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X-ray and radio variability in the low-luminosity active galactic nucleus NGC 7213

Identifieur interne : 001474 ( PascalFrancis/Checkpoint ); précédent : 001473; suivant : 001475

X-ray and radio variability in the low-luminosity active galactic nucleus NGC 7213

Auteurs : M. E. Bell [Royaume-Uni] ; T. Tzioumis [Australie] ; P. Uttley [Royaume-Uni] ; R. P. Fender [Royaume-Uni] ; P. Arevalo [Allemagne, Chili] ; E. Breedt [Royaume-Uni] ; I. Mchardy [Royaume-Uni] ; D. E. Calvelo [Royaume-Uni] ; O. Jamil [Royaume-Uni] ; E. Körding [France]

Source :

RBID : Pascal:11-0081189

Descripteurs français

English descriptors

Abstract

We present the results of a ˜3 yr campaign to monitor the low-luminosity active galactic nucleus (LLAGN) NGC 7213 in the radio (4.8 and 8.4 GHz) and X-ray bands (2-10 keV). With a reported X-ray Eddington ratio of 7 x 10-4LEdd, NGC 7213 can be considered to be comparable to a hard-state black hole X-ray binary. We show that a weak correlation exists between the X-ray and radio light curves. We use the cross-correlation function to calculate a global time-lag between events in the X-ray and radio bands to be 24 ± 12 d lag (8.4 GHz radio lagging X-ray) and 40 ± 13 d lag (4.8 GHz radio lagging X-ray), respectively. The radio-radio light curves are extremely well correlated with a lag of 20.5 ± 12.9 d (4.8 GHz lagging 8.4 GHz). We explore the previously established scaling relationship between core radio and X-ray luminosities and black hole mass LR W0.6-0.8L0.6X, known as the 'Fundamental Plane of black hole activity', and show that NGC 7213 lies very close to the best-fitting 'global' correlation for the plane as one of the most-luminous LLAGNs. With a large number of quasi-simultaneous radio and X-ray observations, we explore for the first time the variations of a single AGN with respect to the Fundamental Plane. Although the average radio and X-ray luminosities for NGC 7213 are in good agreement with the Plane, we show that there is intrinsic scatter with respect to the Plane for the individual data points.


