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dc.contributor.authorPérez, Isabel
dc.contributor.authorAguerri, J. A. L.
dc.contributor.authorMéndez-Abreu, J.
dc.date.accessioned2013-10-15T09:16:15Z
dc.date.available2013-10-15T09:16:15Z
dc.date.issued2012
dc.identifier.citationPérez, I.; Aguerri, J.A.L.; Méndez-Abreu, J. Bar pattern speed evolution over the las 7 Gyr. Astronomy and Astrophysics, 540: A103 (2012). [http://hdl.handle.net/10481/28431]es_ES
dc.identifier.issn0004-6361
dc.identifier.issn1432-0746
dc.identifier.otherarXiv:1202.1929v1
dc.identifier.urihttp://hdl.handle.net/10481/28431
dc.description.abstractContext. The tumbling pattern of a bar is the main parameter characterising its dynamics. From numerical simulations, its evolution since bar formation is tightly linked to the dark halo in which the bar is formed through dynamical friction and angular momentum exchange. Observational measurements of the bar pattern speed with redshift can restrict models of galaxy formation and bar evolution.es_ES
dc.description.abstractAims. We aim to determine for the first time the bar pattern speed evolution with redshift based on morphological measurements.es_ES
dc.description.abstractMethods. We have selected a sample of 44 low-inclination ringed galaxies from the SDSS and COSMOS surveys covering the redshift range 0 < z < 0.8 to investigate the evolution of the bar pattern speed. We derived morphological ratios between the deprojected outer ring radius (Rring) and the bar size (Rbar). This quantity is related to the parameter ℛ = RCR/Rbar used for classifiying bars in slow and fast rotators, and allows us to investigate possible differences with redshift.es_ES
dc.description.abstractResults. We obtain a similar distribution of R at all redshifts. We do not find any systematic effect that could be forcing this result.es_ES
dc.description.abstractConclusions. The results obtained here are compatible with the main bulk of the bar population (~70%) being fast-rotators and with no evolution of the pattern speed with redshift. We argue that if bars are long-lasting structures, the results presented here imply that there has not been a substantial angular momentum exchange between the bar and halo, as predicted by numerical simulations. In consequence, this might imply that the discs of these high surface-brightness galaxies are maximal.es_ES
dc.description.sponsorshipI.P. was supported by the Spanish Ministry of Science and Innovation (MICINN) (via grants AYA2010-21322-C03-02, AYA2010-21322-C03-03, AYA2007-67625-C02-02 and Consolider-Ingenio CSD2010-00064) and by the Junta de Andalucía (FQM-108). J.A.L.A. and J.M.A. were supported by the projects AYA2010-21887-C04-04 and by the Consolider-Ingenio 2010 Program grant CSD2006-00070.es_ES
dc.language.isoenges_ES
dc.publisherEuropean Southern Observatory (ESO); Springer Verlages_ES
dc.rightsCreative Commons Attribution-NonCommercial-NoDerivs 3.0 Licensees_ES
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/3.0/es_ES
dc.subjectGalaxies es_ES
dc.subjectHigh redshiftes_ES
dc.subjectEvolution es_ES
dc.subjectStructurees_ES
dc.subjectKinematics and dynamicses_ES
dc.titleBar pattern speed evolution over the las 7 Gyres_ES
dc.typeinfo:eu-repo/semantics/preprintes_ES
dc.rights.accessRightsinfo:eu-repo/semantics/openAccesses_ES
dc.identifier.doi10.1051/0004-6361/201118396es_ES


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