Table 4
Mean flux densities for the detected MSPs in the frequency range 110–188 MHz.
| PSR | DM | W eff | δ | S mean | KL01 flux density | Predicted Smean | S ref | ν ref | Spectral | Reference |
| (pc cm-3) | (ms) | (%) | (mJy) | (mJy at 102 MHz) | (mJy) | (mJy) | (MHz) | index | ||
|
|
||||||||||
| J0030+0451 | 4 .333 | 0.61(1)⋆ | 12.6(2)⋆ | 99(1) | 380 ± 200† | 80 ± 40 | 7.9 ± 0.2 | 430 |
|
1, 38 |
| J0034−0534 | 13 .765 | 0.54(1)⋆ | 28.8(4)⋆ | 491(2) | 250 ± 120 | 400 ± 100 | 17 ± 5 | 436 | −2.64 ± 0.05 | 2, 38 |
| J0214+5222 | 22 .037 | 1.5(2)⋆ | 6.1(8)⋆ | 21.0(7) | ... | 4.1 | 0.90 | 350 | −1.6 | 32 |
| J0218+4232 | 61 .252 | 0.77(2) | 33.1(8) | 37.6(8) | 270 ± 150 ‡ | 530 ± 70 | 30–40 | 410 | −2.41 ± 0.04 | 3, 38 |
| J0337+1715 | 21 .316 | 0.85(4)⋆ | 16(2) | 5.0(7) | ... | 50 ± 100 | ~ 2 | 1400 | −1.4 ± 1 | 30, 22 |
| J0407+1607 | 35 .65 | 4.2(1)⋆ | 16.4(4)⋆ | 56.5(8) | ... | 50 ± 50 | 10.2 | 430 | −1.4 ± 1 | 34, 22 |
| J0621+1002 | 36 .601 | 6.1(2) | 21.3(8) | 20(1) | 50 ± 25† | 170 ± 380 | 1.9 ± 0.3 | 800 | −2.5 ± 1.4 | 4 |
| J0636+5129 | 11 .107 | 0.14(2) | 4.9(8) | 4.1(8) | ... | 5.5 | 1.8 | 350 | −1.2 | 32 |
| J0645+5158 | 18 .247 | 0.16(2)⋆ | 1.8(2)⋆ | 4.7(7) | ... | 20 | 2.4 | 350 | −2.2 | 32 |
| J0737−3039A | 48 .920 | 2.5(2) | 11.2(8) | 64(10) | ... | 40 ± 80 | 1.6 ± 0.3 | 1400 | −1.4 ± 1 | 5, 22 |
| J0751+1807 | 30 .249 | 0.65(5) | 19(2) | 5.5(8) | 70 ± 30 | 30 ± 10 | 10 | 430 | −0.9 ± 0.3 | 6, 4 |
| J1012+5307 | 9 .023 | 0.69(2)⋆ | 13.1(4)⋆ | 34.5(5) | 30 ± 15 | 220 ± 90 | 30 | 410 | −1.8 ± 0.4 | 7, 4 |
| J1022+1001 | 10 .252 | 1.00(3)⋆ | 6.1(2)⋆ | 40.7(9) | 90 ± 40 | 110 ± 40 | 20 ± 9 | 370 | −1.7 ± 0.1 | 8, 4 |
| J1023+0038 | 14 .325 | 0.15(1)⋆ | 9.1(8)⋆ | 48(2) | ... | 440–3400 | 0.4–3.1ʠ | 1600 | ~ −2.8 | 31, 9 |
| J1024−0719 | 6 .485 | 0.54(4)⋆ | 10.4(8)⋆ | 21(2) | 200 ± 100 | 30 ± 10 | 4.6 ± 1.2 | 410/430 | −1.5 ± 0.2 | 10, 4 |
| J1038+0032 | 26 .59 | 5.4(2) | 18.7(8) | 16(1) | ... | 5 ± 10 | 0.20 ± 0.04 | 1400 | −1.4 ± 1 | 5, 22 |
| J1231−1411 | 8 .090 | 0.41(3) | 11.1(8) | 22(3) | ... | 5 ± 7 | 0.4 | 820 | −1.4 ± 1 | 27, 22 |
| B1257+12 | 10 .166 | 0.63(1)⋆ | 10.2(2)⋆ | 80.9(9) | 150 ± 50 | 180 ± 90 | 20 | 430 | −1.9 ± 0.5 | 11, 4 |
| J1453+1902 | 14 .049 | 0.96(9) | 17(2) | 6(1) | ... | 10 ± 10 | 2.2 ± 0.1 | 430 | −1.4 ± 1 | 36, 22 |
| J1544+4937 | 23 .226 | 0.45(3) | 21(2) | 11.5(5) | ... | 40 | 5.4 | 322 | −2.3 | 37 |
