Please use this identifier to cite or link to this item: https://hdl.handle.net/2445/218358
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dc.contributor.authorArita, J.-
dc.contributor.authorKashikawa, N.-
dc.contributor.authorMatsuoka, Y.-
dc.contributor.authorHe, W.-
dc.contributor.authorIto, K.-
dc.contributor.authorLiang, Y.-
dc.contributor.authorIshimoto, R.-
dc.contributor.authorYoshioka, T.-
dc.contributor.authorTakeda, Y.-
dc.contributor.authorIwasawa, Kazushi-
dc.contributor.authorOnoue, M.-
dc.contributor.authorToba, Y.-
dc.contributor.authorImanishi, M.-
dc.date.accessioned2025-01-31T16:54:48Z-
dc.date.available2025-01-31T16:54:48Z-
dc.date.issued2023-
dc.identifier.issn0004-637X-
dc.identifier.urihttps://hdl.handle.net/2445/218358-
dc.description.abstractWe present, for the first time, dark matter halo (DMH) mass measurement of quasars at z ∼ 6 based on a clustering analysis of 107 quasars. Spectroscopically identified quasars are homogeneously extracted from the Hyper Suprime-Cam Strategic Survey Program wide layer over 891 deg2. We evaluate the clustering strength by three different autocorrelation functions: projected correlation function, angular correlation function, and redshift–space correlation function. The DMH mass of quasars at z ∼ 6 is evaluated as with the bias parameter b = 20.8 ± 8.7 by the projected correlation function. The other two estimators agree with these values; though, each uncertainty is large. The DMH mass of quasars is found to be nearly constant ∼1012.5h−1M⊙ throughout cosmic time, suggesting that there is a characteristic DMH mass where quasars are always activated. As a result, quasars appear in the most massive halos at z ∼ 6, but in less extreme halos thereafter. The DMH mass does not appear to exceed the upper limit of 1013h−1M⊙, which suggests that most quasars reside in DMHs with across most of the cosmic time. Our results supporting a significant increasing bias with redshift are consistent with the bias evolution model with inefficient active galactic nucleus feedback at z ∼ 6. The duty cycle (fduty) is estimated as 0.019 ± 0.008 by assuming that DMHs in some mass interval can host a quasar. The average stellar mass is evaluated from stellar-to-halo mass ratio as, which is found to be consistent with [C ii] observational results.-
dc.format.extent1 p.-
dc.format.mimetypeapplication/pdf-
dc.language.isoeng-
dc.publisherInstitute of Physics (IOP)-
dc.relation.isformatofReproducció del document publicat a: https://doi.org/10.3847/1538-4357/ace43a-
dc.relation.ispartofAstrophysical Journal, 2023, vol. 954, num.210-
dc.relation.urihttps://doi.org/10.3847/1538-4357/ace43a-
dc.rights(c) American Astronomical Society, 2023-
dc.sourceArticles publicats en revistes (Institut de Ciències del Cosmos (ICCUB))-
dc.subject.classificationQuàsars-
dc.subject.classificationForats negres (Astronomia)-
dc.subject.classificationGalàxies-
dc.subject.otherQuasars-
dc.subject.otherBlack holes (Astronomy)-
dc.subject.otherGalaxies-
dc.titleSubaru High-z Exploration of Low-luminosity Quasars (SHELLQs). XVIII. The Dark Matter Halo Mass of Quasars at z ∼ 6-
dc.typeinfo:eu-repo/semantics/article-
dc.typeinfo:eu-repo/semantics/publishedVersion-
dc.identifier.idgrec753896-
dc.date.updated2025-01-31T16:54:48Z-
dc.rights.accessRightsinfo:eu-repo/semantics/openAccess-
Appears in Collections:Articles publicats en revistes (Institut de Ciències del Cosmos (ICCUB))

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