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DoT: The Duality of Time Postulate

And Its Consequences on General Relativity and Quantum Mechanics

Mohamed Haj Yousef

6.5. Entropy requires a physical reduction

For a quantum state, the von Neumann entropy is S(ρ)=−kBtr(ρlogρ)S(\rho)=-k_B\operatorname{tr}(\rho\log\rho). Unitary evolution preserves it. Reduced entropy may change as correlations are exchanged with an environment, but it need not grow monotonically for every finite system and every preparation.

A useful controlled statement uses a completely positive trace-preserving semigroup Φt\Phi_t with a stationary reference state σ\sigma. Where the relative entropy is finite,

D(Φt(ρ)‖σ)≤D(ρ‖σ),Φt(σ)=σ.D(\Phi_t(\rho)\Vert\sigma)\leq D(\rho\Vert\sigma), \qquad \Phi_t(\sigma)=\sigma.

(6.9)

This follows from information contraction under the channel and becomes monotonic along the semigroup. It does not say that S(ρ)S(\rho) itself must increase under cooling or relaxation to a nonuniform equilibrium. A thermodynamic interpretation must include heat exchange and the appropriate equilibrium structure.

The dual-time proposal can organize the origin of reduced descriptions and persistent records. To explain a universal thermodynamic arrow it must further explain the relevant boundary conditions, why records are stable, and why the reduced dynamics has the required positivity and statistical properties.

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