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: a past-directed parametrization of a timelike line is not a worldline
Statement refuted
False claim: if a curve parametrizes a straight timelike line, then it is a future timelike worldline of the model and the proper-time construction gives the clock reading of its history.
The claim is refuted by orienting the parametrization backwards: the same geometric line with the opposite parametrization has past timelike tangents, is not a worldline of the model, and yet the proper-time integrand takes exactly the same values as for the future-directed parametrization. This is why the parametrization, and not merely the image of the curve, is part of the definition of a worldline.
Facts & Assumptions
Given: A future timelike displacement and an event , and the two parametrizations and , , of the same straight timelike segment; .
Causal classification (Timelike, null, spacelike and causal vectors of a Lorentz vector space): is timelike when ; the sign of does not distinguish future from past.
Time orientation (Time orientation, future and past timelike/null/causal vectors, and the closed cones): the timelike set is the disjoint union of the future component and the past component , and a timelike vector is future or past but not both; whenever .
Worldlines (Curves, regular causal curves and future timelike worldlines in affine Minkowski space): a future timelike worldline is a curve whose tangent at every parameter value is future timelike; the parametrization is part of the curve.
Proper time (Proper time along a future timelike worldline): the proper-time integrand is , which depends on the tangent through the quadratic form only.
Counterexample
In an inertial chart with let : then , so is timelike, and choosing in the future component makes it a future timelike displacement; then belongs to by [L2].
The curve on has difference quotients identically , so is past timelike for every ; by [L3] the curve is not a future timelike worldline of the model, The curve for has tangent , is a future timelike worldline and has exactly the same image, since is a bijection of .
The proper-time integrand of both curves agrees pointwise: by bilinearity of , so the proper-time integral alone does not distinguish the future-directed from the past-directed parametrization: by [L4] the proper-time construction is attached to the parametrized history, together with its future timelike hypothesis, and not to the bare image of the curve.
Remarks
- Orientation is data, not geometry of the image. The same set of events carries two opposite worldline parametrizations with identical proper-time densities; only the future-directed one is a worldline of the model, and the past-directed one is its orientation reversal.
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
Time orientation, future and past timelike/null/causal vectors, and the closed cones
Lorentz forms of inertia (3,1,0) on a 4-dimensional real vector space