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Le document en format XML

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<div type="abstract" xml:lang="en">We present the results of a ˜3 yr campaign to monitor the low-luminosity active galactic nucleus (LLAGN) NGC 7213 in the radio (4.8 and 8.4 GHz) and X-ray bands (2-10 keV). With a reported X-ray Eddington ratio of 7 x 10
<sup>-4</sup>
L
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W
<sup>0.6-0.8</sup>
L
<sup>0.6</sup>
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<s2>Highfield, Southampton SO17 1BJ</s2>
<s3>GBR</s3>
<sZ>1 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>7 aut.</sZ>
<sZ>8 aut.</sZ>
<sZ>9 aut.</sZ>
</fA14>
<fA14 i1="02">
<s1>Australia Telescope National Facility, CSIRO</s1>
<s2>Marsfield, NSW 2122</s2>
<s3>AUS</s3>
<sZ>2 aut.</sZ>
</fA14>
<fA14 i1="03">
<s1>Max-Planck-Institut für Astrophysik, Karl-Schwarzschild-Strasse 1</s1>
<s2>85741 Garching</s2>
<s3>DEU</s3>
<sZ>5 aut.</sZ>
</fA14>
<fA14 i1="04">
<s1>Departamento de Ciencias Fisicas, Universidad Andres Bello, Av. Republica 252</s1>
<s2>Santiago</s2>
<s3>CHL</s3>
<sZ>5 aut.</sZ>
</fA14>
<fA14 i1="05">
<s1>Department of Physics, University of Warwick, Gibbet Hill Road</s1>
<s2>Coventry CV4 7AL</s2>
<s3>GBR</s3>
<sZ>6 aut.</sZ>
</fA14>
<fA14 i1="06">
<s1>AIM/CEA Saclay and University Paris Diderot, l'Orme des Merisers</s1>
<s2>91219 Gif-sur-vette</s2>
<s3>FRA</s3>
<sZ>10 aut.</sZ>
</fA14>
<fA20>
<s1>402-410</s1>
</fA20>
<fA21>
<s1>2011</s1>
</fA21>
<fA23 i1="01">
<s0>ENG</s0>
</fA23>
<fA43 i1="01">
<s1>INIST</s1>
<s2>2067</s2>
<s5>354000193526170350</s5>
</fA43>
<fA44>
<s0>0000</s0>
<s1>© 2011 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45>
<s0>3/4 p.</s0>
</fA45>
<fA47 i1="01" i2="1">
<s0>11-0081189</s0>
</fA47>
<fA60>
<s1>P</s1>
</fA60>
<fA61>
<s0>A</s0>
</fA61>
<fA64 i1="01" i2="1">
<s0>Monthly Notices of the Royal Astronomical Society</s0>
</fA64>
<fA66 i1="01">
<s0>USA</s0>
</fA66>
<fC01 i1="01" l="ENG">
<s0>We present the results of a ˜3 yr campaign to monitor the low-luminosity active galactic nucleus (LLAGN) NGC 7213 in the radio (4.8 and 8.4 GHz) and X-ray bands (2-10 keV). With a reported X-ray Eddington ratio of 7 x 10
<sup>-4</sup>
L
<sub>Edd</sub>
, NGC 7213 can be considered to be comparable to a hard-state black hole X-ray binary. We show that a weak correlation exists between the X-ray and radio light curves. We use the cross-correlation function to calculate a global time-lag between events in the X-ray and radio bands to be 24 ± 12 d lag (8.4 GHz radio lagging X-ray) and 40 ± 13 d lag (4.8 GHz radio lagging X-ray), respectively. The radio-radio light curves are extremely well correlated with a lag of 20.5 ± 12.9 d (4.8 GHz lagging 8.4 GHz). We explore the previously established scaling relationship between core radio and X-ray luminosities and black hole mass L
<sub>R</sub>
W
<sup>0.6-0.8</sup>
L
<sup>0.6</sup>
<sub>X</sub>
, known as the 'Fundamental Plane of black hole activity', and show that NGC 7213 lies very close to the best-fitting 'global' correlation for the plane as one of the most-luminous LLAGNs. With a large number of quasi-simultaneous radio and X-ray observations, we explore for the first time the variations of a single AGN with respect to the Fundamental Plane. Although the average radio and X-ray luminosities for NGC 7213 are in good agreement with the Plane, we show that there is intrinsic scatter with respect to the Plane for the individual data points.</s0>
</fC01>
<fC02 i1="01" i2="3">
<s0>001E03</s0>
</fC02>
<fC03 i1="01" i2="X" l="FRE">
<s0>Variabilité</s0>
<s5>26</s5>
</fC03>
<fC03 i1="01" i2="X" l="ENG">
<s0>Variability</s0>
<s5>26</s5>
</fC03>
<fC03 i1="01" i2="X" l="SPA">
<s0>Variabilidad</s0>
<s5>26</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE">
<s0>Luminosité</s0>
<s5>27</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG">
<s0>Luminosity</s0>
<s5>27</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE">
<s0>Noyau galactique actif</s0>
<s5>28</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG">
<s0>Active galaxy nuclei</s0>
<s5>28</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE">
<s0>Trou noir</s0>
