Search arXiv⌕ Search

arXiv · 1405.7575

Iron K$α$ emission in type-I and type-II Active Galactic Nuclei

Abstract

The narrow Fe K$α$ line is one of the main signatures of the reprocessing of X-ray radiation from the material surrounding supermassive black holes, and it has been found to be omnipresent in the X-ray spectra of active galactic nuclei (AGN). In this work we study the characteristics of the narrow Fe K$α$ line in different types of AGN. Using the results of a large Suzaku study we find that Seyfert 2s have on average lower Fe K$α$ luminosities than Seyfert 1s for the same 10-50 keV continuum luminosity. Simulating dummy Sy1s and Sy2s populations using physical torus models of X-ray reflected emission, we find that this difference can be explained by means of different average inclination angles with respect to the torus, as predicted by the unified model. Alternative explanations include differences in the intensities of Compton humps or in the photon index distributions. We show that the ratio between the flux of the broad and narrow Fe K$α$ line in the 6.35-6.45 keV range depends on the torus geometry considered, and is on average $<25\%$ and $<15\%$ for type I and type II AGN, respectively. We find evidence of absorption of the narrow Fe K$α$ line flux in Compton-thick AGN, which suggests that part of the reflecting material is obscured. We estimate that on average in obscured AGN the reflected radiation from neutral material is seen through a column density which is 1/4 of that absorbing the primary X-ray emission. This should be taken into account in synthesis models of the CXB and when studying the luminosity function of heavily obscured AGN. We detect the first evidence of the X-ray Baldwin effect in Seyfert 2s, with the same slope as that found for Seyfert 1s, which suggests that the mechanism responsible for the decrease of the equivalent width with the continuum luminosity is the same in the two classes of objects.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Claudio Ricci, Yoshihiro Ueda, Stephane Paltani, Kohei Ichikawa, Poshak Gandhi, Hisamitsu Awaki. 2014-05-29. Iron K$α$ emission in type-I and type-II Active Galactic Nuclei. https://doi.org/10.1093/mnras%2Fstu735

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

The missing ultra-faint satellites of the Milky Way

We combine the highest resolution N-body simulation of a $\sim10^{12}M_\odot$ $Λ$CDM halo (Aquarius-A) with the semi-analytic model GALFORM to study the full satellite population of Milky Way (MW)-like galaxies. The model assumes that galaxies form only in subhalos whose peak circular velocity exceeds the hydrogen-cooling threshold, and predicts that the total number of satellites ever accreted into the main halo, down to arbitrarily low luminosity, should not exceed a few hundred. The model tracks satellites even after their halos become unresolved ("orphan" galaxies), and includes a novel treatment of dark matter and stellar tidal stripping which takes into account that $Λ$CDM subhalos survive tidal disruption because of their cuspy density profiles. Our results match the massive end of the observed MW satellite mass function and predict that many ultra-faint dwarfs (UFDs) with $M_V>-5$ are missing from the current MW satellite census. The missing UFDs are predicted to avoid the innermost regions of the host, and have properties overlapping those of the recently-discovered ultra-faint compact MW satellites (UFCSs). If the faintest dwarfs are initially as compact as UFCSs, our results suggest that many UFCSs should be dark matter-dominated dwarfs with velocity dispersions $1-3$ km/s which survived disruption because they inhabit the cusp of $Λ$CDM subhalos. UFCSs have predicted densities of $10^{10}$-$10^{11}\,M_\odot/$kpc$^3$, higher than those of more extended UFDs. If confirmed, our results provide strong support for the cuspy nature of $Λ$CDM halos and for the hydrogen-cooling threshold for galaxy formation.

astro-ph.GA↗

A Unified HI Rotation Curve Database for 122 Dwarf and Irregular Galaxies

We present a unified HI rotation curve database for 122 dwarf and irregular galaxies drawn from three Local Volume surveys, the Local Volume HI Survey (LVHIS; 32 galaxies), VLA-ANGST (29) and LITTLE THINGS (26), and from the WALLABY DR2 kinematic catalogue (35). The database provides standardised kinematic parameters, distance estimates, morphological classifications, and rotation curve data in machine-readable JSON, JSONL, and CSV formats with a documented schema, supporting retrieval-augmented generation (RAG) applications and cross-survey kinematic analysis. Quality tiers distinguish 26 galaxies with published tilted-ring rotation curves and per-point uncertainties from 96 automated-pipeline, single-ring or profile-width entries. Three worked examples demonstrate corpus queries, including evaluation of the $ω$ estimator for DDO 154 (LITTLE THINGS). This work is presented as a data resource; no new dynamical model is proposed. This version describes corpus v1.3, which corrects the LITTLE THINGS curves (v1.1), the WALLABY entries (v1.2) and the LVHIS entries and reference (v1.3) of v1.0. The database and all computation scripts are available at Zenodo (https://doi.org/10.5281/zenodo.23503221).

astro-ph.GA↗

Collisional excitation of SiC$_6$ by helium: cross sections, rate coefficients, and astrophysical implications

Rotational transitions of SiC$_6$ with $j=26$--$40$ have been detected in IRC+10216, but collisional rate coefficients for SiC$_6$ with He or H$_2$ were previously unavailable. We present rate coefficients for SiC$_6$ rotational excitation by He, calculated using a two-dimensional potential energy surface (PES) at the RCCSD(T)-F12 level under the rigid-rotor approximation. Close-coupling (CC) calculations were performed for low rotational levels, while the coupled-states (CS) method was used for higher levels. Convergence tests were conducted, and CC and CS scattering cross sections were compared. The CS rate coefficients cover rotational levels up to $j=40$ and temperatures of 3--60\,K. Although CC and CS rate coefficients differ by up to a factor of $\sim 2$ for some transitions, particularly those affected by weak coupling and resonances, they yield nearly identical excitation and brightness temperatures for the high-$j$ transitions examined, including $19\rightarrow18$. These results support the reliability of the CS method for non-LTE modelling of the high-$j$ transitions considered, for which CC calculations are computationally impractical. We use reduced-mass scaling of the SiC$_6$--He rate coefficients to estimate those for SiC$_6$--H$_2$ and model the observed transitions. A $χ^2$ analysis of the observed line fluxes, excluding heavily blended features, yields a best-fitting of $n(\mathrm{H_2})=4.33\times10^5$\,cm$^{-3}$ and $N(\mathrm{SiC_6})=8.11\times10^{11}$\,cm$^{-2}$. The latter agrees excellently with the previous observational estimate of $(7.9\pm1.5)\times10^{11}$\,cm$^{-2}$, supporting the consistency of our non-LTE modelling with observational constraints.

astro-ph.GA↗