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dc.contributor.authorDíaz Rivero, Ana
dc.contributor.authorDvorkin, Cora
dc.contributor.authorCyr-Racine, Francis-Yan
dc.contributor.authorZavala, Jesús
dc.contributor.authorVogelsberger, Mark
dc.date.accessioned2018-11-20T21:43:01Z
dc.date.available2018-11-20T21:43:01Z
dc.date.issued2018-11
dc.date.submitted2018-09
dc.identifier.issn2470-0010
dc.identifier.issn2470-0029
dc.identifier.urihttp://hdl.handle.net/1721.1/119245
dc.description.abstractStrong gravitational lensing has been identified as a promising astrophysical probe to study the particle nature of dark matter. In this paper we present a detailed study of the power spectrum of the projected mass density (convergence) field of substructure in a Milky Way-sized halo. This power spectrum has been suggested as a key observable that can be extracted from strongly-lensed images and yield important clues about the matter distribution within the lens galaxy. We use two different N-body simulations from the ETHOS framework: one with cold dark matter and another with self-interacting dark matter and a cutoff in the initial power spectrum. Despite earlier works that identified k≳100  kpc[superscript -1] as the most promising scales to learn about the particle nature of dark matter we find that even at lower wave numbers—which are actually within reach of observations in the near future—we can gain important information about dark matter. Comparing the amplitude and slope of the power spectrum on scales 0.1≲k/kpc[subscript -1]≲10 from lenses at different redshifts can help us distinguish between cold dark matter and other exotic dark matter scenarios that alter the abundance and central densities of subhalos. Furthermore, by considering the contribution of different mass bins to the power spectrum we find that subhalos in the mass range 10[superscript 7]-10[superscript 8]  M[subscript ⊙] are on average the largest contributors to the power spectrum signal on scales 2≲k/kpc[superscript -1]≲15, despite the numerous subhalos with masses >10[superscript 8]  M[subscript ⊙] in a typical lens galaxy. Finally, by comparing the power spectra obtained from the subhalo catalogs to those from the particle data in the simulation snapshots we find that the seemingly-too-simple halo model is in fact a fairly good approximation to the much more complex array of substructure in the lens.en_US
dc.description.sponsorshipAlfred P. Sloan Foundationen_US
dc.description.sponsorshipUnited States. National Aeronautics and Space Administration (ATP Grant NNX17AG29G)en_US
dc.description.sponsorshipMassachusetts Institute of Technology (RSC Award)en_US
dc.description.sponsorshipKavli Foundationen_US
dc.publisherAmerican Physical Societyen_US
dc.relation.isversionofhttp://dx.doi.org/10.1103/PhysRevD.98.103517en_US
dc.rightsArticle is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use.en_US
dc.sourceAmerican Physical Societyen_US
dc.titleGravitational lensing and the power spectrum of dark matter substructure: Insights from the ETHOSen_US
dc.typeArticleen_US
dc.identifier.citationDíaz Rivero, Ana, et al. “Gravitational Lensing and the Power Spectrum of Dark Matter Substructure: Insights from the ETHOS N -Body Simulations.” Physical Review D, vol. 98, no. 10, Nov. 2018.en_US
dc.contributor.departmentMassachusetts Institute of Technology. Department of Physicsen_US
dc.contributor.mitauthorVogelsberger, Mark
dc.relation.journalPhysical Review Den_US
dc.eprint.versionFinal published versionen_US
dc.type.urihttp://purl.org/eprint/type/JournalArticleen_US
eprint.statushttp://purl.org/eprint/status/PeerRevieweden_US
dc.date.updated2018-11-19T18:00:14Z
dc.language.rfc3066en
dc.rights.holderAmerican Physical Society
dspace.orderedauthorsDíaz Rivero, Ana; Dvorkin, Cora; Cyr-Racine, Francis-Yan; Zavala, Jesús; Vogelsberger, Marken_US
dspace.embargo.termsNen_US
dc.identifier.orcidhttps://orcid.org/0000-0001-8593-7692
mit.licensePUBLISHER_POLICYen_US


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