appendix f: h i 21-cm absorption spectra · 2018. 9. 5. · 1 appendix f: hi 21-cm absorption...
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APPENDIX F: H I 21-cm ABSORPTION SPECTRA
The H I 21-cm absorption spectra towards all the sources observedby us are shown here. The QGP name as given in Table A1 areprovided for each spectra.
APPENDIX G: QGP IMAGES
The radio continuum contours overlaid on the optical images of theQGPs observed by us are presented here. The QGP name as givenin Table A1 are provided for each image.
© 0000 RAS, MNRAS 000, 000–000
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2
-200 -100 0 100 200Velocity Relative to z = 0.01769 (km/s)
0.99
1.00
1.01N
orm
alis
ed F
lux
J0041-0143N
1396.5 1396.0 1395.5 1395.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.01769 (km/s)
0.90
0.95
1.00
1.05
1.10
Nor
mal
ised
Flu
x
J0041-0143C
1396.5 1396.0 1395.5 1395.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.01769 (km/s)
0.94
0.96
0.98
1.00
Nor
mal
ised
Flu
x
J0041-0143S
1396.5 1396.0 1395.5 1395.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.07975 (km/s)
0.96
0.98
1.00
1.02
1.04
Nor
mal
ised
Flu
x
J0043+0024
1316.0 1315.5 1315.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.05198 (km/s)
0.995
1.000
1.005
Nor
mal
ised
Flu
x
J0134+0003
1351.0 1350.5 1350.0 1349.5Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.01565 (km/s)
0.95
1.00
1.05N
orm
alis
ed F
lux
J0802+1601
1399.0 1398.5 1398.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.04363 (km/s)
0.99
1.00
1.01
Nor
mal
ised
Flu
x
J0817+1958
1361.5 1361.0 1360.5Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.18350 (km/s)
0.90
0.95
1.00
1.05
1.10
Nor
mal
ised
Flu
x
J0821+5031
1200.5 1200.0 1199.5Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.07342 (km/s)
0.99
1.00
1.01
Nor
mal
ised
Flu
x
J0849+5108_1
1324.0 1323.5 1323.0 1322.5Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.31200 (km/s)
0.90
0.92
0.94
0.96
0.98
1.00
Nor
mal
ised
Flu
x
J0849+5108_2
1083.2 1083.0 1082.8 1082.6 1082.4 1082.2 1082.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.10425 (km/s)
0.95
1.00
1.05
Nor
mal
ised
Flu
x
J0856+1020
1287.0 1286.5 1286.0 1285.5Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.02293 (km/s)
0.99
1.00
1.01
Nor
mal
ised
Flu
x
J0911+1958
1389.0 1388.5 1388.0Heliocentric Frequency (MHz)
Figure F1. H I 21-cm absorption spectra towards the radio sources in our primary sample, smoothed to ∼4 km s−1. The shaded regions are affected by RFI.
© 0000 RAS, MNRAS 000, 000–000
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3
-200 -100 0 100 200Velocity Relative to z = 0.05436 (km/s)
0.96
0.98
1.00
1.02
1.04
Nor
mal
ised
Flu
x
J1015+1637
1348.0 1347.5 1347.0 1346.5Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.02996 (km/s)
0.99
1.00
1.01
Nor
mal
ised
Flu
x
J1110+0321E
1380.0 1379.5 1379.0 1378.5Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.02996 (km/s)
0.99
1.00
1.01
Nor
mal
ised
Flu
x
J1110+0321W
1380.0 1379.5 1379.0 1378.5Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.06190 (km/s)
0.96
0.98
1.00
1.02
1.04
Nor
mal
ised
Flu
x
J1126+3802
1338.5 1338.0 1337.5 1337.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.07620 (km/s)
0.99
1.00
1.01
Nor
mal
ised
Flu
x
J1133+0015_1
1320.5 1320.0 1319.5 1319.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.07584 (km/s)
0.99
1.00
1.01N
orm
alis
ed F
lux
J1133+0015_2
1321.0 1320.5 1320.0 1319.5Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.13797 (km/s)
0.96
0.98
1.00
1.02
1.04
Nor
mal
ised
Flu
x
J1156+3412
1249.0 1248.5 1248.0 1247.5Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.17098 (km/s)
0.96
0.98
1.00
1.02
Nor
mal
ised
Flu
x
J1209+4119
1213.5 1213.0 1212.5Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.13837 (km/s)
0.99
1.00
1.01
Nor
mal
ised
Flu
x
J1228+3706
1248.5 1248.0 1247.5 1247.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.14300 (km/s)
0.80
0.85
0.90
0.95
1.00
Nor
mal
ised
Flu
x
J1241+6332
1243.5 1243.0 1242.5 1242.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.01693 (km/s)
0.80
0.85
0.90
0.95
1.00
Nor
mal
ised
Flu
x
J1243+4043
1397.5 1397.0 1396.5 1396.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.00263 (km/s)
0.996
0.998
1.000
1.002
1.004
Nor
mal
ised
Flu
x
J1243+1622N
1417.5 1417.0 1416.5 1416.0Heliocentric Frequency (MHz)
Figure F1. Continued from previous page.
