Please use this identifier to cite or link to this item: https://hdl.handle.net/2445/218249
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dc.contributor.authorIzumi ,T.-
dc.contributor.authorMatsuoka, Y.-
dc.contributor.authorOnoue, M.-
dc.contributor.authorStrauss, M. A.-
dc.contributor.authorUmehata, H.-
dc.contributor.authorSilverman, J. D.-
dc.contributor.authorNagao, T.-
dc.contributor.authorImanishi, M.-
dc.contributor.authorKohno, K.-
dc.contributor.authorToba, Y.-
dc.contributor.authorIwasawa, Kazushi-
dc.contributor.authorNakanish,i K.-
dc.contributor.authorSawamura, M.-
dc.contributor.authorFujimoto, S.-
dc.contributor.authorKikuta, S.-
dc.contributor.authorKawaguchi, T.-
dc.contributor.authorAoki, K.-
dc.contributor.authorGoto, T.-
dc.date.accessioned2025-01-30T16:46:16Z-
dc.date.available2025-01-30T16:46:16Z-
dc.date.issued2024-
dc.identifier.issn0004-637X-
dc.identifier.urihttps://hdl.handle.net/2445/218249-
dc.description.abstractWe present Atacama Large Millimeter/submillimeter Array [C ii] 158 μm line and underlying far-IR continuum emission observations (0farcs57 × 0farcs46 resolution) toward a quasar–quasar pair system recently discovered at z = 6.05. The quasar nuclei (C1 and C2) are faint (M1450 ≳ −23 mag), but we detect very bright [C ii] emission bridging the 12 kpc between the two objects and extending beyond them (total luminosity L[C ii] ≃ 6 × 109L⊙). The [C ii]-based total star formation rate of the system is ∼550 M⊙ yr−1 (the IR-based dust-obscured star formation is ∼100 M⊙ yr−1), with a [C ii]-based total gas mass of ∼1011M⊙. The dynamical masses of the two galaxies are large (∼9 × 1010M⊙ for C1 and ∼5 × 1010M⊙ for C2). There is a smooth velocity gradient in [C ii], indicating that these quasars are a tidally interacting system. We identified a dynamically distinct, fast-[C ii] component around C1: detailed inspection of the line spectrum there reveals the presence of a broad-wing component, which we interpret as the indication of fast outflows with a velocity of ∼600 km s−1. The expected mass-loading factor of the outflows, after accounting for multiphase gas, is ≳2 − 3, which is intermediate between AGN-driven and starburst-driven outflows. Hydrodynamic simulations in the literature predict that this pair will evolve to a luminous (M1450 ≲ −26 mag), starbursting (≳1000 M⊙ yr−1) quasar after coalescence, one of the most extreme populations in the early Universe.-
dc.format.extent1 p.-
dc.format.mimetypeapplication/pdf-
dc.language.isoeng-
dc.language.isoeng-
dc.publisherInstitute of Physics (IOP)-
dc.relation.isformatofReproducció del document publicat a: https://doi.org/10.3847/1538-4357/ad57c6-
dc.relation.ispartofAstrophysical Journal, 2024, vol. 972, num.116-
dc.relation.urihttps://doi.org/10.3847/1538-4357/ad57c6-
dc.rights(c) American Astronomical Society, 2024-
dc.sourceArticles publicats en revistes (Institut de Ciències del Cosmos (ICCUB))-
dc.subject.classificationGalàxies-
dc.subject.classificationQuàsars-
dc.subject.otherGalaxies-
dc.subject.otherQuasars-
dc.titleMerging Gas-rich Galaxies That Harbor Low-luminosity Twin Quasars at z = 6.05: A Promising Progenitor of the Most Luminous Quasars<br />-
dc.typeinfo:eu-repo/semantics/article-
dc.typeinfo:eu-repo/semantics/publishedVersion-
dc.identifier.idgrec753792-
dc.date.updated2025-01-30T16:46:16Z-
dc.rights.accessRightsinfo:eu-repo/semantics/openAccess-
Appears in Collections:Articles publicats en revistes (Institut de Ciències del Cosmos (ICCUB))

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