Swift-XRT Survey of Fermi Unassociated Sources

These results are part of the Swift program to follow-up Fermi unassociated sources in an attempt to find X-ray counterparts to the unidentified gamma-ray sources. As new observations are performed, these pages will be updated in nearly real time. Please use these results as a guide and proceed with caution when using them in a publication since they are the result of an automated analysis.

When using these data and results in publications, please reference M.C. Stroh & A.D. Falcone 2013, ApJS, 207, 28; arXiv: 1305.4949 for a description of many of the analysis techniques used to reduce these data (note: a more detailed paper describing the complete data set and analysis is forthcoming). Please contact Abe Falcone and Michael Stroh at unassociated@swift.psu.edu if you have any questions about the program or the analysis, or to simply to let us know that you've made use of these data.
Caution: For completeness, sources are listed if the "detection" exceeds 3 sigma. The significances and images are shown so you can make more stringent significance cuts, if desired.

2FGL J1614.9-5212

Field

Detected Excesses
Swift-XRT image of the field for 2FGL J1614.9-5212 Swift-XRT detections in the field for 2FGL J1614.9-5212


No detected excesses found.

X-Ray and Gamma Ray Catalogs

More Catalogs
Swift-XRT image with known X-ray and gamma ray sources for 2FGL J1614.9-5212 Swift-XRT image with known radio, optical and UV sources for 2FGL J1614.9-5212

