199 research outputs found

    The soft X-ray polarization in obscured AGN

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    The soft X-ray emission in obscured active galactic nuclei (AGN) is dominated by emission lines, produced in a gas photoionized by the nuclear continuum and likely spatially coincident with the optical narrow line region (NLR). However, a fraction of the observed soft X-ray flux appears like a featureless power law continuum. If the continuum underlying the soft X-ray emission lines is due to Thomson scattering of the nuclear radiation, it should be very highly polarized. We calculated the expected amount of polarization assuming a simple conical geometry for the NLR, combining these results with the observed fraction of the reflected continuum in bright obscured AGN.Comment: 6 pages, 3 figures, to appear in 'X-ray Polarimetry: A New Window in Astrophysics', edited by R. Bellazzini, E. Costa, G. Matt and G. Tagliaferr

    Spatially resolved Fe K spectroscopy of NGC 4945

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    We present the imaging and spectroscopic analysis of the combined Chandra ACIS-S observations of the Compton-thick Seyfert 2 galaxy NGC 4945. We performed a spatially-resolved spectroscopy of the circumnuclear environment of the source, picturing the innermost 200 parsecs around the highly absorbed nucleus. The additional 200 ks ACIS-S data with respect to the previous campaign allowed us to map with even greater detail the central structure of this source and to discover an enhanced iron emission in the innermost nuclear region, with respect to the associated Compton reflection continuum. We revealed that the Equivalent Width of the iron Kα\alpha line is spatially variable (ranging from 0.5 to 3 keV), on scales of tens of parsecs, likely due to the ionization state and orientation effects of the reprocessing material, with respect to the central X-ray illuminating source. A clump of highly ionized Fe XXV He-α\alpha is also detected, 40 parsecs east to the nucleus. When observations taken years apart are considered, the central unresolved reflected emission is found to remain constant.Comment: 10 pages, 6 figures, 4 tables, accepted for publication in MNRA

    The NuSTAR view of the Seyfert Galaxy HE 0436-4717

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    We present the multi epoch spectral analysis of HE 0436-4717, a bright Seyfert 1 galaxy serendipitously observed by the high energy satellite NuSTAR four times between December 2014 and December 2015. The source flux shows modest variability within each pointing and among the four observations. Spectra are well modelled in terms of a weakly variable primary power law with constant photon index (Γ\Gamma=2.01±\pm0.08). A constant narrow \ion{Fe} Kα\alpha emission line suggests that this feature has an origin far from the central black hole, while a broad relativistic component is not required by the data. The Compton reflection component is also constant in flux with a corresponding reflection fraction R=0.70.3+0.2^{+0.2}_{-0.3}. The iron abundance is compatible with being Solar (AFe_{Fe}=1.20.4+1.4^{+1.4}_{-0.4}), and a lower limit for the high energy cut-off Ec_c>280 keV is obtained. Adopting a self-consistent model accounting for a primary Comptonized continuum, we obtain a lower limit for the hot corona electron temperature kTe_e>65 keV and a corresponding upper limit for the coronal optical depth of τe\tau_e<1.3. The results of the present analysis are consistent with the locus of local Seyfert galaxies in the kTe_e-τe\tau_e and temperature-compactness diagrams.Comment: accepted for publication in A&

    HST unveils a compact mildly relativistic Broad Line Region in the candidate true type 2 NGC 3147

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    NGC 3147 has been considered the best case of a true type 2 AGN: an unobscured AGN, based on the unabsorbed compact X-ray continuum, which lacks a broad line region (BLR). However, the very low luminosity of NGC 3147 implies a compact BLR, which produces very broad lines, hard to detect against the dominant background host galaxy. Narrow (0.1"x0.1") slit HST spectroscopy allowed us to exclude most of the host galaxy light, and revealed an Hα\alpha line with an extremely broad base (FWZI27000\sim27\,000 km s1^{-1}). The line profile shows a steep cutoff blue wing and an extended red wing, which match the signature of a mildly relativistic thin accretion disk line profile. It is indeed well fit with a nearly face on thin disk, at i23i\sim23^\circ, with an inner radius at 77±1577\pm15 rg_g, which matches the prediction of 6214+1862^{+18}_{-14} rg_g from the RBLRL1/2R_{\rm BLR} \sim L^{1/2} relation. This result questions the very existence of true type 2 AGN. Moreover, the detection of a thin disk, which extends below 100 rg_g in an L/LEdd104L/L_{\rm Edd}\sim10^{-4} system, contradicts the current view of the accretion flow configuration at extremely low accretion rates.Comment: 6 pages, 3 figures, accepted for publication in MNRAS Letter

