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Zhang XueGuang

Publications and source records attributed to Zhang XueGuang.

At least 19 recordsLinked to original sources

A Short-timescale Negative Optical Continuum Lag in SDSS J083717.88+191647

Continuum reverberation mapping (RM) is a powerful technique for constraining the accretion disk structure in active galactic nuclei (AGNs). In typical cases, the shorter-wavelength emission is used as the reference, and a positive time lag is observed since the inner, hotter regions of the accretion disk respond earlier than the cooler outer regions at longer wavelengths. However, we detect a short-timescale negative inter-band lag in SDSS~J083717.88+191647 using RM techniques, where the \textit{g}-band lags behind the \textit{r}-band emission. The light curves from the Zwicky Transient Facility reveal two distinct phases, a stabilizing and a declining phase, in which the time lags show opposite signs. Using \texttt{JAVELIN} with the $g$-band as the reference, we obtain time lags of $3.68^{+1.94}_{-2.78}$~days during the stabilizing phase and $-1.60^{+0.69}_{-0.54}$~days during the declining phase. Although negative continuum lags have been reported in a few previous studies, the present case is distinguished by its clear phase dependence and the accompanying color evolution. We attribute the observed lag reversal to a moving dust-cloud obscuration scenario, in which the cloud crossing the line of sight preferentially obscures emission from the outer longer-wavelength regions of the disk, causing the $r$-band to decline earlier than the $g$-band and thus producing the observed negative inter-band lag. Our results indicate that AGN variability may be more complex than previously thought. Future high-cadence, multi-band observations will be essential to test this dust-obscuration model and to further explore the interplay between the accretion disk emission and dust in AGNs.

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Unique photometric variability in SDSS J134628.62+173659.5: clues for moving dust clouds as physical origin of changing-look AGN

The scenario of variations in accreting process around central black hole has been widely accepted as the preferred physical origin of changing-look active galactic nuclei (CLAGN), rather than obscuration effects by moving dust clouds. In this manuscript, after analyzing long-term photometric variability in Type-1.8 AGN SDSS J1346+1736 with apparent broad H$α$ but very weak broad H$β$, robust clues for obscurations can be confirmed with confidence level higher than 10$σ$. Then, based on obscurations related to moving dust clouds, from dark state with E(B-V)$\sim$1.26 to bright state with E(B-V)$\sim$0.55, apparent both broad H$α$ and broad H$β$ can be clearly expected. Meanwhile, the expected line luminosity from reddening corrected continuum luminosity is consistent with the reddening corrected line luminosity, to support the obscuration effects. Furthermore, through symmetric features in the light curves, probability is only 3.2\% in SDSS J1346+1736 to support the scenario of variations of accretion rates traced by CAR process. Therefore, besides the more and more preferred scenario of variations in accreting process, the scenario of moving dust clouds could be more reasonable in some CLAGN with apparent variations in optical colors.

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Clues for the accretion regulated dust torus in the changing-look AGN SDSS J101152.98+544206.4

Dust torus plays the key role in determining active galactic nuclei (AGN) observational appearance. Here, the scenario of accretion regulated central dust torus is tested for the first time in the individual changing-look AGN (CLAGN) SDSS J1011+5442. Through the dependence of broad H$α$ luminosity on continuum luminosity, the scenario of moving dust clouds can be ruled out in SDSS J1011+5442. Meanwhile, virial BH mass in the bright state is consistent with the M-sigma relation determined mass, indicating the virialization assumptions efficient in central BLRs. However, the virial BH mass determined in the dim state is 60 times smaller than the M-sigma relation determined value. The contrary properties of broad H$α$ in different states can be naturally explained by the scenario of accretion regulated dust torus. Below a critical Eddington ratio, opening angle of dust torus declines with increasing accretion rate, leading to only outer part of central BLRs for broad H$α$ with smaller line widths detected in the dim state but all the BLRs detected in the bright state. The results in this manuscript not only indicate properties of central dust torus having apparent effects on variability properties of CLAGN, but also indicate that studying CLAGN could provide further clues to check dynamical evolving models for dust torus in AGN.

