In:
The Astrophysical Journal, American Astronomical Society, Vol. 945, No. 1 ( 2023-03-01), p. 59-
Abstract:
We present a study of the relation between the [O iii ] 5007 Å emission line width ( σ [O III ] ) and stellar velocity dispersion ( σ * ), utilizing a sample of 740 type 1 active galactic nuclei (AGNs) with high-quality spectra at redshift z 〈 1.0. We find the broad correlation between the core component of the [O iii ] emission line width ( σ [ O III , core ] ) and σ * with a scatter of 0.11 dex for the low redshift ( z 〈 0.1) sample; for redshift (0.3 〈 z 〈 1.0) AGNs, the scatter is larger, being 0.16 dex. We also find that the Eddington ratio ( L bol / L Edd ) may play an important role in the discrepancies between σ [ O III , core ] and σ * . As the L bol / L Edd increases, σ [ O III , core ] tends to be larger than σ * . By classifying our local sample with different minor-to-major axis ratios, we find that σ * is larger than σ [ O III , core ] for those edge-on spiral galaxies. In addition, we also find that the effects of outflow strength properties such as maximum outflow velocity ( V max ) and the broader component of the [O iii ] emission line width and line shift ( σ [O III ,out] and V [O III ,out] ) may play a major role in the discrepancies between σ [ O III , core ] and σ * . The discrepancies between σ [ O III , core ] and σ * are larger when V max , V [O III ,out] , and σ [O III ,out] increase. Our results show that the outflow strengths may have significant effects on the differences between narrow-line region gas and stellar kinematics in AGNs. We suggest that caution should be taken when using σ [ O III , core ] as a surrogate for σ * . In addition, the substitute of σ [ O III , core ] for σ * could be used only for low luminosity AGNs.
Type of Medium:
Online Resource
ISSN:
0004-637X
,
1538-4357
DOI:
10.3847/1538-4357/acb770
Language:
Unknown
Publisher:
American Astronomical Society
Publication Date:
2023
detail.hit.zdb_id:
2207648-7
detail.hit.zdb_id:
1473835-1
SSG:
16,12
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