A Proposal for a Covariant Entropy Relation

A density-dependent conformal killing vector (CKV) field is attained from a conformally transformed action composed of a unique constraint and a Klein-Gordon field. The CKV is re-expressed into an information identity and studied in its integro-differential form for both null and time-like geodesics...

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description A density-dependent conformal killing vector (CKV) field is attained from a conformally transformed action composed of a unique constraint and a Klein-Gordon field. The CKV is re-expressed into an information identity and studied in its integro-differential form for both null and time-like geodesics. It is conjectured that the identity corresponds to a generalized second law of thermodynamics which holographically relates the covariant entropy contained within a volumetric \(n\)- and \((n-1)\)-form, starting from an \((n-2)\)-spatial area. The time-like geodesics inherit an effective `geometric spin' while the null geodesics are suggested to obey the generalized covariant entropy bound so long as they conform to Einstein's equation of state. To then comply with the equation of state, a metriplectic system is introduced, whereby a newly defined energy functional is derived for the entropy. Such an entropy functional mediates the Casimir invariants of the Hamiltonian and therefore preserves the symplectic form of quantum mechanics. For null geodesics, the Poisson bracket of the entropy functional with the Hamiltonian is shown to elegantly result in Einstein's energy-mass relation.
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The CKV is re-expressed into an information identity and studied in its integro-differential form for both null and time-like geodesics. It is conjectured that the identity corresponds to a generalized second law of thermodynamics which holographically relates the covariant entropy contained within a volumetric \(n\)- and \((n-1)\)-form, starting from an \((n-2)\)-spatial area. The time-like geodesics inherit an effective `geometric spin' while the null geodesics are suggested to obey the generalized covariant entropy bound so long as they conform to Einstein's equation of state. To then comply with the equation of state, a metriplectic system is introduced, whereby a newly defined energy functional is derived for the entropy. Such an entropy functional mediates the Casimir invariants of the Hamiltonian and therefore preserves the symplectic form of quantum mechanics. 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subjects Einstein equations
Entropy
Equations of state
Geodesy
Quantum mechanics
Thermodynamics
title A Proposal for a Covariant Entropy Relation
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