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Similar ratios of rise timescale to decline timescale of optical light curves in common tidal disruption events

Totally similar physical process in tidal disruption events (TDEs) basically indicates that there should be potential parameter to distinguish variability properties of TDEs from the other transient events having different physical processes. Here, we try to report such a parameter, the timescale ratio $R_{2/1,rd}$ of rise timescale $t_{1/2,r}$ (from half-max to maximum) to decline timescale $t_{1/2,d}$ (from maximum to half-max), especially based on the 34 optical TDEs with reported $t_{1/2,r}$ and $t_{1/2,d}$. Among the 34 optical TDEs, AT2020wey is an outlier with $R_{2/1,rd}\sim2.7$ which is 4.5 times larger than the mean value 0.6 of the other optical TDEs. However, after considering similar but more flexible model functions, the re-determined $R_{2/1,rd}$ is $\sim$0.9 in AT2020wey, totally similar as the values of the other optical TDEs. Therefore, the parameter $R_{1/2,rd}\sim0.6$ could be a potential classification parameter for optical TDEs. Furthermore, $R_{1/2,rd}$ have been checked in the unique optical transients of AT2019avd, PS1-10adi, SDSS J0946+3512 and J2334+1457. We can find that the second flare with $R_{1/2,rd}\sim11$ in AT2019avd should be very different from the other optical TDEs, but PS1-10adi, SDSS J0946+3512, J2334+1457 and the first flare in AT2019avd should be similar as the other optical TDEs. In the near future, properties of $R_{1/2,rd}$ through large sample of optical transients could provide further clues to support whether $R_{1/2,rd}$ could be a better classification parameter to distinguish TDEs and the other transient events.

astro-ph.HE

Optical QPOs with different periodicities in CSS and ZTF light curves of the quasar 4C 50.43

Long-standing optical quasi-periodic oscillations (QPOs) with periodicity of hundreds to thousands of days have been accepted as indicators for central sub-pc binary black hole systems (BBHs) in broad line active galactic nuclei (BLAGN). However, there are so far no direct reports on whether such reported optical QPOs have their periodicities constant in different periods. Here, based on different methods applied to light curves of 4C 50.43 in different periods, optical QPOs with periodicity of 1124days was detected in the CSS V-band light curve, while a shorter periodicity of 513days was detected in the ZTF g/r band light curves. Despite the two periodicities near-harmonic 2:1 ratio, their absence of simultaneous detection in the lomb-scargle periodograms of the ZTF light curves suggests that they are unlikely to be harmonically related. Potential factors were considered to explain these two distinct periodicities, especially different temporal coverage, signal-to-noise ratio and time steps between the CSS and ZTF light curves, as well as the effects of red noises related to intrinsic AGN variability. Our analysis shows that red noises have strong influence on the different periodicities in 4C 50.43 supporting our previous simulations. The results in this manuscript strongly indicate that it should be cautioned for applications of determined optical QPOs in BLAGN having strong intrinsic AGN variability.

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Double tidal disruption events or repeating partial tidal disruption events in AT 2020vdq

AT 2020vdq has been known as a candidate of repeating partial tidal disruption events (pTDEs), due to its two flares with a time interval of $\sim$1000 days. Here, a simplified method is proposed to test such repeating pTDEs scenario considering a main-sequence star tidally disrupted twice. For the two flares in AT 2020vdq if related to the repeating pTDEs scenario, theoretical TDE model determined stellar mass of the original star disrupted for the first flare should be not very different from the mass of the star (to trace the reminder of the original star) disrupted for the second flare, because a partial TDE with impact parameter $β$ smaller than 1 can lead to most of (probable higher than 90\%) the stellar mass also bound to the reminder of the original star. After considering theoretical TDE model applied to describe the two flares in AT 2020vdq, the model determined stellar masses are about 2${\rm M_\odot}$ and $0.36{\rm M_\odot}$ for the stars disrupted in the first flare and the second flare. The large mass difference cannot be reasonably expected by the repeating pTDEs with $β$ around 0.6 in AT 2020vdq. The results in this manuscript indicate that the repeating pTDEs scenario is not preferred at current stage in AT 2020vdq, but the probable double TDEs for two individual stars tidally disrupted should be currently recommended.