© 0000 RAS, MNRAS 000, 000–000
-
4
-200 -100 0 100 200Velocity Relative to z = 0.00263 (km/s)
0.995
1.000
1.005N
orm
alis
ed F
lux
J1243+1622C
1417.5 1417.0 1416.5 1416.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.00263 (km/s)
0.995
1.000
1.005
Nor
mal
ised
Flu
x
J1243+1622S
1417.5 1417.0 1416.5 1416.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.02460 (km/s)
0.98
0.99
1.00
1.01
1.02
Nor
mal
ised
Flu
x
J1254+0546
1387.0 1386.5 1386.0 1385.5Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.02275 (km/s)
0.96
0.98
1.00
1.02
Nor
mal
ised
Flu
x
J1300-0121
1389.5 1389.0 1388.5 1388.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.22290 (km/s)
0.96
0.98
1.00
1.02
1.04
Nor
mal
ised
Flu
x
J1300+2830
1162.2 1162.0 1161.8 1161.6 1161.4 1161.2 1161.0 1160.8Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.26220 (km/s)
0.96
0.98
1.00
1.02N
orm
alis
ed F
lux
J1345+0347
1126.0 1125.8 1125.6 1125.4 1125.2 1125.0 1124.8 1124.6Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.14607 (km/s)
0.96
0.98
1.00
1.02
1.04
Nor
mal
ised
Flu
x
J1359+2935
1240.0 1239.5 1239.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.05422 (km/s)
0.98
0.99
1.00
1.01
1.02
Nor
mal
ised
Flu
x
J1422+0540
1348.0 1347.5 1347.0 1346.5Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.14680 (km/s)
0.7
0.8
0.9
1.0
1.1
Nor
mal
ised
Flu
x
J1438+1758
1239.0 1238.5 1238.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.37140 (km/s)
0.70
0.75
0.80
0.85
0.90
0.95
1.00
Nor
mal
ised
Flu
x
J1443+0214
1036.4 1036.2 1036.0 1035.8 1035.6 1035.4 1035.2Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.21980 (km/s)
0.96
0.98
1.00
1.02
Nor
mal
ised
Flu
x
J1457+0519
1165.2 1165.0 1164.8 1164.6 1164.4 1164.2 1164.0 1163.8Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.09094 (km/s)
0.94
0.96
0.98
1.00
1.02
1.04
1.06
Nor
mal
ised
Flu
x
J1525+4201
1302.5 1302.0 1301.5Heliocentric Frequency (MHz)
Figure F1. Continued from previous page.
© 0000 RAS, MNRAS 000, 000–000
-
5
-200 -100 0 100 200Velocity Relative to z = 0.02593 (km/s)
0.96
0.98
1.00
1.02
1.04
Nor
mal
ised
Flu
x
J1539+0534
1385.0 1384.5 1384.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.10070 (km/s)
0.96
0.98
1.00
1.02
1.04
Nor
mal
ised
Flu
x
J1551+0713
1291.0 1290.5 1290.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.04620 (km/s)
0.98
0.99
1.00
1.01
1.02
Nor
mal
ised
Flu
x
J1606+2717
1358.5 1358.0 1357.5 1357.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.36620 (km/s)
0.996
0.998
1.000
1.002
1.004
Nor
mal
ised
Flu
x
J1634+3900
1040.2 1040.0 1039.8 1039.6 1039.4 1039.2 1039.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.07900 (km/s)
0.4
0.5
0.6
0.7
0.8
0.9
1.0
Nor
mal
ised
Flu
x
J1639+1127
1317.0 1316.5 1316.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.03121 (km/s)
0.96
0.98
1.00
1.02N
orm
alis
ed F
lux
J1643+3547
1378.0 1377.5 1377.0 1376.5Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.03583 (km/s)
0.99
1.00
1.01
Nor
mal
ised
Flu
x
J1648+2429
1372.0 1371.5 1371.0 1370.5Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.00008 (km/s)
0.995
1.000
1.005
1.010
1.015
Nor
mal
ised
Flu
x
J1748+7005
1421.0 1420.5 1420.0 1419.5Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.21110 (km/s)
0.95
1.00
1.05
Nor
mal
ised
Flu
x
J2240-0836
1173.6 1173.4 1173.2 1173.0 1172.8 1172.6 1172.4 1172.2Heliocentric Frequency (MHz)
Figure F1. Continued from previous page.
