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A Census of Ionized Gas Outflows in Type 1 AGNs: Gas Outflows in AGNs. V.
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Abstract
We present a systematic study of ionized gas outflows based on the velocity shift and dispersion of the [O
iii
]
λ
5007 emission line using a sample of ∼5000 Type 1 AGNs at
z
< 0.3 selected from the Sloan Digital Sky Survey. This analysis is supplemented by the gas kinematics of Type 2 AGNs from Woo et al. For the majority of Type 1 AGNs (i.e., ∼89%), the [O
iii
] line profile is best represented by a double Gaussian model, presenting the kinematic signature of the nonvirial motion. Blueshifted [O
iii
] is more frequently detected than redshifted [O
iii
] by a factor of 3.6 in Type 1 AGNs, while the ratio between blueshifted and redshifted [O
iii
] is only 1.08 in Type 2 AGNs due to the projection and orientation effect. The fraction of AGNs with outflow signatures is found to increase steeply with [O
iii
] luminosity and Eddington ratio, while Type 1 AGNs have larger velocity dispersion and more negative velocity shift than Type 2 AGNs. The [O
iii
] velocity–velocity dispersion diagram of Type 1 AGNs expands toward higher values with increasing luminosity and Eddington ratio, suggesting that the radiation pressure or wind is the main driver of gas outflows, as similarly found in Type 2 AGNs. In contrast, the kinematics of gas outflows is not directly linked to the radio activity of AGNs.
Title: A Census of Ionized Gas Outflows in Type 1 AGNs: Gas Outflows in AGNs. V.
Description:
Abstract
We present a systematic study of ionized gas outflows based on the velocity shift and dispersion of the [O
iii
]
λ
5007 emission line using a sample of ∼5000 Type 1 AGNs at
z
< 0.
3 selected from the Sloan Digital Sky Survey.
This analysis is supplemented by the gas kinematics of Type 2 AGNs from Woo et al.
For the majority of Type 1 AGNs (i.
e.
, ∼89%), the [O
iii
] line profile is best represented by a double Gaussian model, presenting the kinematic signature of the nonvirial motion.
Blueshifted [O
iii
] is more frequently detected than redshifted [O
iii
] by a factor of 3.
6 in Type 1 AGNs, while the ratio between blueshifted and redshifted [O
iii
] is only 1.
08 in Type 2 AGNs due to the projection and orientation effect.
The fraction of AGNs with outflow signatures is found to increase steeply with [O
iii
] luminosity and Eddington ratio, while Type 1 AGNs have larger velocity dispersion and more negative velocity shift than Type 2 AGNs.
The [O
iii
] velocity–velocity dispersion diagram of Type 1 AGNs expands toward higher values with increasing luminosity and Eddington ratio, suggesting that the radiation pressure or wind is the main driver of gas outflows, as similarly found in Type 2 AGNs.
In contrast, the kinematics of gas outflows is not directly linked to the radio activity of AGNs.
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