1,133 research outputs found

    Broadband X-ray spectral analysis of the Seyfert 1 galaxy GRS 1734-292

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    We discuss the broadband X-ray spectrum of GRS 1734-292 obtained from non-simultaneous XMM-Newton and NuSTAR observations, performed in 2009 and 2014, respectively. GRS1734-292 is a Seyfert 1 galaxy, located near the Galactic plane at z=0.0214z=0.0214. The NuSTAR spectrum (3−803-80 keV) is dominated by a primary power-law continuum with Γ=1.65±0.05\Gamma=1.65 \pm 0.05 and a high-energy cutoff Ec=53−8+11E_c=53^{+11}_{-8} keV, one of the lowest measured by NuSTAR in a Seyfert galaxy. Comptonization models show a temperature of the coronal plasma of kTe=11.9−0.9+1.2kT_e=11.9^{+1.2}_{-0.9} keV and an optical depth, assuming a slab geometry, τ=2.98−0.19+0.16\tau=2.98^{+0.16}_{-0.19} or a similar temperature and τ=6.7−0.4+0.3\tau=6.7^{+0.3}_{-0.4} assuming a spherical geometry. The 2009 XMM-Newton spectrum is well described by a flatter intrinsic continuum (Γ=1.47−0.03+0.07\Gamma=1.47^{+0.07}_{-0.03}) and one absorption line due to Fe\textsc{XXV} Kα\alpha produced by a warm absorber. Both data sets show a modest iron Kα\alpha emission line at 6.46.4 keV and the associated Compton reflection, due to reprocessing from neutral circumnuclear material

    Investigating the evolution of the dual AGN system ESO~509-IG066

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    We analyze the evolution of the dual AGN in ESO 509-IG066, a galaxy pair located at z=0.034 whose nuclei are separated by 11 kpc. Previous observations with XMM-Newton on this dual AGN found evidence for two moderately obscured (NH∼1022N_H\sim10^{22} cm−2^{-2}) X-ray luminous (LX∼1043L_X\sim10^{43} erg/s) nuclear sources. We present an analysis of subsequent Chandra, NuSTAR and Swift/XRT observations that show one source has dropped in flux by a factor of 10 between 2004 and 2011, which could be explained by either an increase in the absorbing column or an intrinsic fading of the central engine possibly due to a decrease in mass accretion. Both of these scenarios are predicted by galaxy merger simulations. The source which has dropped in flux is not detected by NuSTAR, which argues against absorption, unless it is extreme. However, new Keck/LRIS optical spectroscopy reveals a previously unreported broad H-alpha line which is highly unlikely to be visible under the extreme absorption scenario. We therefore conclude that the black hole in this nucleus has undergone a dramatic drop in accretion rate. From AO-assisted near-infrared integral-field spectroscopy of the other nucleus, we find evidence that the galaxy merger is having a direct effect on the kinematics of the gas close to the nucleus of the galaxy, providing a direct observational link between the galaxy merger and the mass accretion rate on to the black hole.Comment: Accepted for publication in Ap

    Measuring the Obscuring Column of a Disk Megamaser AGN in a Nearby Merger

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    Active galactic nuclei (AGNs) hosting disk water megamasers are well known to be obscured by large amounts of gas, likely due to the presence along the line of sight of an almost edge-on disky structure orbiting the supermassive black hole. Correcting for the high obscuration is crucial to infer parameters intrinsic to the source, like its luminosity. We present a broadband X-ray spectral analysis of a water megamaser AGN in an early merger (NGC 5765B), combining Chandra and NuSTAR data. NGC 5765B is highly Compton-thick and reflection-dominated, following the general trend among disk megamasers. Combining the exquisite black hole mass from masers with our X-ray spectroscopy, the Eddington ratio of the megamaser is estimated to be in the 2%–14% range, and its robustness is confirmed through SED fitting

    The relationship between adverse childhood experiences, coping using sex, and adult sexual coercion in non-incarcerated, community-based females

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    Adverse childhood experiences have been associated with negative outcomes in adulthood, including sexual offending. Using a cross-sectional design, we investigated whether self-reported adverse childhood experiences related to the perpetration of coercive sexual acts among 250 females recruited from the community. Furthermore, we examined whether sexualised coping mediated any potential relationship between childhood experiences and sexual coercion. A Spearman’s rank order correlation revealed no relationship between adverse childhood experiences and sexual coercion. However, adverse childhood experiences were significantly correlated with sexualised coping, which in turn was correlated with sexual coercion. Additionally, there was a significant but small indirect effect of adverse childhood experiences on sexual coercion through sexualised coping. Findings may help researchers to better understand the causal relationship between childhood experiences, sexual coping, and sexual coercion in females

