Table 1.
LoTSS sources selected as pulsar candidates based on their polarisation properties.
LoTSS source | Field | l | b | S144 | p | RM | ![]() |
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---|---|---|---|---|---|---|---|---|---|
(°) | (°) | (mJy) | (%) | (rad m−2) | (pc cm−3) | (rad m−2) | |||
Linearly polarised | L/I | ||||||||
ILT J024831.01+423020.3* | P044+44 | 144.88 | −15.32 | 9.0 | 41 | −37.8 | 94.8 | 103.9 | −52 |
ILT J042737.00+684536.9 | P068+69 | 140.49 | +13.63 | 16.0 | 7 | −72.7 | 103.6 | 137.4 | −44 |
ILT J095618.49+461712.5 | P149+47 | 171.92 | +50.68 | 5.7 | 82 | 8.1 | 37.2 | 24.9 | 5 |
ILT J104140.11+542419.3 | P160+55 | 154.93 | +53.90 | 1.8 | 31 | 2.1 | 34.6 | 24.0 | 2 |
ILT J104937.86+582217.6⋆ | P161+60 | 148.65 | +52.24 | 2.0 | 64 | 4.0 | 35.0 | 25.0 | 10 |
ILT J105132.39+591355.8 | P161+60 | 147.36 | +51.83 | 5.6 | 17 | 8.2 | 35.1 | 25.2 | 7 |
ILT J140326.96+490750.2 | P211+50 | 95.48 | +63.98 | 23.6 | 8 | 12.7 | 30.0 | 22.2 | 13 |
ILT J163035.93+355042.5† | P249+38 | 57.88 | +43.08 | 5.9 | 33 | 8.5 | 34.9 | 29.5 | 13 |
ILT J172307.05+651557.0 | P260+65 | 95.17 | +33.65 | 19.2 | 8 | 31.7 | 43.9 | 38.0 | 25 |
Circularly polarised | |V|/I | ||||||||
ILT J003904.45+625711.4 | P007+64 | 121.53 | +0.12 | 20.7 | 5 ± 2 | – | 238.5 | 332.7 | −204 |
ILT J012902.97+191907.6 | P024+21 | 135.04 | −42.68 | 62 | 22 ± 6 | – | 39.8 | 30.6 | −43 |
ILT J013942.10+312331.5 | P024+31 | 134.87 | −30.36 | 24.1 | 2 ± 1 | – | 51.6 | 43.7 | −65 |
ILT J022042.12+362655.7† | P035+36 | 142.32 | −23.04 | 24.5 | 4 ± 1 | – | 66.4 | 63.7 | −75 |
ILT J024340.68+265149.7 | P039+26 | 151.80 | −29.64 | 15.4 | 5 ± 1 | – | 54.8 | 49.4 | −77 |
ILT J074212.22+411015.0† | P114+39 | 178.13 | +26.57 | 7.5 | 7 ± 2 | – | 63.1 | 68.6 | 6 |
ILT J101650.83+433122.4 | P153+42 | 174.86 | +54.89 | 19.0 | 3 ± 1 | – | 35.3 | 22.6 | 5 |
ILT J114600.31+504733.8 | P16Hetdex13 | 146.25 | +63.27 | 8.6 | 5 ± 1 | – | 29.7 | 21.1 | 11 |
ILT J115553.76+574020.9 | P176+60 | 136.92 | +57.92 | 236 | 2 ± 1 | – | 32.3 | 23.2 | 5 |
ILT J120106.46+284839.3 | P181+27 | 201.40 | +78.77 | 18.5 | 4 ± 1 | – | 20.0 | 18.9 | 9 |
ILT J120223.78+611016.4 | P180+62 | 133.21 | +54.97 | 7.8 | 6 ± 1 | – | 33.2 | 24.4 | 14 |
ILT J152745.28+545324.7 | P232+55 | 88.28 | +50.39 | 9.4 | 4 ± 1 | – | 33.8 | 26.2 | −2 |
ILT J153514.64+483659.6 | P231+50 | 78.38 | +51.86 | 84.5 | 2 ± 1 | – | 33.5 | 25.6 | 7 |
ILT J154721.26+493621.5 | P236+48 | 78.90 | +49.66 | 6.5 | 5 ± 1 | – | 34.3 | 26.4 | 11 |
ILT J160218.82+390101.5⋆ | P242+38 | 62.18 | +48.79 | 27 | 9 ± 2 | – | 29.9 | 26.6 | 14 |
ILT J163607.29+314631.5 | P250+33 | 52.63 | +41.40 | 16.3 | 4 ± 1 | – | 36.1 | 30.6 | 20 |
ILT J164033.62+541943.4 | P250+55 | 82.67 | +40.61 | 31.0 | 2 ± 1 | – | 38.5 | 31.2 | 9 |
ILT J181551.08+390739.3 | P272+40 | 66.41 | +23.24 | 33.7 | 5 ± 1 | – | 61.3 | 51.5 | 78 |
ILT J212311.55+210431.7 | P320+23 | 71.25 | −20.28 | 5.2 | 14 ± 4 | – | 68.3 | 57.1 | −71 |
ILT J221227.63+245036.7† | P333+26 | 82.96 | −25.43 | 8.3 | 6 ± 1 | – | 55.0 | 46.9 | −82 |
ILT J222741.77+303820.8† | P336+31 | 89.72 | −22.81 | 17.0 | 7 ± 2 | – | 60.5 | 52.0 | −156 |
Notes. Columns provide the LoTSS catalogue source name, based on the right ascension and declination in the ILT Jhhmmss.ss+ddmmss.s format and with uncertainties (Shimwell et al. 2022); LoTSS observing field identifier; source location in Galactic longitude and latitude; total Stokes I flux density at 144 MHz with 3% median fractional uncertainty (Shimwell et al. 2022); linear or circular fractional polarisation percentage (O’Sullivan et al., in prep.; Callingham et al., in prep.); RM measured from the RM GRID processing (only applicable to linearly polarised sources) with uncertainties ≈0.1 rad m−2 including ionospheric RM correction (O’Sullivan et al., in prep.); maximum DM expected for the source line of sight using Galactic electron density models: NE2001 and YMW16 (see Sect. 2); maximum Galactic RM expected for the source line of sight using the Faraday Sky 2020 reconstruction with 22% median fractional uncertainty (see Sect. 2). LoTSS sources associated with the TULIPP pulsar discoveries or re-detections of known pulsars are noted using ⋆ and †, respectively, and they are also summarised in Table 2. Furthermore, the LoTSS source noted using * is coincident with PSR J0248+4230, recently discovered using the GMRT at 322 MHz (Bhattacharyya et al. 2021) and further discussed in Sect. 5.2.
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