| J1640+2224 | 18 .426 | 0.21(1)⋆ | 6.7(4)⋆ | 15.1(9) | 450 ± 200† | 370 ± 180 | 2 ± 1 | 1472 | −2.18 ± 0.12 | 4, 38 |
| J1709+2313 | 25 .347 | 0.80(7) | 17(2) | 3.4(6) | ... | 30 ± 5 | 2.52 ± 0.07 | 430 | −2.1 ± 0.1 | 35 |
| J1713+0747 | 15 .992 | 0.44(4) | 9.5(8) | 11(1) | 250 ± 100 | 200 ± 20 | 36 | 430 | −1.5 ± 0.1 | 12, 4 |
| J1730−2304 | 9 .617 | 0.78(6) | 9.6(8) | 130(20) | 310 ± 120 | 350 ± 120 | 43 ± 6 | 436 | −1.8 ± 0.3 | 13, 4 |
| J1738+0333 | 33 .778 | 0.58(5) | 9.9(8) | 17(3) | ... | 50 ± 100 | 2 | 1400 | −1.4 ± 1 | 29, 22 |
| J1744−1134 | 3 .139 | 0.23(3)⋆ | 5.6(8)⋆ | 38(5) | 220 ± 100† | 160 ± 20 | 18 ± 2 | 436 | −1.85 ± 0.08 | 2, 38 |
| J1810+1744 | 39 .659 | 0.566(3) | 34.1(2) | 563(1) | ... | 240 ± 30 | 20 | 350 | −2.57 ± 0.16 | 14, 38 |
| J1816+4510 | 38 .887 | 0.69(2) | 21.7(8) | 83.5(5) | ... | 10 | 1.5 | 350 | −2 | 32 |
| J1853+1303 | 30 .570 | 0.75(6) | 18(2) | 18(2) | ... | 10 ± 20 | 0.4 ± 0.2 | 1400 | −1.4 ± 1 | 15, 22 |
| B1855+09 | 13 .300 | 0.85(4) | 15.9(8) | 32(3) | 450 ± 250 | 140 ± 30 | 32 ± 6 | 430 | −1.3 ± 0.2 | 16 |
| J1905+0400 | 25 .692 | 0.7(1) | 18(3) | 21(4) | ... | 1 ± 2 | 0.05 ± 0.01 | 1400 | −1.4 ± 1 | 33, 22 |
| J1911−1114 | 30 .975 | 0.64(6) | 18(2) | 38(4) | 260 ± 130 | 470 ± 110 | 31 ± 9 | 400 | −2.45 ± 0.06 | 17, 38 |
| J1918−0642 | 26 .554 | 1.9(1) | 24(2) | 38(3) | ... | 30 ± 5 | 5.9 ± 0.6 | 350 | −1.67 ± 0.06 | 18 |
| J1923+2515 | 18 .858 | 0.37(1)⋆ | 9.7(4)⋆ | 17(1) | ... | 15 ± 5 | 0.6 ± 0.2 | 820 | −1.7 | 28 |
| B1937+21 | 71 .040 | 0.697(6) | 44.7(4) | 370(2) | ... | 4950 ± 490 | 232 ± 25 | 430 | −2.59 ± 0.04 | 16, 38 |
| J1944+0907 | 24 .34 | 1.48(2) | 28.6(4) | 81(2) | ... | 20 ± 20 | 3.9 ± 0.3 | 430 | −1.4 ± 1 | 19, 22 |
| B1953+29 | 104 .501 | 1.98(5) | 32.3(8) | 38(1) | ... | 200 ± 80 | 15 ± 5 | 430 | −2.2 ± 0.3 | 20, 4 |
| B1957+20 | 29 .117 | 0.576(6) | 35.8(4) | 155(1) | ... | 400–1300 |
~
|
430 | −2.79 ± 0.11 | 21, 38 |
| J2019+2425 | 17 .203 | 0.51(6) | 13(2) | 6(1) | 190 ± 100 | 15 ± 15 | 2.7 ± 0.7 | 430 | −1.4 ± 1 | 26, 22 |
| J2043+1711 | 20 .710 | 0.415(9)⋆ | 17.4(4)⋆ | 34(1) | ... | 3 ± 2 | 0.8 | 350 | −1.4 ± 1 | 14, 22 |
| J2051−0827 | 20 .745 | 0.48(2)⋆ | 10.7(4)⋆ | 43(3) | 250 ± 100† | 180 ± 60 | 22 | 436 | −1.8 ± 0.3 | 23, 4 |
| J2145−0750 | 8 .998 | 1.17(2)⋆ | 7.3(1)⋆ | 162(2) | 480 ± 120 | 470 ± 130 | 100 ± 30 | 436 | −1.33 ± 0.18 | 2, 38 |
| J2214+3000 | 22 .557 | 0.47(5) | 15(2) | 5.4(7) | ... | 30 ± 40 | 2.1 | 820 | −1.4 ± 1 | 27, 22 |
| J2215+5135 | 69 .2 | 0.76(1) | 29.0(4) | 53(2) | ... | 120 ± 20 | 5 | 350 |
