2025A&A...704A.308D


Query : 2025A&A...704A.308D

2025A&A...704A.308D - Astronomy and Astrophysics, volume 704A308 (2025/12-1)

Systemic recoil velocity distribution of field millisecond pulsar systems: Implications for neutron star retention in star clusters.

DING H.

Abstract (from CDS):

Aims. The systemic recoil velocity (vsys) distribution of millisecond pulsars (MSPs) is essential for understanding the MSP formation channel(s) and for estimating the retention fractions of MSPs in star clusters, which can potentially be determined using the precise astrometry of MSPs. However, the determination is complicated by the long-term dynamic evolution of MSPs and the scarcity of radial velocity measurements. The goal of this work is to overcome the complexity and derive the MSP vsys distribution from high-precision astrometric measurements.
Methods. We compiled 64 field MSP systems (including 52 binary MSPs and 12 solitary MSPs) that have been well determined astrometrically. We calculated their transverse peculiar (or space) velocities, v⊥, and Galactic heights, z. Assuming that the Galactic-longitude components, v1, of v⊥ are statistically stable over time (i.e. the 'stable- v1' assumption), we approached the distribution of the v1 components of vsys using the observed v1 sample. Under the 'isotropic- vsys' assumption that vsys directions are uniformly distributed, we derived the MSP vsys distribution from the distribution of the v1 component of vsys. Based on the derived vsys distribution, we tested the stable- v1 assumption with dynamical population synthesis (DPS). In addition, by matching the observed z and the Galactic-latitude components, vb, of v⊥ to the DPS counterparts, we estimated the initial and the current Galaxy-wide scale heights of field MSP systems.
Results. We find that solitary field MSPs have similar v1 magnitudes to those of binary ones. Additionally, the observed v1 can be well described by a linear combination of three normal distributions. Accordingly, the MSP vsys distribution can be approximated by a linear combination of three Maxwellian components. Our DPS analysis verified the stable- v1 assumption in the parameter space of this work and estimated the initial and the current Galaxy-wide scale heights of field MSP systems to be about 0.32 kpc and 0.68 kpc, respectively.
Conclusions. According to the MSP vsys distribution, ≈14% of all the MSPs born in a globular cluster with the nominal 50 km s–1 central escape velocity can be retained. Therefore, the vsys distribution of field MSP systems may account for the high number of MSPs discovered in globular clusters, which implies that MSPs in star clusters might follow the same formation channel(s) as field MSP systems.

Abstract Copyright: © The Authors 2026

Journal keyword(s): astrometry - parallaxes - proper motions - stars: kinematics and dynamics - stars: neutron - pulsars: general

