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.
Observer energy, spatial momentum and mass shell of a boosted test body
Example
Keep the setting of The relative-velocity decomposition of a boost, checked in an explicit tetrad: the flat metric on , the tetrad , the observer , the parameters , , , and the future unit timelike vector with and . Let and set
Then is future timelike, its rest mass is , and relative to the observer its energy and spatial momentum are
so that and the mass shell holds. This is the standard boosted test-body kinematics in the abstract observer split.
Facts & Assumptions
Given: The flat metric and tetrad of the boosted-frame example, the observer , parameters , the vector , a mass , and the vector .
is future unit timelike, , , and with (The relative-velocity decomposition of a boost, checked in an explicit tetrad).
For the observer energy and spatial momentum are and ; for the rest mass is , and if then satisfies (Observer-relative energy, spatial momentum and rest mass of a tangent vector).
If is future timelike with rest mass , then with and one has , , and (Positivity, relative-velocity identities and the mass shell of observer-relative energy and momentum).
For the nonnegative square root satisfies and (Rational powers of a positive base).
Verification
Since by [L1], we get , so ; by [L4] and [L2] the rest mass is . In particular is future timelike and .
By [L2] and [L1], because ; and .
Using and , we compute , which is the mass shell relation of [L3]; equivalently . The energy is positive because .
Remarks
The example computes the same numbers as the elementary boost formula in an inertial frame, but only through the observer split of a single tetrad: the energy and momentum are vector and scalar data in and its dual, not coordinate components. No measurement or empirical claim is made; the physical reading of and belongs to the framework's units and postulates.
Depends on
Dependency tree · 2 levels
Sources
- S. M. Carroll, Lecture Notes on General Relativity, arXiv:gr-qc/9712019v1 (1997), Ch. 1 on four-momentum, energy and the mass shell, printed pp. 26-28 (PDF pp. 33-35)
- H. S. Reall, Part III General Relativity (Cambridge, October 12, 2022 revision), section 6.3, equations (6.17)-(6.19) on P = m u, g(P,P) = -m^2 and observer energy, printed pp. 63-65 (PDF pp. 64-66)