2018
DOI: 10.1093/mnras/sty1811
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Optical spectroscopy of local type-1 AGN LINERs

Abstract: The Balmer emission originated in the broad line region (BLR) of active galactic nuclei (AGNs) could be either weak and difficult to detect, or even absent, for low luminosity AGNs, as LINERs. Our goals in this paper are threefold. First, we want to explore the AGN-nature of nearby type-1 LINERs. Second, we aim at deriving a reliable interpretation for the different components of emission lines by studying their kinematics and ionization mechanism. Third, we intend to probe the neutral gas in the nuclei of the… Show more

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Cited by 35 publications
(79 citation statements)
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References 131 publications
(224 reference statements)
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“…While the first one is most likely associated with cold material in the torus, the latter may be explained as material along the line of sight in the galaxy or as outflows. Recent optical spectroscopy of NGC 1052 show evidence of possible outflows, preferentially seen in [O I], in agreement with the second scenario (Cazzoli et al 2018). However, our X-ray analysis shows an ionisation degree consistent with the neutral state.…”
Section: Absorption and Reflectionsupporting
confidence: 78%
“…While the first one is most likely associated with cold material in the torus, the latter may be explained as material along the line of sight in the galaxy or as outflows. Recent optical spectroscopy of NGC 1052 show evidence of possible outflows, preferentially seen in [O I], in agreement with the second scenario (Cazzoli et al 2018). However, our X-ray analysis shows an ionisation degree consistent with the neutral state.…”
Section: Absorption and Reflectionsupporting
confidence: 78%
“…We plan to measure emission lines in both new and archival optical spectra of the selected AGNs fitting both narrow and broad lines, as in Cazzoli et al (2018). The measurements will be compared to those in the literature and to the optical/X-ray properties.…”
Section: Main Results and Future Workmentioning
confidence: 99%
“…The observed value is 221±2 km s −1 , whereas the instrumental broadening is 183±7 km s −1 , thus we obtained σ =124±11 km s −1 . Using this measurement and following the relation in Gültekin et al (2009) Following Cazzoli et al (2018), we estimated the accuracy of the fit as the ratio between the standard deviation values estimated from a wavelength range under the line of interest ε line and that from a portion of the continuum free of both emission and absorption lines, ε c , i.e. ε fit line = ε line /ε c .…”
Section: Clumpymentioning
confidence: 99%