by [L3], so at every point; the integrand of [L4] is the square root of a negative real number and is not defined. The proper-time construction therefore produces no real value on this curve.
The geometric spacing along the curve is governed by the spacelike length per unit parameter, , not by a clock reading: this curve is not a timelike worldline, has no causal-character tangent that is timelike, and the failure is exactly the hypothesis of the timelike restriction in [L4].
Remarks
- Spacelike length and proper time are different constructions. The number measures a spatial separation in the model; times it is not an elapsed time along the curve, and no clock is associated with a spacelike displacement by this framework.
Depends on
Curves, regular causal curves and future timelike worldlines in affine Minkowski space
Proper time along a future timelike worldline
Timelike, null, spacelike and causal vectors of a Lorentz vector space
Inertial frames and inertial charts of the affine Minkowski model
Lorentz forms of inertia (3,1,0) on a 4-dimensional real vector space