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Variability of optical spectral index to support a central sub-parsec binary black hole system in quasar SDSS J001224-102226.51

In this manuscript, variations in optical spectral index $α_{5100}$ are applied for detecting central sub-parsec binary black hole systems (sub-pc BBHs) in broad line active galactic nuclei (BLAGN), due to apparent effects of obscurations on central two BH accreting systems. For sub-pc BBHs in BLAGN, two main characteristics on $α_{5100}$ can be expected. First, if a BLAGN harbours a central sub-pc BBH, the expected unique variability in $α_{5100}$ should lead the BLAGN to be an outlier in the space of $α_{5100}$ versus continuum luminosity $L_{5100}$ determined from normal BLAGN. Second, BLAGN harbouring central sub-pc BBHs could lead to periodic variations in $α_{5100}$. Here, after checking the two-epoch SDSS spectra of quasar SDSS J0012-1022 reported as a candidate of sub-pc BBH by large velocity offset between narrow and broad Balmer emission lines, unique variability of $α_{5100}$ can be explained by effects of obscurations related to an assumed central sub-pc BBH. In the near future, to detect and report periodic variations of $α_{5100}$ for sub-pc BBHs in BLAGN should be our main objective. The results provide a new method by applications of properties of optical continuum emissions for detecting sub-pc BBHs in BLAGN.

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Quasi-periodic oscillations in optical color evolutions to support sub-pc binary black hole systems in broad line active galactic nuclei

Optical quasi-periodic oscillations (QPOs) with periodicity around hundreds to thousands of days have been accepted as an efficient indicator for sub-pc binary black hole systems (BBHs) in broad line active galactic nuclei (BLAGN). However, considering intrinsic variability (red noises) of BLAGN, it is still an open question on physical origin of detected optical QPOs from AGN variability or truly from sub-pc BBHs. Here, a simple method is proposed to support optical QPOs related to sub-pc BBHs by detecting QPOs in time dependent optical color evolutions of BLAGN. Periodic variations of obscurations are expected on optical light curves related to sub-pc BBHs, but there should be non-periodic variable obscurations on optical light curves in normal BLAGN. Through simulated optical light curves for intrinsic AGN variability by Continuous AutoRegressive process with time durations around 2800days (similar as time durations of light curves in ZTF), the probability is definitely smaller than $3.3\times10^{-7}$ that QPOs can be detected in the corresponding optical color evolutions, but about $3.1\times10^{-2}$ that optical QPOs with periodicity smaller than 1400days (at least two cycles) can be detected in the simulated single-band light curves. Therefore, confidence level is definitely higher than 5$σ$ to support the QPOs in color evolutions not related to intrinsic AGN variability but truly related to sub-pc BBHs. In the near future, the proposed method can be applied for searching reliable optical QPOs in BLAGN through multi-band light curves from the ZTF and the upcoming LSST.

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Double tidal disruption events in the changing-look AGN Mrk1018

Tidal disruption events (TDEs) as excellent beacons to black hole (BH) accreting systems have been studied for more than five decades with a single star tidally disrupted by a central massive BH. However, if considering two stars passing through a central BH and being tidally disrupted in a short period, so-called double TDEs could be expected and lead to unique variability features very different from features from standard TDEs. Here, we report such oversimplified double TDEs in the known changing-look AGN Mrk1018, of which 15years-long light curve with plateau features can be described by two main-sequence stars tidally disrupted by the central supermassive BH. Meanwhile, the BH mass determined by the double TDEs is consistent with the M-sigma relation determined value by the measured stellar velocity dispersions in Mrk1018. The results indicate tight connections between the TDEs and the changing-look properties in Mrk1018.

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More than 60% of double-peaked narrow emission lines not related to dual galaxy systems?

