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DoT: The Duality of Time Postulate

And Its Consequences on General Relativity and Quantum Mechanics

Mohamed Haj Yousef

7.7. Vacuum energy and the cosmological term

The original distinction between void and vacuum can be retained with precise meanings. Void denotes the absence of an already specified spatial or material background in the ontology. A physical vacuum is a state of a defined theory with observables and correlations. Calling that vacuum a superfluid requires a dynamical order parameter and physical response properties; homogeneity or indistinguishability alone does not establish superfluidity.

In a finite regulated field model, zero-point mode energies contribute schematically as

ρE=1V∑kℏωk2,\rho_E=\frac1V\sum_k\frac{\hbar\omega_k}{2},

(7.9)

before the appropriate renormalization and gravitational interpretation. Producing the terms in an inner sequence does not change a Hamiltonian sum into an average. Dividing by the number of modes changes the observable unless the model supplies a physical rule requiring that normalization. A mode count also depends on the volume and regulator; a quantity proportional to ℓ−3\ell^{-3} is a number density, not a dimensionless count.

The earlier proposed suppression by 117 orders of magnitude is therefore not retained as a demonstrated solution. The problem is to derive the gravitating vacuum contribution consistently, including its response to matter and changes of scale. For vacuum energy density ρE\rho_E with vacuum equation of state, the usual dictionary is

Λvac=8πGc4ρE,\Lambda_{\mathrm{vac}}=\frac{8\pi G}{c^4}\rho_E,

(7.10)

with the total observed cosmological term also depending on the chosen bare or renormalized gravitational parameters.

There is a useful obstruction. Replacing a nongravitational Hamiltonian by H+E*IdH+E_*\mathrm{Id} leaves density-matrix evolution unchanged, since [Id,ρ]=0[\mathrm{Id},\rho]=0. Thus those normalized observables cannot select the absolute energy offset. Once a vacuum energy density gravitates, that offset matters. A successful completion theory must supply the gravitational information missing from a reconstruction based solely on normalized quantum dynamics.

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