Equation 144 · The Entry a Relabeling Cannot Write
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The resemblance between this picture and the ledger built above is real, and so is the point where it stops. Mapped: both settings share one logical shape, that a globally conserved charge requires the generator of the relevant symmetry to be exactly present in the description doing the accounting, and that reporting a nonzero “defect” in its absence is meaningful only once that absence is named precisely — a missing bath Hamiltonian in one case, a missing timelike Killing vector in the other. Unmapped, and this is the load-bearing distinction: is a choice. A laboratory observer decides to stop tracking a bath, and a different observer, tracking more of it, gets a smaller or zero…
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The resemblance between this picture and the ledger built above is real, and so is the point where it stops. Mapped: both settings share one logical shape, that a globally conserved charge requires the generator of the relevant symmetry to be exactly present in the description doing the accounting, and that reporting a nonzero “defect” in its absence is meaningful only once that absence is named precisely — a missing bath Hamiltonian in one case, a missing timelike Killing vector in the other. Unmapped, and this is the load-bearing distinction: is a choice. A laboratory observer decides to stop tracking a bath, and a different observer, tracking more of it, gets a smaller or zero defect for the identical physical situation, exactly as the uncorrelated-bath limit above showed. The absence of a timelike Killing vector in an FLRW spacetime is not a choice available to any observer; it is a geometric fact about the manifold that no relabeling, no decision about which degrees of freedom to track, and no more generous coarse-graining channel can restore. Nothing in this article’s formalism plays the role of a “finer channel” that would recover a photon’s redshifted energy the way tracing further into a bath recovers a qubit’s swapped excitation, and claiming otherwise would be exactly the overreach this construction was built to refuse. The two pictures share a family resemblance in their grammar and nothing more: no shared Hilbert space, no shared mechanism, and no attempt here to unify them into one formalism.
Sources cited in the article section
- [7] Quasi-Local Energy-Momentum and Angular Momentum in General Relativity ↗
- [5] Covariant Conservation Laws in General Relativity ↗
- [15] General Relativity ↗
- [3] Republication of: The Dynamics of General Relativity ↗
- [6] A New Proof of the Positive Energy Theorem ↗
These citations give research context. Read each source to check which claims it supports.