Dual galaxy system (DGS) is one of the widely accepted scenarios to explain the double-peaked narrow emission lines (DPNELs) due to orbital motions of the two galaxies in a merging system. After considering no physical connections between two independent narrow emission line regions in two galaxies in one DGS, there should be no correlations between flux ratios $R_{R}$ of red-shifted narrow emission components from one galaxy and flux ratios $R_{B}$ of blue-shifted narrow emission components from the other galaxy in the DGS. However, after checking the large sample of DPNELs in the SDSS, there are strong linear correlations in different groups between $R_{R}$ as the flux ratio of red-shifted narrow [O~{\sc iii}] to the red-shifted narrow H$α$ and $R_{B}$ as the flux ratio of blue-shifted narrow [O~{\sc iii}] to the blue-shifted narrow H$α$. Meanwhile, after checking narrow emission line properties of galaxy pairs within 30 (20, 10) arcmins, there are no connections between narrow emission line fluxes in the galaxy pairs, to support the detected linear correlations being robust enough between $R_{R}$ and $R_{B}$ in the DPNELs in SDSS. Furthermore, through oversimplified simulations, at least more than 60% of the DPNELs should be not related to the expected DGSs.

astro-ph.GA

No apparent forbidden/permitted narrow emission lines in the broad line quasar SDSS J1251+0613

Strong both broad and narrow emission lines from central broad emission line regions (BLRs) and narrow emission line regions (NLRs) are fundamental spectroscopic characteristics of broad line Active Galactic Nuclei (BLAGNs). Lack of central BLRs leads to the identified true Type-2 AGNs without central hidden BLRs, providing clues on formation/suppression of AGN BLRs. Whether were there BLAGNs with lack of central NLRs is still an open question. Here, in the blue quasar SDSS J1251+0613, both blue continuum emissions and broad emission lines can be clearly detected in its SDSS spectrum, however there are no apparently detected narrow emission lines in the optical/NUV bands, leading to no central normal NLRs in the blue quasar SDSS J1251+0613. In order to explain the lack of NLRs, evolving NLRs is proposed that the radial outflows are carrying materials from BLRs to NLRs and the current narrow line emission materials are lying closer to the outer side of central BLRs in SDSS J1521+0613. The results in this manuscript can indicate a new unique subclass of BLAGNs, the BLAGNs without central normal NLRs, which will provide potential clues on physical origin/evolution of AGN NLRs.

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A candidate for True Type-2 AGN without hidden central BLRs Identified by central Tidal Disruption Event

In this manuscript, through applications of TDE (tidal disruption event) expected variability properties, a potential candidate for True type-2 AGN without hidden central broad line regions (=TT2AGN) is reported in the SDSS J233454.07+145712.9 (=SDSS J2334). Through analyzing the 20-years optical light curves of SDSS J2334 from different Sky Survey projects, a TDE is preferred with a $4.7{\rm M_\odot}$ main-sequence star tidally disrupted by the central BH with mass $11.7\times 10^6{\rm M_\odot}$, indicating that central region within distance about 20 light-days to central BH in SDSS J2334 is directly in the line-of-sight. Moreover, AGN activities in SDSS J2334 can be confirmed through applications of BPT diagrams. Meanwhile, comparing virial BH mass determined through assumed broad Balmer emission components and M-sigma expected BH mass by well measured stellar velocity dispersion through stellar absorption features, optical broad emission lines in SDSS J2334 are disfavored with confidence level higher than 6$σ$. Therefore, combining the unique properties of the TDE and the spectroscopic results with only narrow emission lines, SDSS J2334 can be well identified as a potential candidate for a TT2AGN. The results indicate the to detect TDE expected flares in normal Type-2 AGN classified by spectroscopic results should be a new practicable method for identifying

astro-ph.GA

Evolution of broad emission lines from double-peaked to single-peaked to support a central tidal disruption event

