2011ApJ...743..122A


Query : 2011ApJ...743..122A

2011ApJ...743..122A - Astrophys. J., 743, 122 (2011/December-3)

Ultra steep spectrum radio sources in the Lockman Hole: SERVS identifications and redshift distribution at the faintest radio fluxes.

AFONSO J., BIZZOCCHI L., IBAR E., GROSSI M., SIMPSON C., CHAPMAN S., JARVIS M.J., ROTTGERING H., NORRIS R.P., DUNLOP J., IVISON R.J., MESSIAS H., PFORR J., VACCARI M., SEYMOUR N., BEST P., GONZALEZ-SOLARES E., FARRAH D., FERNANDES C.A.C., HUANG J.-S., LACY M., MARASTON C., MARCHETTI L., MAUDUIT J.-C., OLIVER S., RIGOPOULOU D., STANFORD S.A., SURACE J. and ZEIMANN G.

Abstract (from CDS):

Ultra steep spectrum (USS) radio sources have been successfully used to select powerful radio sources at high redshifts (z ≳ 2). Typically restricted to large-sky surveys and relatively bright radio flux densities, it has gradually become possible to extend the USS search to sub-mJy levels, thanks to the recent appearance of sensitive low-frequency radio facilities. Here a first detailed analysis of the nature of the faintest USS sources is presented. By using Giant Metrewave Radio Telescope and Very Large Array radio observations of the Lockman Hole at 610 MHz and 1.4 GHz, a sample of 58 USS sources, with 610 MHz integrated fluxes above 100 µJy, is assembled. Deep infrared data at 3.6 and 4.5 µm from the Spitzer Extragalactic Representative Volume Survey (SERVS) are used to reliably identify counterparts for 48 (83%) of these sources, showing an average total magnitude of [3.6]AB= 19.8 mag. Spectroscopic redshifts for 14 USS sources, together with photometric redshift estimates, improved by the use of the deep SERVS data, for a further 19 objects, show redshifts ranging from z = 0.1 to z = 2.8, peaking at z ∼ 0.6 and tailing off at high redshifts. The remaining 25 USS sources, with no redshift estimate, include the faintest [3.6] magnitudes, with 10 sources undetected at 3.6 and 4.5 µm (typically [3.6] ≳ 22-23 mag from local measurements), which suggests the likely existence of higher redshifts among the sub-mJy USS population. The comparison with the Square Kilometre Array Design Studies Simulated Skies models indicates that Fanaroff-Riley type I radio sources and radio-quiet active galactic nuclei may constitute the bulk of the faintest USS population, and raises the possibility that the high efficiency of the USS technique for the selection of high-redshift sources remains even at the sub-mJy level.

Abstract Copyright: ∼

Journal keyword(s): galaxies: active - galaxies: evolution - galaxies: high-redshift - radio continuum: galaxies - surveys