|
14, 38 |
| J2235+1506 | 18 .09 | 2.5(2)⋆ | 4.2(4)⋆ | 6(1) | 170 ± 80 ‡ | 15 ± 15 | 3 | 430 | −1.4 ± 1 | 12, 22 |
| J2302+4442 | 13 .762 | 0.64(4) | 12.4(8) | 8.8(7) | ... | 30 ± 60 | 1.2 ± 0.4 | 1400 | −1.4 ± 1 | 24, 22 |
| J2317+1439 | 21 .907 | 0.27(1)⋆ | 7.7(4)⋆ | 37.9(8) | 90 ± 50 | 90 ± 30 | 19 ± 5 | 430 | −1.4 ± 0.3 | 25, 4 |
| J2322+2057 | 13 .372 | 0.3(2) | 7(3) | 2(1) | 75 ± 40 | 15 ± 15 | 2.8 ± 1.2 | 430 | −1.4 ± 1 | 25, 22 |
Notes. Smean errors in parentheses are only nominal uncertainties. The realistic uncertainties are estimated to be within 50% of the actual flux density values (see Sect. 3.2.2). Flux densities by Kuzmin & Losovsky (2001, KL01) are at 102 or 111 MHz.
Observations were done both at 102 and 111 MHz, and it is not clear for which frequency the flux densities were reported.
Subject to substantial intrinsic variability, as pointed out by both Archibald et al. (2009) and Deller et al. (2012).
Reference. (1) Lommen et al. (2000); (2) Toscano et al. (1998); (3) Navarro et al. (1995); (4) Kramer et al. (1998); (5) Burgay et al. (2006); (6) Lundgren et al. (1995); (7) Nicastro et al. (1995); (8) Sayer et al. (1997); (9) Archibald et al. (2009); (10) Bailes et al. (1997); (11) Wolszczan & Frail (1992); (12) Camilo (1995); (13) Lorimer et al. (1995); (14) Hessels et al. (2011); (15) Stairs et al. (2005); (16) Foster et al. (1991); (17) Lorimer et al. (1996); (18) Janssen et al. (2010); (19) Champion et al. (2005); (20) Boriakoff et al. (1984); (21) Fruchter et al. (1990); (22) Bates et al. (2013); (23) Stappers et al. (1996); (24) Cognard et al. (2011); (25) Camilo et al. (1996b); (26) Nice et al. (1993); (27) Ransom et al. (2011); (28) Lynch et al. (2013); (29) Jacoby (2005); (30) Ransom et al. (2014); (31) Deller et al. (2012); (32) Stovall et al. (2014a); (33) Hobbs et al. (2004a); (34) Lorimer et al. (2005); (35) Lewandowski et al. (2004); (36) Lorimer et al. (2007); (37) Bhattacharyya et al. (2013); (38) Kuniyoshi et al. (2015).
Current usage metrics show cumulative count of Article Views (full-text article views including HTML views, PDF and ePub downloads, according to the available data) and Abstracts Views on Vision4Press platform.
Data correspond to usage on the plateform after 2015. The current usage metrics is available 48-96 hours after online publication and is updated daily on week days.
Initial download of the metrics may take a while.