Simbad objects: 70

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Number of rows : 70
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 PSR J0023+0923 Psr 00 23 16.890 +09 23 24.18           ~ 137 0
2 PSR J0030+0451 Psr 00 30 27.42348 +04 51 39.7144           ~ 596 1
3 PSR J0125-23 Psr 01 25 01.075151 -23 27 08.13167           ~ 20 0
4 PSR J0437-47 Psr 04 37 15.7994581776 -47 15 08.544351636           DC 1032 0
5 V* CM Tau Psr 05 34 31.9474694616 +22 00 52.153698024           ~ 5476 0
6 PSR J0610-2100 Psr 06 10 13.602953 -21 00 27.74435           ~ 116 0
7 PSR B0613-02.0 Psr 06 13 43.977070 -02 00 47.34294           ~ 319 1
8 PSR J0614-3329 Psr 06 14 10.3479 -33 29 54.116           ~ 134 1
9 PSR J0621+10 Psr 06 21 22.11108 +10 02 38.7410           ~ 128 1
10 PSR J0636+5129 Psr 06 36 04.84645 +51 28 59.9625           ~ 101 0
11 PSR J0636-3044 Psr 06 36 34.398358 -30 44 01.10761           ~ 11 0
12 PSR J0645+5158 Psr 06 45 59.08191 +51 58 14.9210           ~ 65 0
13 PSR J0737-3039A Psr 07 37 51.24669 -30 39 40.6895           ~ 317 1
14 PSR J0751+1807 Psr 07 51 09.1539 +18 07 38.335           ~ 316 1
15 PSR J1012+5307 Psr 10 12 33.4345449600 +53 07 02.548542576     19.5     DA 419 1
16 PSR J1022+10 Psr 10 22 57.990 +10 01 52.92           ~ 279 2
17 PSR J1023+0038 Psr 10 23 47.6841824712 +00 38 41.005893516     17.31     GV 470 0
18 PSR J1025-07 Psr 10 24 38.6991893112 -07 19 19.045523388     19.81 18.78 18.00 ~ 286 1
19 PSR J1125-6014 Psr 11 25 55.243299 -60 14 06.80942           ~ 61 0
20 XSS J12270-4859 Psr 12 27 58.7476831464 -48 53 42.824592960           ~ 321 0
21 PSR B1257+12 Psr 13 00 03.1075 +12 40 55.155           ~ 546 1
22 PSR J1400-1431 Psr 14 00 37.00370 -14 31 47.0422           ~ 49 0
23 PSR J1417-4402 Psr 14 17 30.5732900514 -44 02 57.497992802     15.84     ~ 32 0
24 PSR J1431-4715 Psr 14 31 44.6313693632 -47 15 27.399549133           ~ 49 0
25 PSR J1446-4701 Psr 14 46 35.709721 -47 01 26.79678           ~ 82 1
26 PSR J1455-3300 Psr 14 55 47.976991 -33 30 46.40280           ~ 165 1
27 PSR J1518+4904 Psr 15 18 16.832 +49 04 34.19           ~ 201 1
28 PSR B1534+11 Psr 15 37 09.9603 +11 55 55.554           ~ 453 1
29 PSR J1545-4550 Psr 15 45 55.945403 -45 50 37.50813           ~ 34 0
30 PSR J1600-3053 Psr 16 00 51.902514 -30 53 49.45343           ~ 218 0
31 PSR J1614-2230 Psr 16 14 36.50974 -22 30 31.5420           ~ 452 1
32 PSR J1629-6902 Psr 16 29 08.744211 -69 02 45.46922           ~ 22 0
33 PSR J1640+2224 Psr 16 40 16.744850 +22 24 08.84119           ~ 210 0
34 PSR J1643-1224 Psr 16 43 38.16612 -12 24 58.6334           ~ 260 2
35 PSR J1658-5324 Psr 16 58 39.343556 -53 24 06.97315           ~ 47 0
36 PSR J1713+0747 Psr 17 13 49.5367813 +07 47 37.450240           ~ 530 1
37 PSR J1719-14 Psr 17 19 10.076221 -14 38 01.00200           ~ 92 2
38 PSR J1723-2837 Psr 17 23 23.1937506912 -28 37 57.210408048   16.81 15.77 15.71   ~ 105 0
39 PSR J1730-2304 Psr 17 30 21.68471 -23 04 31.2590           ~ 194 1
40 PSR J1738+0333 Psr 17 38 53.966386 +03 33 10.87200           ~ 191 1
41 PSR J1741+1351 Psr 17 41 31.1499024 +13 51 44.279709           ~ 122 0
42 PSR J1744-1134 Psr 17 44 29.4220844 -11 34 54.801320           ~ 323 1
43 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 16269 0
44 Cl Terzan 5 Cl* 17 48 05.00 -24 46 48.0           ~ 948 1
45 PSR J1756-5322 Psr 17 57 15.154960 -53 22 26.59604           ~ 56 0
46 PSR J1804-27 Psr 18 04 21.13307 -27 17 31.3370           ~ 87 1
47 PSR J1811-2405 Psr 18 11 19.854352 -24 05 18.42800           ~ 56 1
48 PSR J1832-0836 Psr 18 32 27.589497 -08 36 55.14540           ~ 86 0
49 PSR J1853+1303 Psr 18 53 57.3183 +13 03 44.088           ~ 107 1
50 PSR B1855+09 Psr 18 57 36.390620 +09 43 17.20712           DA 569 1
51 PSR J1909-3744 Psr 19 09 47.42820 -37 44 14.7740           ~ 343 2
52 PSR J1910+1256 Psr 19 10 09.701454 +12 56 25.48680           ~ 108 1
53 PSR J1911+1347 Psr 19 11 55.204694 +13 47 34.38383           ~ 72 0
54 PSR J1915+1606 Psr 19 15 27.99999 +16 06 27.4034     22.5     ~ 1032 1
55 PSR J1918-0642 Psr 19 18 48.027685 -06 42 34.95735           ~ 146 0
56 PSR J1933-6210 Psr 19 33 32.413330 -62 11 46.69324           ~ 48 0
57 PSR B1937+21.4 Psr 19 39 38.560096 +21 34 59.13552           ~ 1142 0
58 PSR J1946-5403 Psr 19 46 34.4933990 -54 03 42.558670           ~ 45 0
59 PSR J2043+1711 Psr 20 43 20.8828 +17 11 28.941           ~ 129 1
60 PSR J2124-3358 Psr 21 24 43.834930 -33 58 45.49195           ~ 337 1
61 PSR J2129-04 Psr 21 29 45.0469239408 -04 29 06.973600236     16.68     ~ 100 0
62 PSR B2145-07.8 Psr 21 45 50.45590 -07 50 18.5900           ~ 336 0
63 PSR J2222-0137 Psr 22 22 06.00015 -01 37 15.7827           ~ 78 0
64 PSR J2234+06 Psr 22 34 22 +06 11.0           ~ 76 0
65 PSR J2234+0944 Psr 22 34 46.856913 +09 44 30.04150           ~ 82 0
66 PSR J2241-5236 Psr 22 41 42.03161 -52 36 36.2492           ~ 143 1
67 PSR J2256-1024 Psr 22 56 56.390 -10 24 34.37           ~ 88 0
68 PSR J2317+1439 Psr 23 17 09.235606 +14 39 31.29559           ~ 211 1
69 PSR J2322+2057 Psr 23 22 22.320041 +20 57 02.50080           ~ 129 1
70 PSR J2322-2650 Psr 23 22 34.638615 -26 50 58.38398           ~ 35 0

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