2011A&A...530A.149Y


Query : 2011A&A...530A.149Y

2011A&A...530A.149Y - Astronomy and Astrophysics, volume 530A, 149-149 (2011/6-1)

Study of LINER sources with broad Hα emission X-ray properties and comparison to luminous AGN and X-ray binaries.

YOUNES G., PORQUET D., SABRA B. and REEVES J.N.

Abstract (from CDS):

An important number of multiwavelength studies of low ionization nuclear emission-line regions (LINERs) were dedicated to investigate the excitation mechanism responsible for the detected emission lines. Radiative emission from accretion into a super massive black hole (SMBH) is now believed to be, in an increasing number of LINERs, the source of excitation. However, the accretion mode is not yet firmly understood, and could be explained in either a thin accretion disk or a radiatively inefficient accretion flow (RIAF). Our purpose is to study the X-ray properties of LINER sources with definite detection of a broad Hα emission line in their optical spectra, LINER 1s from Ho et al. sample. These objects preferentially harbor a low luminosity active nucleus at the center and show small or no intrinsic absorption (≤1022cm–1). We compare their X-ray properties to both X-ray binaries and luminous AGN. We analyzed all available X-ray archived [XMM-Newton and [Chandra observations of 13 LINER 1s satisfying the above criterion in a systematic homogeneous way. We looked for any correlations between the X-ray properties and the intrinsic parameters of our sample of LINER 1s. An absorbed power-law gave a good fit to the spectra of 9 out of the 13 sources in our sample. A combination of a thermal component and an absorbed power-law were required in the remaining 4 sources. We found a photon index for our sample between 1.3±0.2 for the hardest source and 2.4+0.2–0.3 for the softest one with a mean value of 1.9±0.2 and a dispersion σ=0.3. The thermal component had a mean temperature kT≃0.6keV. Significant short (hours to days) time-scale variability is not common in the present sample and was observed in only 2 sources (NGC 3226 and NGC 4278). Three other sources indicate a possible variability with a low K-S test probability (2-4%) that the nuclear emission originates from a constant source. On the other hand, significant variability on a longer time-scale (months to years) is detected in 7 out of the 9 sources observed more than once. No significant Fe Kα emission line at 6.4keV was detected and upper limits were derived for the 4 sources with a high enough signal to noise ratio around 6keV. Finally, we established, for the first time for a sample of LINER 1s, that the photon index Γ is significantly anticorrelated to L2–10keV/LEdd. Whereas this anticorrelation is in contrast to the positive correlation found for type 1 AGN, it is similar to the one seen in XRBs in their low/hard state where a radiatively inefficient accretion flow is thought to be responsible for the X-ray emitted energy.

Abstract Copyright:

Journal keyword(s): accretion, accretion disks - galaxies: active - galaxies: nuclei - X-rays: galaxies

Simbad objects: 27

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Number of rows : 27
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2023
#notes
1 NGC 22 GiG 00 09 48.2026917744 +27 49 56.127280584   14.9       ~ 41 0
2 NGC 112 GiG 00 26 48.7498157664 +31 42 11.978411760   14.5       ~ 49 0
3 NGC 266 LIN 00 49 47.8149787992 +32 16 39.786194928 12.98 12.54 11.63     ~ 179 2
4 NGC 315 LIN 00 57 48.88334410 +30 21 08.8119345 12.80 12.20 11.16 11.26   ~ 760 2
5 NGC 1052 GiP 02 41 04.79849989 -08 15 20.7519527 11.84 11.41 10.47 10.71   ~ 1261 2
6 NGC 1097 LIN 02 46 19.059 -30 16 29.68 10.46 9.97 9.48 8.72 9.8 ~ 1288 3
7 NGC 2681 LIN 08 53 32.7183058512 +51 18 49.159212120 11.40 11.09 10.29     ~ 312 1
8 NGC 2787 LIN 09 19 18.6046606656 +69 12 11.630716128   12.92 11.79     ~ 337 0
9 M 81 Sy2 09 55 33.1726556496 +69 03 55.062505368   7.89 6.94     ~ 4284 3
10 CXOU J102326.7+195407 X 10 23 26.7 +19 54 07           ~ 4 0
11 NGC 3226 GiP 10 23 27.0064075320 +19 53 54.674937420   14.32 13.33     ~ 414 1
12 CXOU J102334.1+195347 X 10 23 34.1 +19 53 47           ~ 3 0
13 V* KV UMa HXB 11 18 10.7930420496 +48 02 12.314730120     12.25     K5V-M1V 788 0
14 NGC 3642 LIN 11 22 17.9010437568 +59 04 28.275641436   14.86 14.04     ~ 198 0
15 NGC 3718 GiP 11 32 34.8571790688 +53 04 04.520222040   11.35 10.61     ~ 370 1
16 Mrk 176 Sy2 11 32 40.2448971432 +52 57 01.289256768   15.50 14.61 13.52   ~ 232 2
17 NGC 3998 SyG 11 57 56.1334044408 +55 27 12.922443432   11.64 12.10 10.09   ~ 619 2
18 NGC 4143 LIN 12 09 36.0679174440 +42 32 03.031963368   13.04 12.08     ~ 225 0
19 NGC 4203 LIN 12 15 05.0549203560 +33 11 50.383965120   12.98 11.99     ~ 479 2
20 M 106 Sy2 12 18 57.620 +47 18 13.39   9.14 8.41 8.11   ~ 2282 3
21 NGC 4278 LIN 12 20 06.82538739 +29 16 50.7134758 11.54 11.09 10.16     ~ 921 2
22 M 58 SyG 12 37 43.597 +11 49 05.12 10.80 10.48 9.66     ~ 1042 2
23 NGC 4636 LIN 12 42 49.8333280080 +02 41 15.951929028   12.62 11.84     ~ 1096 1
24 NGC 4750 LIN 12 50 07.3113940944 +72 52 28.653179520   11.8       ~ 131 0
25 NGC 4772 LIN 12 53 29.1636448512 +02 10 06.146331708 12.29 11.96 11.04     ~ 241 1
26 NGC 5005 GiP 13 10 56.312 +37 03 32.19   14.67 13.67     ~ 527 2
27 NGC 7213 Sy1 22 09 16.2100443720 -47 10 00.115999716   10.97 12.08 10.50 10.6 ~ 635 0

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2023.03.26-15:05:51

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