AGN component in Deep Radio Fields

AGN component in Deep Radio Fields
Alessandro Maini
co-tutelle PhD student
Dipartimento di Fisica e Astronomia
Università di Bologna
&
Istituto di Radio Astronomia
INAF
Department of Physics and Astronomy
Macquarie University
&
Astronomy & Space Science Division
CSIRO
Main collaborators
Giovannini G.
Prandoni I.
Parker Q. A.
Norris R. P.
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AGN component in Deep Radio Fields
Outline
Deep Radio Surveys and AGN component
Focus on two populations:
I - Radio-Quiet AGNs (RQ AGN)
II - Infrared-Faint Radio Sources (IFRS)
Future Perspectives
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Deep Radio Surveys and AGN component
The current picture
S1.4 GHz down to ∼ 10 µJy
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adapted from Norris R. P., 2012
(Proc. IAU Symp. 284, 2011, 489)
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Deep Radio Surveys and AGN component
AGN Population decline
Seymour et al., 2008
(MNRAS 386, 1695)
S1.4 GHz
∼ 1 µJy
∼ 100 µJy
∼ 1 mJy
∼ 10 mJy
AGN
. 10%
∼ 30–40%
∼ 80–90%
& 99%
∼ 90%
∼ 60–70%
. 20%
SFG
Wilman et al. (2008)
model
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. 1%
Windhorst et al., 1990
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Deep Radio Surveys and AGN component
AGN count
Steady decline of
Radio Galaxies and RL AGN
flattening below 1 mJy due to
RQ AGN
Smolˇci´c et al. 2014
(PoS AASKA14 069)
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I - Radio-Quiet AGN
A new component
adapted from Czerny B. et al., 2005
found in samples selected in
X-ray, optical and MIR-bands
(until recently!)
radio emission
negligible part
of the bolometric luminosity
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Sradio
Soptical
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∼ 10
6 / 24
I - Radio-Quiet AGN
A new component
Bonzini et al., 2013
MNRAS 436, 3759
S1.4 GHz
∼ 1 µJy
∼ 100 µJy
∼ 1 mJy
∼ 10 mJy
RL AGN
. 10%
. 30%
∼ 80–90%
& 99%
RQ AGN
∼ 20%
∼ 20%
. 10%
1%
SFG
∼ 70%
. 50%
. 10%
. 1%
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I - Radio-Quiet AGN
Open issues
The origin of the radio emission in deep-field RQ AGNs is still matter of debate:
scaled down version of RL AGNs?
(Miller et al. 1993; Giroletti & Panessa 2009; Prandoni et al. 2010, Jarvis & Rawlings 2004)
ongoing star formation activity in the host galaxy?
(Sopp & Alexander 1991; Padovani et al. 2011; Bonzini et al. 2013)
mixed contribution from AGN and SF processes to the total radio emission?
(Daddi et al. 2007; Gruppioni et al. 2011; Del Moro et al. 2013)
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I - Radio-Quiet AGN
Implications
Disentangling the origin of the radio emission in RQ AGNs would have relevant
implications on general topics like:
triggering mechanism of AGN radio activity and its duty cycle;
role played by low-accretion/radiative efficiency AGN activity in the global black
hole accretion history of the Universe;
relative contribution of radiative versus jet-driven (kinetic) feedback to the global
AGN feedback in galaxy formation and evolution models.
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I - Radio-Quiet AGN
The project: searching for a compact radio core
P.I.:
Co.I.:
Maini A.
Prandoni I.
Norris R. P.
Giovannini G.
Parker Q. A.
Extended Chandra Deep Field South (E-CDFS)
7 RQ AGNs
9 RL AGNs
(flux densities 200–400 µJy)
Completed 20.5 h of the requested 72 h
Australian LBA
+
Data reduction:
ongoing...
