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.
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These labels describe origin, not correctness: citations and verification chips remain separate evidence.
Energy-condition verdicts for dust, radiation and the cosmological effective fluid
Pointwise algebraic reading of the four energy conditions for prescribed perfect-fluid models in a rest frame, including the effective fluid associated with a cosmological parameter in the adopted field law. No dynamics, no solution of any field equation, no measurement and no claim about nature is asserted; the example records the inequalities alone.
Example
Adopt a perfect-fluid model in the classical framework (The perfect-fluid matter model: rest energy density, pressure, four-velocity and stress-energy) with derived stress-energy tensor , and use the rest-frame equivalences of Consistency conditions of the adopted field law: conservation, trace, parameter variation and the energy conditions of a perfect fluid clause (f): at a point with rest frame , , the four conditions of The pointwise energy conditions WEC, NEC, DEC and SEC read
Then:
- Dust (, ): WEC, NEC, DEC and SEC all hold.
- Radiation (, ): WEC, NEC, DEC and SEC all hold.
- Positive cosmological effective fluid (, , as for the term with in Adopted Einstein field equation in the direct-equation presentation): WEC, NEC and DEC hold (with equality in the non-strict inequalities) and SEC fails.
- Negative cosmological effective fluid (, , ): WEC and DEC fail, NEC holds with equality and SEC holds. Together with clause 3, this shows that WEC and SEC are incomparable by implication.
Facts & Assumptions
Given: A perfect-fluid model with rest energy density and pressure , and the four equivalences displayed above.
The rest-frame equivalences for the four conditions are the equivalences of Consistency conditions of the adopted field law: conservation, trace, parameter variation and the energy conditions of a perfect fluid clause (f), derived there from the tensor form .
The stress-energy tensor of the field-law term has the perfect-fluid form with and : with (Adopted Einstein field equation in the direct-equation presentation clause (i), The perfect-fluid matter model: rest energy density, pressure, four-velocity and stress-energy, SI unit and coordinate conventions of the classical gravitational framework).
Verification
(Dust and radiation.) By [L1] the four conditions are read off from the displayed inequalities. For and : , , and , so all four right-hand sides hold. For and : , , , and , so all four hold. These are clauses 1 and 2.
(Positive effective fluid.) By [L1] and [L2], let , . Then and : WEC holds; : NEC holds; : DEC holds; but , so SEC fails. This is clause 3.
(Negative effective fluid.) By [L1] and [L2], let , . Then fails, so WEC fails; fails (an inequality with is false), so DEC fails; , so NEC holds; and together with gives SEC. This is clause 4 and shows that SEC need not imply WEC or DEC. Clause 3 shows that WEC need not imply SEC, so WEC and SEC are incomparable. These examples are consistent with the implications DEC WEC NEC and SEC NEC proved in The pointwise energy conditions WEC, NEC, DEC and SEC.
Remarks
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Not a solution claim. The verdicts concern the pointwise inequalities for prescribed values of and ; they do not assert that the corresponding fluid model solves the field equation or that the cosmological parameter has either sign.
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Convention dependence. The equivalences use the strict-timelike convention of The pointwise energy conditions WEC, NEC, DEC and SEC; the proof obtains boundary inequalities by limits of timelike vectors, using continuity of this tensor.
Depends on
Consistency conditions of the adopted field law: conservation, trace, parameter variation and the energy conditions of a perfect fluid
The pointwise energy conditions WEC, NEC, DEC and SEC
The perfect-fluid matter model: rest energy density, pressure, four-velocity and stress-energy
Adopted Einstein field equation in the direct-equation presentation
SI unit and coordinate conventions of the classical gravitational framework
Smooth time-oriented Lorentzian four-manifolds: the geometric objects of the model
The inverse metric, musical isomorphisms and index raising
Dependency tree · 2 levels
Sources
- D. Tong, General Relativity (Cambridge Part III Mathematical Tripos, Michaelmas 2019), section 4.5.7: the perfect-fluid energy conditions and the cosmological-constant case, printed pp. 194-198 (PDF pp. 201-205)
- S. M. Carroll, Lecture Notes on General Relativity, arXiv:gr-qc/9712019v1 (1997), Ch. 4: the Weak Energy Condition and the perfect-fluid specialization, printed pp. 117-118 (PDF pp. 124-125)