Simbad objects: 62

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Number of rows : 62
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 ELAIS S1 reg 00 34 44 -43 28.2           ~ 254 0
2 NAME Chandra Deep Field-South reg 03 32 28.0 -27 48 30           ~ 2282 1
3 NAME Lockman Hole reg 10 45 00.0 +58 00 00           ~ 910 0
4 [IIB2009] LH610MHz J104949.1+571656 Rad 10 49 49.07 +57 16 57.6           ~ 1 0
5 LHW J105004+572733 Rad 10 50 04.13 +57 27 31.4           ~ 2 0
6 [IIB2009] LH610MHz J105004.3+572214 Rad 10 50 04.29 +57 22 14.5           ~ 1 0
7 [IIB2009] LH610MHz J105009.2+571653 Rad 10 50 09.18 +57 16 54.5           ~ 1 0
8 [IIB2009] LH610MHz J105025.4+572212 Rad 10 50 25.35 +57 22 12.6           ~ 1 0
9 [IIB2009] LH610MHz J105031.9+572027 Rad 10 50 31.96 +57 20 27.1           ~ 1 0
10 [IIB2009] LH610MHz J105041.8+572130 Rad 10 50 41.66 +57 21 31.1           ~ 1 0
11 [IIB2009] LH610MHz J105042.2+572454 Rad 10 50 42.20 +57 24 55.1           ~ 1 0
12 [IIB2009] LH610MHz J105053.3+571549 Rad 10 50 53.31 +57 15 49.3           ~ 1 0
13 [IIB2009] LH610MHz J105054.3+570416 Rad 10 50 54.28 +57 04 16.3           ~ 1 0
14 [IIB2009] LH610MHz J105055.6+571803 Rad 10 50 55.55 +57 18 04.7           ~ 1 0
15 [IIB2009] LH610MHz J105056.6+573219 Rad 10 50 56.55 +57 32 19.3           ~ 1 0
16 [IIB2009] LH610MHz J105057.5+572955 Rad 10 50 57.43 +57 29 55.8           ~ 1 0
17 [IIB2009] LH610MHz J105101.9+565750 Rad 10 51 01.80 +56 57 50.0           ~ 1 0
18 [IIB2009] LH610MHz J105105.0+571922 Rad 10 51 04.87 +57 19 23.2           ~ 1 0
19 ISO-LHDS J105108+573343 rG 10 51 08.38 +57 33 45.4           ~ 14 0
20 [IIB2009] LH610MHz J105108.9+572534 Rad 10 51 08.91 +57 25 35.0           ~ 1 0
21 [IIB2009] LH610MHz J105115.3+571820 Rad 10 51 15.19 +57 18 20.6           ~ 1 0
22 [IIB2009] LH610MHz J105133.3+571833 Rad 10 51 33.35 +57 18 33.4           ~ 1 0
23 [IIB2009] LH610MHz J105134.5+573218 Rad 10 51 34.37 +57 32 17.2           ~ 1 0
24 [IIB2009] LH610MHz J105146.8+572032 Rad 10 51 46.58 +57 20 32.4           ~ 1 0
25 [IIB2009] LH610MHz J105152.8+571347 Rad 10 51 52.73 +57 13 47.1           ~ 1 0
26 [IIB2009] LH610MHz J105155.2+570409 Rad 10 51 55.01 +57 04 09.6           ~ 1 0
27 [IIB2009] LH610MHz J105158.0+571940 Rad 10 51 58.03 +57 19 40.4           ~ 1 0
28 [IIB2009] LH610MHz J105200.3+571052 Rad 10 52 00.32 +57 10 52.7           ~ 1 0
29 [IIB2009] LH610MHz J105201.4+565947 Rad 10 52 01.12 +56 59 47.6           ~ 2 0
30 [IIB2009] LH610MHz J105201.5+571105 Rad 10 52 01.49 +57 11 06.0           ~ 1 0
31 [IIB2009] LH610MHz J105207.8+573346 Rad 10 52 07.66 +57 33 46.8           ~ 1 0
32 [IIB2009] LH610MHz J105208.0+571349 Rad 10 52 07.91 +57 13 49.6           ~ 1 0
33 [IIB2009] LH610MHz J105208.1+571321 Rad 10 52 08.08 +57 13 21.8           ~ 1 0
34 [IIB2009] LH610MHz J105208.3+571342 Rad 10 52 08.28 +57 13 42.2           ~ 1 0
35 [IIB2009] LH610MHz J105212.8+570641 Rad 10 52 12.63 +57 06 41.3           ~ 1 0
36 [IIB2009] LH610MHz J105214.0+571841 Rad 10 52 14.04 +57 18 42.0           ~ 1 0
37 SWIRE J105220.42+573931.6 rG 10 52 20.42 +57 39 31.5           ~ 2 0
38 [IIB2009] LH610MHz J105220.7+573408 Rad 10 52 20.76 +57 34 08.6           ~ 1 0
39 [IIB2009] LH610MHz J105225.6+571337 Rad 10 52 25.53 +57 13 38.5           ~ 1 0
40 SWIRE J105229.02+574616.8 rG 10 52 29.04 +57 46 16.6           ~ 2 0
41 [IIB2009] LH610MHz J105229.4+574009 Rad 10 52 29.17 +57 40 09.4           ~ 1 0
42 LHW J105230+570028 Rad 10 52 30.16 +57 00 24.3           ~ 2 0
43 RDS 801A Sy1 10 52 45.39 +57 37 45.9           ~ 10 0
44 SWIRE J105256.05+574148.3 rG 10 52 56.07 +57 41 48.6           ~ 2 0
45 [IIB2009] LH610MHz J105257.8+573058 Rad 10 52 57.65 +57 30 58.8           ~ 1 0
46 [IIB2009] LH610MHz J105258.1+573616 Rad 10 52 58.11 +57 36 16.9           ~ 1 0
47 [IIB2009] LH610MHz J105301.5+573429 Rad 10 53 01.34 +57 34 30.3           ~ 1 0
48 [IIB2009] LH610MHz J105303.7+571616 Rad 10 53 03.65 +57 16 17.0           ~ 2 0
49 [IIB2009] LH610MHz J105308.4+573557 Rad 10 53 08.43 +57 35 58.4           ~ 1 0
50 [IIB2009] LH610MHz J105310.5+572320 Rad 10 53 10.51 +57 23 21.9           ~ 1 0
51 [IIB2009] LH610MHz J105319.2+572108 Rad 10 53 19.18 +57 21 08.7           ~ 1 0
52 [IIB2009] LH610MHz J105323.2+571638 Rad 10 53 23.16 +57 16 38.4           ~ 1 0
53 [IIB2009] LH610MHz J105332.0+574145 Rad 10 53 32.16 +57 41 44.2           ~ 1 0
54 [IIB2009] LH610MHz J105345.3+572328 Rad 10 53 45.18 +57 23 29.7           ~ 1 0
55 [IIB2009] LH610MHz J105354.5+572340 Rad 10 53 54.31 +57 23 40.0           ~ 1 0
56 [IIB2009] LH610MHz J105358.1+574001 Rad 10 53 58.08 +57 40 02.5           ~ 1 0
57 [IIB2009] LH610MHz J105401.2+572842 Rad 10 54 01.00 +57 28 43.7           ~ 1 0
58 AzTEC J105406.44+573309.6 rG 10 54 06.87 +57 33 08.7   23.04   22.65   ~ 8 0
59 [IIB2009] LH610MHz J105429.1+572939 Rad 10 54 29.08 +57 29 41.5           ~ 1 0
60 [IIB2009] LH610MHz J105500.9+573344 Rad 10 55 01.06 +57 33 45.9           ~ 1 0
61 [IIB2009] LH610MHz J105502.3+573224 Rad 10 55 02.27 +57 32 25.9           ~ 1 0
62 ELAIS N1 reg 16 10 01 +54 30.6           ~ 489 0

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