In this manuscript, considering evolution of fallback accreting debris in a central Tidal Disruption Event (TDE), the outer boundary increased with time of the disk-like broad emission line regions (BLRs) lying into central accretion disk will lead expected broad emission lines changed from double-peaked to single-peaked. Considering common elliptical orbitals for the accreting fallback TDEs debris, based on simulated results through the preferred standard elliptical accretion disk model, a probability about 3.95\% can be estimated for cases with double-peaked profile changed to single-peaked profile in multi-epoch broad emission lines, indicating such unique profile variability could be indicator for BLRs related to TDE debris. Meanwhile, among the reported optical TDE candidates with apparent broad lines, such profile changes in broad H$α$ can be found in the AT 2018hyz. After accepted the outer boundaries of the disk-like BLRs increased with time, the observed multi-epoch broad H$α$ can be described in AT 2018hyz. Moreover, the elliptical accretion disk model determined time dependent ratios of the outer boundaries of the disk-like BLRs are well consistent with the TDE model expected ratios of the outer boundaries of the fallback TDE debris. Furthermore, the evolution properties of disk-like BLRs can be applied to estimate the locations of the disk-like BLRs of which outer boundary could be about one sixth of the outer boundary of the fallback TDE debris in AT 2018hyz. Such unique profile changes from double-peaked to single-peaked could be applied as further clues to support a central TDE.

astro-ph.GA

Dependence of 4000Å~ break strength on narrow emission line properties in local Type-2 AGN

In this manuscript, we report evidence to support the dependence of D{\it n}4000 (4000Å~ break strength to trace stellar ages) on central AGN activity traced by narrow emission line properties in local Type-2 AGN in SDSS DR16. Based on the measured D{\it n}4000 and flux ratios of [O~{\sc iii}] to narrow H$β$ (O3HB) and [N~{\sc ii}] to narrow H$α$ (N2HA) and narrow H$α$ line luminosity $L_{Hα}$, linear dependence of the D{\it n}4000 on the O3HB, N2HA and $L_{Hα}$ in the local Type-2 AGN can provide clues to support the dependence of D{\it n}4000 on properties of narrow emission lines. Linear correlations between the D{\it n}4000 and the O3HB and N2HA can be found in the local Type-2 AGN, with Spearman rank correlations about -0.39 and 0.53. Meanwhile, stronger dependence of the D{\it n}4000 on the $L_{Hα}$ can be confirmed in Type-2 AGN, with Spearman rank correlation coefficient about -0.7. Moreover, combining the $L_{Hα}$ and the N2HA, a more robust and stronger linear correlation can be confirmed between the D{\it n}4000 and the new parameter $LR=0.2\log(L_{Hα})-0.5\log(\rm N2HA)$, with Spearman rank correlation coefficient about -0.76 and with smaller RMS scatters. After considering necessary effects, the dependence of D{\it n}4000 on $LR$ is stable and robust enough for the local Type-2 AGN, indicating the $LR$ on the narrow emission lines can be treated as a better indicator to statistically trace stellar ages of samples of more luminous AGN with weaker host galaxy absorption features.

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Periodic variations of the first and second moments of broad Balmer emission lines from central accretion disks

Broad emission line regions (BLRs) lying into central accretion disks has been widely accepted to explain the unique double-peaked broad emission lines in Active Galactic Nuclei (double-peaked BLAGNs). Here, accepted the accretion disk origin, periodic variations of central wavelength $λ_{0}$ (the first moment) and line width $σ$ (the second moment) of double-peaked broad emission lines are theoretically simulated and determined. Furthermore, through theoretically simulated periodicities of $T_{\lambda0}$ and $T_σ$ for variations of $λ_0$ and $σ$, periodicity ratio $R_{fs}$ of $T_{\lambda0}$ to $T_σ$ to be around 2 can be applied to support the spiral arms to be more preferred in BLRs lying into central accretion disks. Then, periodic variations of $λ_0$ and $σ$ are determined and shown in the known double-peaked BLAGN NGC1097, leading to the parameter $R_{fs}\sim2$, which can be applied as clues to support that the structure of spiral arms in disk-like BLRs in central accretion disk should be the most compelling interpretation to the variability of double-peaked broad H$α$ in NGC1097. The results provide clean criteria to test accretion disk origins of double-peaked broad emission lines in AGN.

