Generalized Scale Invariant Gravity

dc.creatorLin, Shih-Yuin
dc.creatorNg, Kin-Wang
dc.date1997-08-20
dc.date.accessioned2026-07-07T04:23:33Z
dc.date.available2026-07-07T04:23:33Z
dc.descriptionWe generalize the scale invariant gravity by allowing a negative kinetic energy term for the classical scalar field. This gives birth to a new scalar-tensor theory of gravity, in which the scalar field is in fact an auxiliary field. For a pure gravity theory without matter, the scale symmetric phase represents an equivalent class of gravity theories, which the Einstein gravity plus a cosmological constant belongs to under a special gauge choice. The one-loop quantum correction of the theory is calculated by using the Vilkovisky-DeWitt's method. We find that the scale symmetry is broken dynamically, and that the Einstein gravity is the ground state of the broken phase. We also briefly discuss the consequent cosmological implications. It is shown that the time-delay experiment restricts the present universe to be very close to the ground state.
dc.description14 pages, REVTeX, no figure
dc.identifierhttps://arxiv.org/abs/hep-th/9708101
dc.identifierhttp://arxiv.org/abs/hep-th/9708101
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/55071
dc.subjectHigh Energy Physics - Theory
dc.subjectGeneral Relativity and Quantum Cosmology
dc.titleGeneralized Scale Invariant Gravity
dc.typetext

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