Known X-Ray and Gamma Ray Sources

# Source Name R.A. (J2000) Dec. (J2000) Offset (') Observatory/Database Table
1 3XMM J161447.6-521117 16 14 47.66 -52 11 17.16 2.02 XMM-NEWTON
2 3XMM J161444.0-521235 16 14 44.11 -52 12 36.00 2.27 XMM-NEWTON
3 3XMM J161453.4-521432 16 14 53.42 -52 14 32.64 2.31 XMM-NEWTON
4 3XMM J161454.6-520927 16 14 54.70 -52 09 27.36 2.99 XMM-NEWTON
5 3XMM J161515.6-520949 16 15 15.60 -52 09 50.04 3.63 XMM-NEWTON
6 3XMM J161452.1-521630 16 14 52.20 -52 16 31.08 4.26 XMM-NEWTON
7 3XMM J161526.6-521059 16 15 26.64 -52 10 59.88 4.49 XMM-NEWTON
8 3XMM J161456.9-521711 16 14 56.93 -52 17 11.76 4.82 XMM-NEWTON
9 3XMM J161451.0-520729 16 14 51.41 -52 07 29.64 5.03 XMM-NEWTON
10 3XMM J161512.9-520745 16 15 12.91 -52 07 45.12 5.11 XMM-NEWTON
11 3XMM J161424.9-521313 16 14 24.91 -52 13 13.44 5.25 XMM-NEWTON
12 3XMM J161433.2-521606 16 14 33.22 -52 16 06.96 5.41 XMM-NEWTON
13 3XMM J161521.8-520809 16 15 21.91 -52 08 09.24 5.52 XMM-NEWTON
1RXS J161524.3-520828 16 15 24.31 -52 08 27.96 5.54 ROSAT
14 3XMM J161444.8-521744 16 14 44.88 -52 17 44.88 5.77 XMM-NEWTON
15 3XMM J161506.4-520606 16 15 06.43 -52 06 06.48 6.38 XMM-NEWTON
16 3XMM J161438.5-521758 16 14 38.59 -52 17 58.20 6.39 XMM-NEWTON
17 3XMM J161459.2-521846 16 14 59.23 -52 18 46.44 6.40 XMM-NEWTON
18 1RXS J161431.4-520642 16 14 31.39 -52 06 42.12 7.06 ROSAT
19 3XMM J161414.2-521435 16 14 14.21 -52 14 35.16 7.17 XMM-NEWTON
20 3XMM J161450.7-521945 16 14 50.78 -52 19 45.48 7.48 XMM-NEWTON
21 3XMM J161409.2-521239 16 14 09.24 -52 12 39.60 7.59 XMM-NEWTON
22 3XMM J161417.2-520744 16 14 17.23 -52 07 44.76 7.87 XMM-NEWTON
23 3XMM J161427.3-520606 16 14 27.31 -52 06 06.84 7.90 XMM-NEWTON
24 3XMM J161419.6-520707 16 14 19.63 -52 07 08.04 7.97 XMM-NEWTON
25 3XMM J161501.2-520359 16 15 01.30 -52 03 59.40 8.40 XMM-NEWTON
26 3XMM J161409.7-520733 16 14 09.74 -52 07 33.96 8.92 XMM-NEWTON
27 3XMM J161426.9-521954 16 14 27.00 -52 19 54.48 8.96 XMM-NEWTON
28 3XMM J161417.0-521854 16 14 17.90 -52 18 54.72 9.13 XMM-NEWTON
29 3XMM J161355.9-521129 16 13 55.99 -52 11 30.12 9.66 XMM-NEWTON
30 3XMM J161353.3-521210 16 13 53.30 -52 12 10.44 10.03 XMM-NEWTON
31 CXO J161602.0-520948 16 16 02.71 -52 09 48.96 10.04 CHANDRA
X161602.09-520948.5 16 16 02.90 -52 09 48.60 10.04 CHANDRA
32 3XMM J161352.4-521314 16 13 52.42 -52 13 14.16 10.20 XMM-NEWTON
33 3XMM J161350.5-520958 16 13 50.57 -52 09 58.32 10.73 XMM-NEWTON
34 3XMM J161429.2-520235 16 14 29.21 -52 02 35.88 10.78 XMM-NEWTON
35 3XMM J161357.7-521800 16 13 57.79 -52 18 00.36 10.90 XMM-NEWTON
36 3XMM J161346.1-521121 16 13 46.18 -52 11 21.12 11.17 XMM-NEWTON
37 3XMM J161343.1-521200 16 13 43.20 -52 12 00.36 11.58 XMM-NEWTON
38 3XMM J161358.8-522106 16 13 58.97 -52 21 07.56 12.65 XMM-NEWTON
3XMM J161358.8-522106 16 13 58.68 -52 21 05.40 12.66 XMM-NEWTON
39 3XMM J161342.7-520644 16 13 42.72 -52 06 44.28 12.96 XMM-NEWTON
40 3XMM J161413.7-520110 16 14 13.75 -52 01 10.20 13.17 XMM-NEWTON
41 3XMM J161349.0-520345 16 13 49.61 -52 03 45.72 13.73 XMM-NEWTON
42 3XMM J161352.6-520248 16 13 52.61 -52 02 48.84 13.95 XMM-NEWTON
43 3XMM J161356.5-522240 16 13 56.52 -52 22 39.00 14.00 XMM-NEWTON
3XMM J161356.5-522240 16 13 56.62 -52 22 41.52 14.02 XMM-NEWTON
3XMM J161356.5-522240 16 13 56.54 -52 22 42.24 14.04 XMM-NEWTON

Known Radio, Optical and UV Sources

# Source Name R.A. (J2000) Dec. (J2000) Offset (') Database Table
1 [SPT2015] ATCA J1614-5213 16 14 53.71 -52 13 24.96 1.29 FER2FUSRID
[PME2013] J1614-5213 16 14 53.90 -52 13 32.16 1.37 AT2FGLUS
2 PMN J1614-5210 16 14 34.20 -52 10 54.12 4.04 PMN
3 PMN J1615-5205 16 15 30.41 -52 05 47.04 8.19 PMN
4 PMN J1614-5207 16 14 17.11 -52 07 08.04 8.26 PMN
5 PSR J1613-5211 16 13 42.50 -52 11 21.12 11.73 PMPULSAR
PSR J1613-5211 16 13 42.50 -52 11 21.12 11.74 ATNFPULSAR

Penn State University Goddard Space Flight Center Swift