© 0000 RAS, MNRAS 000, 000–000
-
6
-200 -100 0 100 200Velocity Relative to z = 0.07750 (km/s)
0.96
0.98
1.00
1.02N
orm
alis
ed F
lux
J0820+0826
1319.0 1318.5 1318.0 1317.5Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.02376 (km/s)
0.90
0.95
1.00
1.05
1.10
Nor
mal
ised
Flu
x
J0919+3400E
1388.0 1387.5 1387.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.02376 (km/s)
0.85
0.90
0.95
1.00
1.05
1.10
1.15
Nor
mal
ised
Flu
x
J0919+3400W
1388.0 1387.5 1387.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.11240 (km/s)
0.96
0.98
1.00
1.02
Nor
mal
ised
Flu
x
J0947+1113
1277.5 1277.0 1276.5Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.07282 (km/s)
0.99
1.00
1.01
Nor
mal
ised
Flu
x
J0954+3733
1324.5 1324.0 1323.5Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.03346 (km/s)
0.90
0.95
1.00
1.05
1.10
Nor
mal
ised
Flu
x
J0956+1614N
1375.0 1374.5 1374.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.03346 (km/s)
0.85
0.90
0.95
1.00
1.05
1.10
1.15
Nor
mal
ised
Flu
x
J0956+1614S
1375.0 1374.5 1374.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.23380 (km/s)
0.94
0.96
0.98
1.00
1.02
1.04
Nor
mal
ised
Flu
x
J1050+0002
1152.0 1151.8 1151.6 1151.4 1151.2 1151.0 1150.8 1150.6Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.04320 (km/s)
0.96
0.98
1.00
1.02
Nor
mal
ised
Flu
x
J1359+2708
1362.0 1361.5 1361.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.03029 (km/s)
0.90
0.95
1.00
1.05
1.10
Nor
mal
ised
Flu
x
J1438+0920
1379.5 1379.0 1378.5 1378.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.09382 (km/s)
0.96
0.98
1.00
1.02
1.04
Nor
mal
ised
Flu
x
J1624+2328
1299.0 1298.5 1298.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.05815 (km/s)
0.98
0.99
1.00
1.01
1.02
Nor
mal
ised
Flu
x
J2242-0019
1343.0 1342.5 1342.0 1341.5Heliocentric Frequency (MHz)
Figure F2. Same as in Fig. F1 for the radio sources in the supplementary sample.
© 0000 RAS, MNRAS 000, 000–000
-
7
-200 -100 0 100 200Velocity Relative to z = 0.34235 (km/s)
0.95
1.00
1.05N
orm
alis
ed F
lux
J0846+0704
1058.8 1058.6 1058.4 1058.2 1058.0 1057.8 1057.6Heliocentric Frequency (MHz)
-400 -300 -200 -100 0Velocity Relative to z = 0.12390 (km/s)
0.4
0.5
0.6
0.7
0.8
0.9
1.0
Nor
mal
ised
Flu
x
J0942+0623
1265.5 1265.0 1264.5 1264.0Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.06326 (km/s)
0.90
0.95
1.00
1.05
1.10
Nor
mal
ised
Flu
x
J1214+2931
1336.5 1336.0 1335.5Heliocentric Frequency (MHz)
200 300 400 500 600Velocity Relative to z = 0.20153 (km/s)
0.5
0.6
0.7
0.8
0.9
1.0
1.1
Nor
mal
ised
Flu
x
J2054+0041
1181.2 1181.0 1180.8 1180.6 1180.4 1180.2 1180.0 1179.8Heliocentric Frequency (MHz)
-200 -100 0 100 200Velocity Relative to z = 0.08723 (km/s)
0.98
0.99
1.00
1.01
1.02
Nor
mal
ised
Flu
x
J1643+2419
1307.0 1306.5 1306.0Heliocentric Frequency (MHz)
Figure F3. Same as in Fig. F1 for the radio sources in the miscellaneous sample.