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Effects of intrinsic AGN variability on optical QPOs related to sub-pc binary black hole systems in broad line AGN

In this manuscript, an oversimplified model is proposed to test the effects of intrinsic AGN variability on expected optical quasi-periodic oscillations (QPOs) related to sub-pc binary black hole systems (BBHs) in broad line AGN. The commonly accepted CAR (Continuous AutoRegressive) process is applied to describe intrinsic AGN variability related to each BH accreting system in a sub-pc BBH system. Considering obscurations related to orbital rotations with periodicity $T_p$, artificial light curves including signals for optical QPOs can be built. Then, comparing the intrinsic periodicities $T_p$ with the measured robust periodicities $T_o$ through the artificial light curves, distributions of $T_p/T_o$ have four significant peaks around 1, 2, 3 and 4, leading less than half of the artificial light curves to have consistency between $T_o$ and $T_p$. Moreover, different collected model parameters have few effects on the distributions of $T_p/T_o$, indicating the effects of intrinsic AGN variability on optical QPOs are significantly strong and stable. Furthermore, after checking properties of optical QPOs in the light curves with different time steps, there are tiny effects of time steps on optical QPOs.

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A normal broad line AGN SDSS J1617+0638 as the host galaxy of a central tidal disruption event

In this manuscript, strong clues are reported to support the normal broad line AGN SDSS J1617+0638 as the host galaxy harboring a central tidal disruption event (TDE). Through the optical flare in the CSS 8.5years-long light curve and the none-variability in the up-to-date ASAS-SN light curves, the theoretical TDE model described by the MOSFIT code can be applied in SDSS J1617+0638. Meanwhile, considering the assumed central TDE expected continuum emissions not strong enough to describe the continuum emissions in the SDSS spectrum of SDSS J1617+0638, an additional power law component from pre-existing AGN activity should be necessary in SDSS J1617+0638. Furthermore, considering the short time duration to the observed date for the SDSS spectrum from the starting time of the assumed central TDE in SDSS J1617+0638, TDE model expected accreting mass only about 0.03$M_\odot$ can lead to few effects of TDEs debris on the observed broad emission lines in the SDSS spectrum of SDSS J1617+0638, indicating the TDE model determined BH mass simply consistent with the virial BH mass by broad emission lines, as determined results in SDSS J1617+0638. Therefore, through both the photometric variability and the spectroscopic results, a central TDE can be preferred in the normal broad line AGN SDSS J1617+0638 with pre-existing central AGN activity and pre-existing broad emission line regions.

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Are there higher electron densities in narrow emission line regions of Type-1 AGN than Type-2 AGN?

In the manuscript, we check properties of electron densities $n_e$ traced by flux ratio $R_{sii}$ of [S~{\sc ii}]$\lambda6716$Å~ to [S~{\sc ii}]$\lambda6731$Å~ in narrow emission line regions (NLRs) between Type-1 AGN and Type-2 AGN in SDSS DR12. Under the framework of Unified Model considering kpc-scale structures, similar $n_e$ in NLRs should be expected between Type-1 AGN and Type-2 AGN. Based on reliable measurements of [S~{\sc ii}] doublet with measured parameters at least five times larger than corresponding uncertainties, there are 6039 Type-1 AGN and 8725 Type-2 AGN (excluding the Type-2 LINERs and the composite galaxies) collected from SDSS DR12. Then, lower $R_{sii}$ (higher $n_e$) in NLRs can be well confirmed in Type-1 AGN than in Type-2 AGN, with confidence level higher than 5$σ$, even after considering necessary effects including effects of electron temperatures traced by [O~{\sc iii}]$\lambda4364,4959,5007$Å~ on estimating $n_e$ in NLRs. Two probable methods are proposed to explain the higher $n_e$ in NLRs in Type-1 AGN. First, the higher $n_e$ in NLRs of Type-1 AGN could indicate longer time durations of AGN activities in Type-1 AGN than in Type-2 AGN, if AGN activities triggering galactic-scale outflows leading to more electrons injecting into NLRs were accepted to explain the higher $n_e$ in NLRs of Type-2 AGN than HII galaxies. Second, the lower $n_e$ in NLRs of Type-2 AGN could be explained by stronger star-forming contributions in Type-2 AGN, considering lower $n_e$ in HII regions. The results provide interesting challenges to the commonly and widely accepted Unified Model of AGN.

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