Detection of Iron Emission in the z = 5.74 QSO SDSSp J104433.04 $-$ 012502.2
We obtained near-infrared spectroscopy of the $z = 5.74$ QSO, SDSSp J104433.04 $-$ 012502.2, with the Infrared Camera and Spectrograph of the Subaru Telescope. The redshift of 5.74 corresponds to a cosmological age of 1.0 Gyr for the current $\Lambda$ -dominated cosmology. We found a similar strengt...
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Published in | Publications of the Astronomical Society of Japan Vol. 54; no. 3; pp. 353 - 358 |
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Main Authors | , , |
Format | Journal Article |
Language | English |
Published |
Oxford, UK
Oxford University Press
25.06.2002
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Subjects | |
Online Access | Get full text |
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Summary: | We obtained near-infrared spectroscopy of the
$z = 5.74$
QSO, SDSSp J104433.04
$-$
012502.2, with the Infrared Camera and Spectrograph of the Subaru Telescope. The redshift of 5.74 corresponds to a cosmological age of 1.0 Gyr for the current
$\Lambda$
-dominated cosmology. We found a similar strength of the Fe ii (3000–3500 Å) emission lines in SDSSp J104433.04
$-$
012502.2 as in low-redshift QSOs. This is the highest redshift detection of iron. We subtracted a power-law continuum from the spectrum and fitted model Fe ii emission and the Balmer continuum. The rest equivalent width of Fe ii (3000–3500 Å) is
$\sim 30 \,$
Å, which is similar to those of low-redshift QSOs measured in the same manner. The chemical-enrichment models that assume the lifetime of the progenitor of SNe Ia is longer than 1 Gyr predict that weaker Fe ii emission in high-redshift (
$z \gt 3$
) QSOs than low-redshift ones. However, none of the observed high redshift QSOs show a systematic decrease of Fe ii emission compared with low-redshift QSOs. This may be due to a shorter lifetime of SNe Ia in QSO nuclei than in the solar neighborhood. Another reason for the strong Fe ii emission at
$z = 5.74$
may be a longer cosmological age due to a smaller
$\Omega _\mathrm{M}$
. |
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ISSN: | 0004-6264 2053-051X |
DOI: | 10.1093/pasj/54.3.353 |