© 0000 RAS, MNRAS 000, 000–000
-
8
27.0 26.0 25.0 24.0 23.0 22.0 21.0 0:41:20.0
42:3
0.0
-1:4
3:00
.030
.044
:00.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
S
N
Q
G
CL = 0.0025
(a) J0041−0143
34.5 34.0 33.5 0:43:33.0 32.5 32.0 31.5 31.0
30.0
20.0
10.0
0:25
:00.
050
.040
.024
:30.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
Q
G
CL = 0.0005
(b) J0043+0024
14.5 14.0 13.5 1:34:13.0 12.5 12.0 11.5 11.0
10.0
0:04
:00.
050
.040
.030
.003
:20.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
G
Q
CL = 0.001
(c) J0134+0003
44.0 43.0 42.0 41.0 8:02:40.0 39.0 38.0
40.0
30.0
20.0
10.0
16:0
1:00
.050
.040
.030
.000
:20.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00) Q
G
CL = 0.0005
(d) J0802+1601
08.0 07.0 06.0 8:17:05.0 04.0 03.0
20.0
10.0
19:5
9:00
.050
.040
.030
.020
.010
.058
:00.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00) Q
G
CL = 0.0005
(e) J0817+1958
55.0 54.5 8:21:54.0 53.5 53.0 52.5
35.0
30.0
25.0
50:3
1:20
.015
.010
.0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
CL = 0.0025
Q
G
(f) J0821+5031
01.0 8:50:00.0 59.0 58.0 57.0 56.0 49:55.0
51:0
9:00
.050
.040
.030
.020
.010
.008
:00.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
CL = 0.002
G2
Q
G1
(g) J0849+5108
25.8 25.6 25.4 25.2 8:56:25.0 24.8 24.6 24.4 24.2 24.0
30.0
25.0
10:2
0:20
.015
.010
.005
.0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
Q
G
CL = 0.0005
(h) J0856+1020
35.5 35.0 34.5 9:11:34.0 33.5 33.0 32.5 32.0 31.5
40.0
30.0
20.0
10.0
19:5
8:00
.057
:50.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
G
Q
CL = 0.0005
(i) J0911+1958
16.0 10:15:15.0 14.0 13.0
10.0
16:3
8:00
.050
.040
.030
.020
.037
:10.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
CL = 0.002
Q
G
(j) J1015+1637
28.0 26.0 24.0 22.0 11:10:20.0
30.0
3:22
:00.
030
.021
:00.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
CL = 0.0015
W
Q
G
E
(k) J1110+0321
15.0 14.0 11:26:13.0 12.0 11.0
40.0
30.0
20.0
10.0
38:0
2:00
.001
:50.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
CL = 0.003
Q
G
(l) J1126+3802
05.0 04.5 04.0 03.5 11:33:03.0 02.5 02.0 01.5
10.0
0:16
:00.
050
.040
.030
.015
:20.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
Q
G2
G1
CL = 0.001
(m) J1133+0015
00.5 11:57:00.0 59.5 56:59.0 58.5
30.0
25.0
34:1
2:20
.015
.010
.005
.0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
CL = 0.0005
Q
G
(n) J1156+3412
24.0 23.5 12:09:23.0 22.5 22.0 21.5
55.0
50.0
45.0
41:1
9:40
.035
.030
.0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
G
Q
CL = 0.001
(o) J1209+4119
48.5 12:28:48.0 47.5 47.0 46.5
25.0
20.0
15.0
10.0
05.0
37:0
6:00
.0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
CL = 0.003
G
Q
(p) J1228+3706
Figure G1. SDSS r-band images (DSS image in case of J1749+7008) overlaid with the 1.4 GHz continuum contours of the QGPs in our primary sample. Ineach image the radio source is marked by ‘Q’ and the galaxy is marked by ‘G’. In case of the QGPs J0849+5108 and J1133+0015, there are two galaxiesaround the same radio sightline marked by ‘G1’ and ‘G2’. In case of multiple radio sightlines for the same QGP, the sightlines are marked by N, S, E andW (denoting north, south, east and west, respectively). The restoring beam of the continuum map is shown at the bottom left corner (the sizes are given inTable D1). The contour levels are plotted as CL × (−1,1,2,4,8,...) Jansky beam−1, where CL is given in each image. Solid lines correspond to positive valueswhile dashed lines correspond to negative values.
