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Perturbations of ultralight vector field dark matter

dc.contributor.authorRuiz Cembranos, José Alberto
dc.contributor.authorLópez Maroto, Antonio
dc.contributor.authorNuñez Jareño, Santos José
dc.date.accessioned2023-06-17T22:02:47Z
dc.date.available2023-06-17T22:02:47Z
dc.date.issued2017-02-13
dc.description© The Authors. This work has been supported by the MINECO (Spain) projects FIS2014-52837-P, FPA2014-53375-C2-1-P, and Consolider-Ingenio MULTIDARK CSD2009-00064.
dc.description.abstractWe study the dynamics of cosmological perturbations in models of dark matter based on ultralight coherent vector fields. Very much as for scalar field dark matter, we find two different regimes in the evolution: for modes with k^(2) « Hma, we have a particle-like behaviour indistinguishable from cold dark matter, whereas for modes with k^(2) » Hma, we get a wave-like behaviour in which the sound speed is non-vanishing and of order c^(2)_(s) ∼ k^(2)/m^(2)a^(2) . This implies that, also in these models, structure formation could be suppressed on small scales. However, unlike the scalar case, the fact that the background evolution contains a non-vanishing homogeneous vector field implies that, in general, the evolution of the three kinds of perturbations (scalar, vector and tensor) can no longer be decoupled at the linear level. More specifically, in the particle regime, the three types of perturbations are actually decoupled, whereas in the wave regime, the three vector field perturbations generate one scalar-tensor and two vector-tensor perturbations in the metric. Also in the wave regime, we find that a non-vanishing anisotropic stress is present in the perturbed energy-momentum tensor giving rise to a gravitational slip of order (Φ − Ψ)/Φ ∼ c^(2)_(s). Moreover in this regime the amplitude of the tensor to scalar ratio of the scalar-tensor modes is also h/Φ ∼ c^(2)_(s). This implies that small-scale density perturbations are necessarily associated to the presence of gravity waves in this model. We compare their spectrum with the sensitivity of present and future gravity waves detectors.
dc.description.departmentDepto. de Física Teórica
dc.description.facultyFac. de Ciencias Físicas
dc.description.refereedTRUE
dc.description.sponsorshipMinisterio de Economía y Competitividad (MINECO)
dc.description.sponsorshipConsolider-Ingenio
dc.description.statuspub
dc.eprint.idhttps://eprints.ucm.es/id/eprint/44082
dc.identifier.doi10.1007/JHEP02(2017)064
dc.identifier.issn1029-8479
dc.identifier.officialurlhttp://dx.doi.org/10.1007/JHEP02(2017)064
dc.identifier.relatedurlhttps://link.springer.com
dc.identifier.urihttps://hdl.handle.net/20.500.14352/17979
dc.issue.number2
dc.journal.titleJournal of high energy physics
dc.language.isoeng
dc.publisherSpringer
dc.relation.projectIDFIS2014-52837-P
dc.relation.projectIDFPA2014-53375-C2-1-P
dc.relation.projectIDCSD2009-00064
dc.rightsAtribución 3.0 España
dc.rights.accessRightsopen access
dc.rights.urihttps://creativecommons.org/licenses/by/3.0/es/
dc.subject.cdu53
dc.subject.keywordTime phase-transition
dc.subject.keywordScalar-field
dc.subject.keywordGalactic halos
dc.subject.keywordGalaxy haloes
dc.subject.keywordBose-liquid
dc.subject.keywordUniverse
dc.subject.keywordCores.
dc.subject.ucmFísica-Modelos matemáticos
dc.titlePerturbations of ultralight vector field dark matter
dc.typejournal article
dspace.entity.typePublication
relation.isAuthorOfPublicationc5a4cc87-ceba-494d-95ab-d54b9b1a35e3
relation.isAuthorOfPublicatione14691a1-d3b0-47b7-96d5-24d645534471
relation.isAuthorOfPublication.latestForDiscoveryc5a4cc87-ceba-494d-95ab-d54b9b1a35e3

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