2020A&A...638A.128M


Query : 2020A&A...638A.128M

2020A&A...638A.128M - Astronomy and Astrophysics, volume 638A, 128-128 (2020/6-1)

The γ-ray sky seen at X-ray energies. II. The Swift hunt of Fermi BL Lac objects among unidentified γ-ray sources.

MARCHESINI E.J., PAGGI A., MASSARO F., MASETTI N., D'ABRUSCO R. and ANDRUCHOW I.

Abstract (from CDS):


Context. Nearly 50% of all sources detected by the Fermi Large Area Telescope are classified as blazars or blazar candidates, one of the most elusive classes of active galaxies. Additional blazars can also be hidden within the sample of unidentified or unassociated γ-ray sources (UGSs) that constitute about one-third of all gamma-ray sources detected to date. We recently confirmed that the large majority of Fermi blazars of the BL Lac subclass have an X-ray counterpart.
Aims. Using the X-ray properties of a BL Lac training set and combining these with archival multifrequency information, we aim to search for UGSs that could have a BL Lac source within their γ-ray positional uncertainty regions.
Methods. We reduced and analyzed the Swift X-ray observations of a selected sample of 327 UGSs. We then compared the X-ray fluxes and hardness ratios of all sources detected in the pointed fields with those of known Fermi BL Lacs.
Results. We find at least one X-ray source, lying within the γ-ray positional uncertainty at 95% confidence level, for 223 UGSs and a total of 464 X-ray sources in all fields analyzed. The X-ray properties of a large fraction of them, eventually combined with radio, infrared, and optical information, exhibit BL Lac multi-frequency behavior, thus allowing us to select high-confidence BL Lac candidates; some of them were recently observed during our optical spectroscopic campaign which confirmed their nature.
Conclusions. We find that out of 50 X-ray sources that were confirmed as BL Lacs through optical spectroscopy, 12 do not show canonical mid-infrared or radio BL Lac properties. This indicates that the selection of X-ray BL Lac candidates is a strong method to find new counterparts within Fermi UGSs. Finally, we pinpoint a sample of 32 Swift/XRT candidate counterparts to Fermi UGSs that are most likely BL Lac objects.

Abstract Copyright: © ESO 2020

Journal keyword(s): galaxies: active - galaxies: nuclei - galaxies: jets - BL Lacertae objects: general - X-rays: galaxies - gamma rays: galaxies

