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dc.contributor.authorNesseris, S.en
dc.contributor.authorPerivolaropoulos, L.en
dc.date.accessioned2015-11-24T18:28:34Z-
dc.date.available2015-11-24T18:28:34Z-
dc.identifier.issn1550-7998-
dc.identifier.urihttps://olympias.lib.uoi.gr/jspui/handle/123456789/16157-
dc.rightsDefault Licence-
dc.subjecthigh-redshift supernovaeen
dc.subjecthubble-space-telescopeen
dc.subjectcosmic background imageren
dc.subjectprobe wmap observationsen
dc.subjectequation-of-stateen
dc.subjectdark energyen
dc.subjectaccelerating universeen
dc.subjectconstraintsen
dc.subjectanisotropyen
dc.subjectexpansionen
dc.titleFate of bound systems in phantom and quintessence cosmologiesen
heal.typejournalArticle-
heal.type.enJournal articleen
heal.type.elΆρθρο Περιοδικούel
heal.identifier.primaryDoi 10.1103/Physrevd.70.123529-
heal.identifier.secondary<Go to ISI>://000226054800046-
heal.identifier.secondaryhttp://prd.aps.org/abstract/PRD/v70/i12/e123529-
heal.languageen-
heal.accesscampus-
heal.recordProviderΠανεπιστήμιο Ιωαννίνων. Σχολή Επιστημών και Τεχνολογιών. Τμήμα Βιολογικών Εφαρμογών και Τεχνολογιώνel
heal.publicationDate2004-
heal.abstractWe study analytically and numerically the evolution of bound systems in universes with accelerating expansion where the acceleration either increases with time towards a Big Rip singularity (phantom cosmologies) or decreases with time (quintessence). We confirm the finding of Caldwell [R. R. Caldwell, M. Kamionkowski and N. N. Weinberg, Phys. Rev. Lett. 91, 071301 (2003).] that bound structures get dissociated in phantom cosmologies but we demonstrate that this happens earlier than anticipated in Ref. [R. R. Caldwell, M. Kamionkowski and N. N. Weinberg, Phys. Rev. Lett. 91, 071301 (2003).]. In particular we find that the "rip time" when a bound system gets unbounded is not the time when the repulsive phantom energy gravitational potential due to the average (rho+3p) balances the attractive gravitational potential of the mass M of the system. Instead, the "rip time" is the time when the minimum of the time-dependent effective potential (including the centrifugal term) disappears. For the Milky Way galaxy this happens approximately 180 Myrs before the Big Rip singularity instead of approximately 60 Myrs indicated in [R. R. Caldwell, M. Kamionkowski and N. N. Weinberg, Phys. Rev. Lett. 91, 071301 (2003).] for a phantom cosmology with w=-1.5. A numerical reconstruction of the dissociating bound orbits is presented.en
heal.journalNamePhysical Review Den
heal.journalTypepeer reviewed-
heal.fullTextAvailabilityTRUE-
Appears in Collections:Άρθρα σε επιστημονικά περιοδικά ( Ανοικτά)

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