<s5>29</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG">
<s0>Black holes</s0>
<s5>29</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE">
<s0>Binaire RX</s0>
<s5>30</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG">
<s0>X-ray binary stars</s0>
<s5>30</s5>
</fC03>
<fC03 i1="06" i2="X" l="FRE">
<s0>Source RX binaire</s0>
<s5>31</s5>
</fC03>
<fC03 i1="06" i2="X" l="ENG">
<s0>Binary X ray source</s0>
<s5>31</s5>
</fC03>
<fC03 i1="06" i2="X" l="SPA">
<s0>Fuente RX binaria</s0>
<s5>31</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE">
<s0>Corrélation croisée</s0>
<s5>32</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG">
<s0>Cross correlations</s0>
<s5>32</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE">
<s0>Courbe lumière</s0>
<s5>33</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG">
<s0>Light curves</s0>
<s5>33</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE">
<s0>Fonction corrélation</s0>
<s5>34</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG">
<s0>Correlation functions</s0>
<s5>34</s5>
</fC03>
<fC03 i1="10" i2="X" l="FRE">
<s0>Observation RX</s0>
<s5>35</s5>
</fC03>
<fC03 i1="10" i2="X" l="ENG">
<s0>X ray observation</s0>
<s5>35</s5>
</fC03>
<fC03 i1="10" i2="X" l="SPA">
<s0>Observación RX</s0>
<s5>35</s5>
</fC03>
<fC03 i1="11" i2="X" l="FRE">
<s0>Variation temporelle</s0>
<s5>36</s5>
</fC03>
<fC03 i1="11" i2="X" l="ENG">
<s0>Time variation</s0>
<s5>36</s5>
</fC03>
<fC03 i1="11" i2="X" l="SPA">
<s0>Variación temporal</s0>
<s5>36</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE">
<s0>Disque accrétion</s0>
<s5>37</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG">
<s0>Accretion disks</s0>
<s5>37</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE">
<s0>Galaxies actives</s0>
<s5>38</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG">
<s0>Active galaxies</s0>
<s5>38</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE">
<s0>Noyau galaxies</s0>
<s5>39</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG">
<s0>Galaxy nuclei</s0>
<s5>39</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE">
<s0>Cosmologie</s0>
<s5>40</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG">
<s0>Cosmology</s0>
<s5>40</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE">
<s0>Source RX cosmique</s0>
<s5>41</s5>
</fC03>
<fC03 i1="16" i2="3" l="ENG">
<s0>Cosmic x-ray sources</s0>
<s5>41</s5>
</fC03>
<fN21>
<s1>052</s1>
</fN21>
<fN44 i1="01">
<s1>OTO</s1>
</fN44>
<fN82>
<s1>OTO</s1>
</fN82>
</pA>
</standard>
</inist>
<affiliations>
<list>
<country>
<li>Allemagne</li>
<li>Australie</li>
<li>Chili</li>
<li>France</li>
<li>Royaume-Uni</li>
</country>
</list>
<tree>
<country name="Royaume-Uni">
<noRegion>
<name sortKey="Bell, M E" sort="Bell, M E" uniqKey="Bell M" first="M. E." last="Bell">M. E. Bell</name>
</noRegion>
<name sortKey="Breedt, E" sort="Breedt, E" uniqKey="Breedt E" first="E." last="Breedt">E. Breedt</name>
<name sortKey="Calvelo, D E" sort="Calvelo, D E" uniqKey="Calvelo D" first="D. E." last="Calvelo">D. E. Calvelo</name>
<name sortKey="Fender, R P" sort="Fender, R P" uniqKey="Fender R" first="R. P." last="Fender">R. P. Fender</name>
<name sortKey="Jamil, O" sort="Jamil, O" uniqKey="Jamil O" first="O." last="Jamil">O. Jamil</name>
<name sortKey="Mchardy, I" sort="Mchardy, I" uniqKey="Mchardy I" first="I." last="Mchardy">I. Mchardy</name>
<name sortKey="Uttley, P" sort="Uttley, P" uniqKey="Uttley P" first="P." last="Uttley">P. Uttley</name>
</country>
<country name="Australie">
<noRegion>
<name sortKey="Tzioumis, T" sort="Tzioumis, T" uniqKey="Tzioumis T" first="T." last="Tzioumis">T. Tzioumis</name>
</noRegion>
</country>
<country name="Allemagne">
<noRegion>
<name sortKey="Arevalo, P" sort="Arevalo, P" uniqKey="Arevalo P" first="P." last="Arevalo">P. Arevalo</name>
</noRegion>
</country>
<country name="Chili">
<noRegion>
<name sortKey="Arevalo, P" sort="Arevalo, P" uniqKey="Arevalo P" first="P." last="Arevalo">P. Arevalo</name>
</noRegion>
</country>
<country name="France">
<noRegion>
<name sortKey="Kording, E" sort="Kording, E" uniqKey="Kording E" first="E." last="Körding">E. Körding</name>
</noRegion>
</country>
</tree>
</affiliations>
</record>

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