Simbad objects: 51

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Number of rows : 51
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 1RXS J000626.6+013609 BLL 00 06 26.9244492200 +01 36 10.378006968           ~ 19 1
2 3FGL J0017.1+1445 gam 00 17 11 +14 45.7           ~ 5 0
3 9Y-MST J0020+0322 BLL 00 21 01.6 +03 22 42           ~ 19 0
4 SDSS J003159.85+093618.4 Bla 00 31 59.8629555436 +09 36 18.435307768           ~ 12 0
5 9Y-MST J0031-5521 Bla 00 32 18.7 -55 22 00           ~ 29 0
6 3FGL J0032.5+3912 Bla 00 32 35 +39 12.8           ~ 7 0
7 SDSS J004859.16+422351.1 BLL 00 48 59.1606548688 +42 23 51.064163520           ~ 23 0
8 3FGL J0121.8-3917 BL? 01 21 52.7 -39 15 42           ~ 21 0
9 6dFGS gJ020020.9-410936 BLL 02 00 20.9436129216 -41 09 35.677153008   20.48   18.64   ~ 34 0
10 9Y-MST J0216+0300 BLL 02 15 58.0 +03 00 16           ~ 17 0
11 3FGL J0430.1-3103 BLL 04 29 58.9 -30 59 33           ~ 23 0
12 3FGL J0516.6+1012 BLL 05 16 41 +10 12.4           ~ 9 0
13 2FGL J0536.2-3348 BLL 05 36 29.0674147920 -33 43 02.465333796 17.11 16.97 16.93 16.8   ~ 53 0
14 ICRF J061017.8-184740 Bla 06 10 17.8858288680 -18 47 40.089141708       17.29   ~ 47 0
15 3FGL J0704.3-4828 BLL 07 04 21.820 -48 26 47.59           ~ 15 0
16 2FGL J0737.5-8246 BLL 07 37 06.09652 -82 48 40.0144           ~ 27 0
17 3FHL J0802.2-0943 BLL 08 02 15.74 -09 42 49.1           ~ 24 0
18 3FGL J0809.3-0941 gam 08 09.3 -09 41           ~ 1 0
19 3FGL J0919.4+6604 BLL 09 19 22.1 +66 07 38           ~ 8 0
20 9Y-MST J0921+2335 BLL 09 21 45.358 +23 35 48.41           ~ 24 0
21 2MASX J09402250+6148267 BLL 09 40 22.4527825176 +61 48 26.262994536   19.67 18.69 16.9   ~ 62 0
22 3FGL J1117.7+0217 BLL 11 17 37.9 +02 17 42           ~ 14 0
23 9Y-MST J1120-2646 BLL 11 20 09.3 -26 45 52           ~ 11 0
24 ICRF J112038.4+070447 QSO 11 20 38.44359842 +07 04 47.1724558           ~ 60 1
25 4FGL J1146.0-0638 BLL 11 46 00.8591007005 -06 38 54.797803202           ~ 20 0
26 9Y-MST J1200+0202 BLL 12 00 12.346 +02 02 08.41           ~ 26 0
27 3FGL J1200.9-1432 Bla 12 00 55.11 -14 30 39.7           ~ 19 0
28 3FGL J1225.4-3448 BLL 12 25 36.9 -34 47 20           ~ 23 0
29 4C -02.55 QSO 12 32 00.0159535440 -02 24 04.793069304   17.41 17.06 16.4   ~ 432 1
30 3FGL J1249.5-0546 BL? 12 49 18.3 -05 45 44           ~ 19 0
31 SDSS J125821.45+212351.3 BLL 12 58 21.4555723595 +21 23 51.346858831           ~ 18 0
32 3FGL J1309.0+0347 BLL 13 08 47.7 +03 47 03           ~ 11 0
33 3FGL J1411.4-0724 BLL 14 11 33.3 -07 22 53           ~ 20 0
34 3FHL J1513.4-3721 BLL 15 13 25.8 -37 21 42           ~ 19 0
35 2FGL J1612.0+1403 AGN 16 12 07.5 +14 07 00           ~ 18 0
36 SWIFT J180914.8+350903 X 18 09 14.8 +35 09 03           ~ 1 0
37 3FGL J1809.0+3517 BL? 18 09 14.8 +35 09 03           ~ 20 0
38 BWE 1810+5331 BLL 18 10 37.990 +53 35 01.56           ~ 23 0
39 2FGL J1922.6-7454 BLL 19 22 40.210 -74 53 48.91           ~ 27 0
40 4FGL J1934.2+6002 BLL 19 34 19.6 +60 01 40           ~ 25 0
41 3FGL J2030.5-1439 BLL 20 30 27.91 -14 39 17.1           ~ 19 0
42 2FGL J2034.7-4201 BLL 20 34 51.0909972120 -42 00 38.437476084           ~ 38 0
43 9Y-MST J2043+0000 BLL 20 43 50.14920 +00 01 27.9300           ~ 17 0
44 3FGL J2044.0+1035 Bla 20 44 00.6 +10 36 28           ~ 18 0
45 9Y-MST J2048-3121 Bla 20 47 55.4 -31 22 40           ~ 16 0
46 1FGL J2112.5-3044 gam 21 12 33.6 -30 43 45           ~ 27 0
47 3FGL J2142.7+1957 BLL 21 42 47.5 +19 58 11           ~ 22 0
48 3FGL J2144.6-5640 BLL 21 44 29.57 -56 38 49.0           ~ 10 0
49 2MASS J23001240+4052247 BLL 23 00 12.3707568624 +40 52 24.693697956           ~ 24 1
50 PHL 5711 BLL 23 21 37.0098015261 -16 19 28.388190783   19.4   19.2   ~ 25 0
51 9Y-MST J2336-8426 BLL 23 36 27.85608 -84 26 52.0836           ~ 17 0

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