ASKAP
resolution .20 mas
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II - Infrared-Faint Radio Sources
Serendipitously identified by Norris et al. (2006) and Middelberg et al. (2008)
cross-matching catalogues of:
Australia Telescope Large Area Survey (ATLAS)
5σ sensitivity limit: ∼0.2 mJy at 1.4 GHz
Spitzer Wide-area IR Extragalactic Survey (SWIRE)
5σ sensitivity limits: 3.7 µJy at 3.6 µm (IRAC bands)
5.4 µJy at 4.5 µm
48 µJy at 5.8 µm
37.8 µJy at 8.0 µm
0.23 mJy at 24 µm (MIPS bands)
18 mJy at 70 µm
150 mJy at 160 µm
in the CDFS and in the ELAIS-S1 deep fields
All ATLAS source was expected to have SWIRE counterpart within z ∼ 2
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II - Infrared-Faint Radio Sources
∼50 sources were undetected at
ANY SWIRE band
ATLAS = 0.14 → 26.08 mJy
S20cm
q24 = log
S24µm
S20cm
= 0.84 ± 0.28
Appleton et al. (2004)
No standard SFGs
Sradio /SIR more consistent with AGN
low SIR ⇒ very obscured
and/or
high redshift
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Adapted from Norris et al. 2006
(AJ 132, 2409)
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II - Infrared-Faint Radio Sources
VLBI and spectral analyses
Norris et al. (2007) & Middelberg et al. (2008):
core size < 0.030”
6
TB & 10 K
⇒
linear size . 260 pc
⇒
P1.4GHz ∼ 1025÷28 W/Hz
(z ∼ 1 ÷ 7)
⇓
RL AGN / QSO regime
IFRS ES0427
Middelberg et al. 2008 (A&A 491, 435)
ELAIS-S1 population
α
˜ 2.3
1.4 = −0.86
AGN ELAIS-S1 sample
α
˜ 2.3
1.4 = −0.82
IFRS sample
α
˜ 2.3
1.4 = −1.40
HzRG sample
α
˜ 2.3
1.4 = −1.02
⇓
Middelberg et al. 2011
(A&A 526, A8)
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High redshift
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II - Infrared-Faint Radio Sources
The sample
Spitzer Extragalactic Representative Volume Survey
(SERVS)
5σ sensitivity limits: 1.9 µJy at 3.6 µm
2.2 µJy at 4.5 µm
New selction criteria:
S1.4 GHz
S3.6µm
≥200
Field
unresolved at the SERVS PSF (1.9”)
Covered Original
From
3.6 µm band
Area Number
sources
IFRSs
2
Name
(deg )
in field detected claimed reliable
CDFS
4.5
22
Norris+ (2006)
21
8
7
4
ELAIS-S1
3.0
29
Middelberg+ (2008)
17
6
4
4
ELAIS-N1
2.0
18
Banfield+ (2011)
5
3
2
1
XMM-LSS
4.5
3
Zinn&Oliver (in prep.)
3
–
–
–
LH
4.0
21
Maini+ (sub.)
21
11
11
11
Total
93
67
28
24
20
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4.5 µm band
sources
IFRSs
in field detected claimed reliable
21
7
6
5
14
5
3
3
5
3
2
1
3
–
–
–
19
10
10
10
62
25
21
19
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II - Infrared-Faint Radio Sources
Evolutionary tracks
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II - Infrared-Faint Radio Sources
Evolutionary tracks
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II - Infrared-Faint Radio Sources
A sub-class of the RL AGNs?
Adapted from Collier et al. 2014
(MNRAS 439, 545)
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II - Infrared-Faint Radio Sources
Implications
A good assessment of IFRS nature and density would help to:
pinpont the highest-z AGN populaton in large surveys
constrain the AGN number density at high z
constrain the structure formation scenario up to the reionization epoch
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Deep Radio Surveys and AGN component
Future Perspectives
courtesy Prandoni I.
S1.4 GHz down to sub-µJy / nJy level
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AGN component in Deep Radio Fields
Thank you
for your attention
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Infrared-Faint Radio Sources
Appendices
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Infrared-Faint Radio Sources
Appendices
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Infrared-Faint Radio Sources
Appendices
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Infrared-Faint Radio Sources
Appendices
LH324
LH2633
3.6 µm
3.6 µm
4.5 µm
4.5 µm
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