On the origin of the cosmological constant

dc.creatorYokoyama, Jun'ichi
dc.date2002-04-08
dc.date.accessioned2026-07-07T03:26:47Z
dc.date.available2026-07-07T03:26:47Z
dc.descriptionUnder the assumption that the cosmological constant vanishes in the true ground state with lowest possible energy density, we argue that the observed small but finite vacuum-like energy density can be explained if we consider a theory with two or more degenerate perturbative vacua, which are unstable due to quantum tunneling, and if we still live in one of such states. An example is given making use of the topological vacua in non-Abelian gauge theories.
dc.description5 pages. To be published in the Proc. 11th JGRG ed. by K. Maeda et al
dc.identifierhttps://arxiv.org/abs/gr-qc/0204033
dc.identifierhttp://arxiv.org/abs/gr-qc/0204033
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/34186
dc.subjectGeneral Relativity and Quantum Cosmology
dc.titleOn the origin of the cosmological constant
dc.typetext

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