    Towards precision tests of general relativity with black hole X-ray reflection spectroscopy

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    Astrophysical black hole systems are the ideal laboratories for testing Einstein's theory of gravity in the strong field regime. We have recently developed a framework which uses the reflection spectrum of black hole systems to perform precision tests of general relativity by testing the Kerr black hole hypothesis. In this paper, we analyze XMM-Newton and NuSTAR observations of the supermassive black hole in the Seyfert 1 galaxy MCG-06-30-15 with our disk reflection model. We consider the Johannsen metric with the deformation parameters α13\alpha_{13} and α22\alpha_{22}, which quantify deviations from the Kerr metric. For α22=0\alpha_{22} = 0, we obtain the black hole spin 0.928<a<0.9830.928 < a_* < 0.983 and 0.44<α13<0.15-0.44 < \alpha_{13} < 0.15. For α13=0\alpha_{13} = 0, we obtain 0.885<a<0.9870.885 < a_* < 0.987 and 0.12<α22<1.05-0.12 < \alpha_{22} < 1.05. The Kerr solution is recovered for α13=α22=0\alpha_{13} = \alpha_{22} = 0. Thus, our results include the Kerr solution within statistical uncertainties. Systematic uncertainties are difficult to account for, and we discuss some issues in this regard.Comment: 10 pages, 7 figures. v2: title slightly changed, arXiv version shorter than published versio

    NGC 2992: The interplay between the multiphase disk, wind and radio bubbles

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    We present an analysis of the gas kinematics in NGC 2992, based on VLT/MUSE, ALMA and VLA data, aimed at characterising the disk, the wind and their interplay in the cold molecular and warm ionised phases. CO(2-1) and Hα \rm \alpha~ arise from a multiphase disk with inclination 80 deg and radii 1.5 and 1.8 kpc, respectively. We find that the velocity dispersion of the cold molecular phase is consistent with that of star forming galaxies at the same redshift, except in the inner 600 pc region, and in the region between the cone walls and the disk. This suggests that a disk-wind interaction locally boosts the gas turbulence. We detect a clumpy ionised wind distributed in two wide opening angle ionisation cones reaching scales of 7 kpc. The [O III] wind expands with velocity exceeding -1000 km/s in the inner 600 pc, a factor of 5 larger than the previously reported wind velocity. Based on spatially resolved electron density and ionisation parameter maps, we infer an ionised outflow mass of Mof,ion=(3.2±0.3)×107MM_{\rm of,ion} = (3.2 \pm 0.3) \times \, 10^7 \, M_{\odot}, and a total ionised outflow rate of M˙of,ion=13.5±1\dot M_{\rm of,ion}=13.5\pm1 \sfr. We detected clumps of cold molecular gas located above and below the disk reaching maximum projected distances and velocities of 1.7 kpc and 200 km/s, respectively. On these scales, the wind is multiphase, with a fast ionised component and a slower molecular one, and a total mass of Mof,ion+mol=5.8×107MM_{\rm of, ion+mol}= 5.8 \times 10^7 \, M_{\odot}, of which the molecular component carries the bulk of the mass. The dusty molecular outflowing clumps and the turbulent ionised gas are located at the edges of the radio bubbles, suggesting that the bubbles interact with the surrounding medium through shocks. We detect a dust reservoir co-spatial with the molecular disk, with a cold dust mass Mdust=(4.04±0.03)×106MM_{\rm dust} = (4.04 \pm 0.03) \times \, 10^{6} \, M_{\odot}.Comment: 19 pages, 17 figures, 6 tables; Accepted by A&
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