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The dark side of curvature

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The dark side of curvature

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dc.contributor.author Barenboim Szuchman, Gabriela Alejandra
dc.contributor.author Fernández Martínez, Enrique
dc.contributor.author Mena Requejo, Olga
dc.contributor.author Verde, Licia
dc.date.accessioned 2014-09-11T08:25:41Z
dc.date.available 2014-09-11T08:25:41Z
dc.date.issued 2010
dc.identifier.citation Barenboim Szuchman, Gabriela Alejandra Fernández Martínez, Enrique Mena Requejo, Olga Verde, Licia 2010 The dark side of curvature Journal Of Cosmology And Astroparticle Physics 1003 8
dc.identifier.uri http://hdl.handle.net/10550/37732
dc.description.abstract Geometrical tests such as the combination of the Hubble parameter H(z) and the angular diameter distance d_A(z) can, in principle, break the degeneracy between the dark energy equation of state parameter w(z), and the spatial curvature Omega_k in a direct, model-independent way. In practice, constraints on these quantities achievable from realistic experiments, such as those to be provided by Baryon Acoustic Oscillation (BAO) galaxy surveys in combination with CMB data, can resolve the cosmic confusion between the dark energy equation of state parameter and curvature only statistically and within a parameterized model for w(z). Combining measurements of both H(z) and d_A(z) up to sufficiently high redshifts around z = 2 and employing a parameterization of the redshift evolution of the dark energy equation of state are the keys to resolve the w(z)-Omega_k degeneracy.
dc.language.iso eng
dc.relation.ispartof Journal Of Cosmology And Astroparticle Physics, 2010, vol. 1003, p. 8
dc.title The dark side of curvature
dc.type journal article es_ES
dc.date.updated 2014-09-11T08:25:41Z
dc.identifier.doi 10.1088/1475-7516/2010/03/008
dc.identifier.idgrec 061869
dc.rights.accessRights open access es_ES

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