    IC 751: a new changing-look AGN discovered by NuSTAR

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    We present the results of five NuSTAR observations of the type 2 active galactic nucleus (AGN) in IC 751, three of which were performed simultaneously with XMM-Newton or Swift/XRT. We find that the nuclear X-ray source underwent a clear transition from a Compton-thick (N H≃2×1024 cm−2N_{\rm\,H}\simeq 2\times 10^{24}\rm\,cm^{-2}) to a Compton-thin (N H≃4×1023 cm−2N_{\rm\,H}\simeq 4\times 10^{23}\rm\,cm^{-2}) state on timescales of ≲3\lesssim 3 months, which makes IC 751 the first changing-look AGN discovered by NuSTAR. Changes of the line-of-sight column density at a ∼2σ\sim2\sigma level are also found on a time-scale of ∼48\sim 48 hours (ΔN H∼1023 cm−2\Delta N_{\rm\,H}\sim 10^{23}\rm\,cm^{-2}). From the lack of spectral variability on timescales of ∼100\sim 100 ks we infer that the varying absorber is located beyond the emission-weighted average radius of the broad-line region, and could therefore be related either to the external part of the broad-line region or a clumpy molecular torus. By adopting a physical torus X-ray spectral model, we are able to disentangle the column density of the non-varying absorber (N H∼3.8×1023 cm−2N_{\rm\,H}\sim 3.8\times 10^{23}\rm\,cm^{-2}) from that of the varying clouds [N H∼(1−150)×1022 cm−2N_{\rm\,H}\sim(1-150)\times10^{22}\rm\,cm^{-2}], and to constrain that of the material responsible for the reprocessed X-ray radiation (N H∼6×1024 cm−2N_{\rm\,H} \sim 6 \times 10^{24}\rm\,cm^{-2}). We find evidence of significant intrinsic X-ray variability, with the flux varying by a factor of five on timescales of a few months in the 2-10 and 10-50 keV band.Comment: Accepted for publication in ApJ, 11 pages, 6 figure

    X-ray bolometric corrections for Compton-thick active galactic nuclei

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    We present X-ray bolometric correction factors, κBol\kappa_{Bol} (≡LBol/LX\equiv L_{Bol}/L_X), for Compton-thick (CT) active galactic nuclei (AGN) with the aim of testing AGN torus models, probing orientation effects, and estimating the bolometric output of the most obscured AGN. We adopt bolometric luminosities, LBolL_{Bol}, from literature infrared (IR) torus modeling and compile published intrinsic 2--10 keV X-ray luminosities, LXL_{X}, from X-ray torus modeling of NuSTAR data. Our sample consists of 10 local CT AGN where both of these estimates are available. We test for systematic differences in κBol\kappa_{Bol} values produced when using two widely used IR torus models and two widely used X-ray torus models, finding consistency within the uncertainties. We find that the mean κBol\kappa_{Bol} of our sample in the range LBol≈1042−1045L_{Bol}\approx10^{42}-10^{45} erg/s is log10κBol=1.44±0.12_{10}\kappa_{Bol}=1.44\pm0.12 with an intrinsic scatter of ∼0.2\sim0.2 dex, and that our derived κBol\kappa_{Bol} values are consistent with previously established relationships between κBol\kappa_{Bol} and LBolL_{Bol} and κBol\kappa_{Bol} and Eddington ratio. We investigate if κBol\kappa_{Bol} is dependent on NHN_H by comparing our results on CT AGN to published results on less-obscured AGN, finding no significant dependence. Since many of our sample are megamaser AGN, known to be viewed edge-on, and furthermore under the assumptions of AGN unification whereby unobscured AGN are viewed face-on, our result implies that the X-ray emitting corona is not strongly anisotropic. Finally, we present κBol\kappa_{Bol} values for CT AGN identified in X-ray surveys as a function of their observed LXL_X, where an estimate of their intrinsic LXL_{X} is not available, and redshift, useful for estimating the bolometric output of the most obscured AGN across cosmic time.Comment: Accepted for publication in Ap

    A Hard Look at NGC 5347: Revealing a Nearby Compton-thick AGN

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    Current measurements show that the observed fraction of Compton-thick (CT) active galactic nuclei (AGN) is smaller than the expected values needed to explain the cosmic X-ray background. Prior fits to the X-ray spectrum of the nearby Seyfert-2 galaxy NGC 5347 (z = 0.00792, D = 35.5 Mpc ) have alternately suggested a CT and Compton-thin source. Combining archival data from Suzaku, Chandra, and—most importantly—new data from NuSTAR, ... See full text for complete abstrac

    Optical, near-IR and sub-mm IFU Observations of the nearby dual AGN Mrk 463

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    We present optical and near-IR Integral Field Unit (IFU) and ALMA band 6 observations of the nearby dual Active Galactic Nuclei (AGN) Mrk 463. At a distance of 210 Mpc, and a nuclear separation of ∼\sim4 kpc, Mrk 463 is an excellent laboratory to study the gas dynamics, star formation processes and supermassive black hole (SMBH) accretion in a late-stage gas-rich major galaxy merger. The IFU observations reveal a complex morphology, including tidal tails, star-forming clumps, and emission line regions. The optical data, which map the full extent of the merger, show evidence for a biconical outflow and material outflowing at >>600 km s−1^{-1}, both associated with the Mrk 463E nucleus, together with large scale gradients likely related to the ongoing galaxy merger. We further find an emission line region ∼\sim11 kpc south of Mrk 463E that is consistent with being photoionized by an AGN. Compared to the current AGN luminosity, the energy budget of the cloud implies a luminosity drop in Mrk 463E by a factor 3-20 over the last 40,000 years. The ALMA observations of 12^{12}CO(2-1) and adjacent 1mm continuum reveal the presence of ∼\sim109^{9}M⊙_\odot in molecular gas in the system. The molecular gas shows velocity gradients of ∼\sim800 km/s and ∼\sim400 km/s around the Mrk 463E and 463W nuclei, respectively. We conclude that in this system the infall of ∼\sim100s M⊙M_\odot/yr of molecular gas is in rough balance with the removal of ionized gas by a biconical outflow being fueled by a relatively small, <<0.01% of accretion onto each SMBH.Comment: Accepted by The Astrophysical Journal, 23 pages, 19 figure
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