© 0000 RAS, MNRAS 000, 000–000
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59.0 12:41:58.0 57.0 56.0
55.0
50.0
45.0
63:3
2:40
.035
.030
.0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
CL = 0.0025
G
Q
(q) J1241+6332
12:44:00.0 58.0 56.0 54.0 43:52.0
45:0
0.0
30.0
40:4
4:00
.030
.043
:00.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
CL = 0.003
G
Q
(r) J1243+4043
55.0 12:43:50.0 45.0 40.0
25:0
0.0
24:0
0.0
16:2
3:00
.022
:00.
021
:00.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
S
N
Q
G
CL = 0.0025
(s) J1243+1622
23.2 23.0 22.8 22.6 22.4 22.2 12:54:22.0 21.8 21.6 21.4 21.2
30.0
25.0
5:46
:20.
015
.010
.005
.0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
Q
G
CL = 0.0015
(t) J1254+0546
29.5 13:00:29.0 28.5 28.0 27.5
25.0
20.0
15.0
10.0
05.0
28:3
0:00
.0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
G
Q
CL = 0.0005
(u) J1300+2830
52.0 51.5 51.0 50.5 13:00:50.0 49.5 49.0 48.5
21:2
0.0
30.0
40.0
50.0
-1:2
2:00
.010
.0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
Q
G
CL = 0.0005
(v) J1300−0121
29.6 29.4 29.2 13:45:29.0 28.8 28.6 28.4 28.2 28.0 27.8
30.0
25.0
3:47
:20.
015
.010
.005
.0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
GQ
CL = 0.0006
(w) J1345+0347
13:59:10.0 09.0 08.0 07.0 06.0
29:3
6:00
.050
.040
.030
.020
.035
:10.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
CL = 0.002
Q
G
(x) J1359+2935
55.0 54.5 54.0 53.5 14:22:53.0 52.5 52.0 51.5
40.0
30.0
20.0
10.0
5:40
:00.
039
:50.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
G
Q
CL = 0.0005
(y) J1422+0540
07.8 07.4 14:38:07.0 06.6 06.2 05.8
15.0
10.0
05.0
17:5
8:00
.055
.057
:50.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
CL = 0.0008
G
Q
(z) J1438+1758
05.2 04.8 04.4 14:43:04.0 03.6
30.0
25.0
2:14
:20.
015
.010
.005
.0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
CL = 0.001
Q
(aa) J1443+0214
23.4 23.2 23.0 22.8 22.6 22.4 22.2 14:57:22.0 21.8 21.6
35.0
30.0
25.0
5:19
:20.
015
.010
.0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
Q
G
CL = 0.001
(ab) J1457+0519
26.0 25.5 25.0 24.5 15:25:24.0 23.5 23.0 22.5 22.0 21.5 21.0
40.0
30.0
20.0
10.0
42:0
1:00
.000
:50.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
Q
G
CL = 0.0005
(ac) J1525+4201
08.0 07.0 06.0 15:39:05.0 04.0 03.0
20.0
10.0
5:35
:00.
050
.040
.030
.020
.010
.034
:00.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
CL = 0.001
G
Q
(ad) J1539+0534
22.5 22.0 21.5 21.0 20.5 15:51:20.0
20.0
15.0
10.0
05.0
7:14
:00.
055
.050
.045
.013
:40.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
G
Q
CL = 0.0003
(ae) J1551+0713
00.5 16:07:00.0 59.5 59.0 58.5 58.0 57.5 06:57.0 56.5
30.0
20.0
10.0
27:1
7:00
.050
.016
:40.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
G
Q
CL = 0.0005
(af) J1606+2717
Figure G1. Continued from previous page.
© 0000 RAS, MNRAS 000, 000–000
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04.0 03.5 16:34:03.0 02.5 02.0
15.0
10.0
05.0
39:0
0:00
.055
.038
:59:
50.0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
QG
CL = 0.0008
(ag) J1634+3900
57.2 56.8 56.4 16:39:56.0 55.6
10.0
05.0
11:2
8:00
.055
.027
:50.
045
.0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
CL = 0.003
Q
G
(ah) J1639+1127
22.0 16:43:20.0 18.0 16.0 14.0 12.0 10.0
30.0
48:0
0.0
30.0
35:4
7:00
.030
.046
:00.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
CL = 0.001
G
Q
(ai) J1643+3547
05.0 04.0 03.0 02.0 01.0 16:48:00.0
24:3
0:00
.050
.040
.030
.020
.010
.029
:00.
