Abstract
In standard physics quantum field theory is based on a flat vacuum space-time. This quantum field theory predicts a nonzero cosmological constant. Hence the gravitational field equations do not admit a flat vacuum space-time. This dilemma is resolved using the units covariant gravitational field equations. This paper shows that the field equations admit a flat vacuum space-time with nonzero cosmological constant if and only if the canonical LNH is valid. This allows an interpretation of the LNH phenomena in terms of a time-dependent vacuum state. If this is correct then the cosmological constant must be positive.
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NAS-NRC Senior Research Associate 1981–1983.
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Adams, P.J. Large numbers hypothesis. IV. The cosmological constant and quantum physics. Int J Theor Phys 22, 461–467 (1983). https://doi.org/10.1007/BF02083289
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DOI: https://doi.org/10.1007/BF02083289