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               <mods:name>
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                  <mods:namePart>Arita, J.</mods:namePart>
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               <mods:name>
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                  <mods:namePart>Kashikawa, N.</mods:namePart>
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                  <mods:namePart>Matsuoka, Y.</mods:namePart>
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                  <mods:namePart>He, W.</mods:namePart>
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               <mods:name>
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                  <mods:namePart>Ito, K.</mods:namePart>
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               <mods:name>
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                  <mods:namePart>Liang, Y.</mods:namePart>
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                  <mods:namePart>Ishimoto, R.</mods:namePart>
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                  <mods:namePart>Yoshioka, T.</mods:namePart>
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                  <mods:namePart>Takeda, Y.</mods:namePart>
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                  <mods:namePart>Iwasawa, Kazushi</mods:namePart>
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               <mods:name>
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                  <mods:namePart>Onoue, M.</mods:namePart>
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               <mods:name>
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                     <mods:roleTerm type="text">author</mods:roleTerm>
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                  <mods:namePart>Toba, Y.</mods:namePart>
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               <mods:name>
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                     <mods:roleTerm type="text">author</mods:roleTerm>
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                  <mods:namePart>Imanishi, M.</mods:namePart>
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                  <mods:dateIssued encoding="iso8601">2025-01-31T16:54:48Z2025-01-31T16:54:48Z20232025-01-31T16:54:48Z</mods:dateIssued>
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               <mods:identifier type="none"/>
               <mods:abstract>We 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.</mods:abstract>
               <mods:language>
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               <mods:accessCondition type="useAndReproduction">(c) American Astronomical Society, 2023 info:eu-repo/semantics/openAccess</mods:accessCondition>
               <mods:subject>
                  <mods:topic>Quàsars</mods:topic>
               </mods:subject>
               <mods:subject>
                  <mods:topic>Forats negres (Astronomia)</mods:topic>
               </mods:subject>
               <mods:subject>
                  <mods:topic>Galàxies</mods:topic>
               </mods:subject>
               <mods:subject>
                  <mods:topic>Quasars</mods:topic>
               </mods:subject>
               <mods:subject>
                  <mods:topic>Black holes (Astronomy)</mods:topic>
               </mods:subject>
               <mods:subject>
                  <mods:topic>Galaxies</mods:topic>
               </mods:subject>
               <mods:titleInfo>
                  <mods:title>Subaru High-z Exploration of Low-luminosity Quasars (SHELLQs). XVIII. The Dark Matter Halo Mass of Quasars at z ∼ 6</mods:title>
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