050
.028
:40.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
G
Q
CL = 0.0008
(aj) J1648+2429
30.0 17:50:00.0 30.0 49:00.0
14:0
0.0
12:0
0.0
70:1
0:00
.008
:00.
006
:00.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
CL = 0.0025
Q
G
(ak) J1749+7008
14.4 14.2 14.0 13.8 13.6 13.4 13.2 22:40:13.0 12.8 12.6 12.4
15.0
20.0
25.0
-8:3
6:30
.035
.040
.0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
G
Q
CL = 0.0025
(al) J2240−0836
Figure G1. Continued from previous page.
© 0000 RAS, MNRAS 000, 000–000
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16.8 16.4 8:20:16.0 15.6 15.2
25.0
20.0
15.0
10.0
05.0
8:26
:00.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
Q
G
CL = 0.0008
(a) J0820+0826
21.0 9:19:20.0 19.0 18.0 17.0 16.0 15.0 14.0
01:0
0.0
40.0
20.0
34:0
0:00
.0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
CL = 0.0015
WE
G
(b) J0919+3400
46.8 46.6 46.4 46.2 9:47:46.0 45.8 45.6 45.4 45.2 45.0
05.0
11:1
4:00
.055
.050
.045
.013
:40.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
Q G
CL = 0.0005
(c) J0947+1113
40.0 38.0 36.0 34.0 32.0 9:54:30.0 28.0 26.0
35:0
0.0
30.0
37:3
4:00
.030
.033
:00.
032
:30.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
CL = 0.002
Q
G
(d) J0954+3733
06.0 05.5 05.0 04.5 9:56:04.0 03.5 03.0 02.5 02.0
50.0
40.0
30.0
20.0
10.0
16:1
4:00
.0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
CL = 0.003
S
N
G
(e) J0956+1614
54.8 54.6 54.4 54.2 10:50:54.0 53.8 53.6 53.4 53.2 53.0
25.0
20.0
15.0
10.0
05.0
0:02
:00.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
Q
G
CL = 0.0008
(f) J1050+0002
49.0 48.5 13:59:48.0 47.5 47.0
40.0
35.0
27:0
8:30
.025
.020
.015
.0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
Q
G
CL = 0.001
(g) J1359+2708
12.0 11.0 14:38:10.0 09.0 08.0 07.0
21:0
0.0
50.0
40.0
30.0
20.0
10.0
9:20
:00.
050
.019
:40.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
G
Q
CL = 0.001
(h) J1438+0920
36.0 35.5 35.0 34.5 16:24:34.0 33.5 33.0 32.5 32.0
30.0
20.0
10.0
23:2
9:00
.050
.028
:40.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
G
Q
CL = 0.001
(i) J1623+2329
22:42:50.0 49.0 48.0 47.0 46.0 45.0
19:0
0.0
20.0
40.0
-0:2
0:00
.020
.0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
Q
G
CL = 0.001
(j) J2242−0019
Figure G2. Same as in Fig. G1 for the sources in the supplementary sample.
© 0000 RAS, MNRAS 000, 000–000
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03.0 02.0 01.0 8:46:00.0 59.0 45:58.0
05:0
0.0
50.0
40.0
30.0
20.0
10.0
7:04
:00.
050
.003
:40.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
CL = 0.0025
Q
G
(a) J0846+0704
22.8 22.4 9:42:22.0 21.6 21.2
50.0
45.0
6:23
:40.
035
.030
.025
.0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
CL = 0.0025
Q
G
(b) J0942+0623
12:14:20.0 19.5 19.0 18.5 18.0 17.5 17.0 16.5 16.0
10.0
29:3
2:00
.050
.040
.030
.031
:20.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
G
Q
CL = 0.0005
(c) J1214+2931
32.0 31.0 16:43:30.0 29.0
20.0
10.0
24:2
0:00
.050
.040
.019
:30.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
CL = 0.0015
Q
G
(d) J1643+2419
50.6 50.4 50.2 20:54:50.0 49.8 49.6 49.4 49.2 49.0 48.8
05.0
0:42
:00.
055
.050
.045
.041
:40.
0
Right Ascension (J2000)
Dec
linat
ion
(J20
00)
G
Q
CL = 0.0008
(e) J2054+0041
Figure G3. Same as in Fig. G1 for the sources in the miscellaneous sample.
© 0000 RAS, MNRAS 000, 000–000
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