2026A&A...706A.140B


Query : 2026A&A...706A.140B

2026A&A...706A.140B - Astronomy and Astrophysics, volume 706A140 (2026/2-1)

The environment of TeV halo progenitors.

BOURGUINAT L.-M., EVOLI C., MARTIN P. and RECCHIA S.

Abstract (from CDS):

Context. TeV haloes are extended sources of very-high-energy gamma rays found around some middle-aged pulsars. The emission spanning several tens of parsecs suggests an efficient confinement of the ultra-relativistic lepton pairs produced by pulsars in their vicinity. The physical mechanism responsible for this suppressed transport has not yet been identified. In some scenarios, pair confinement may be linked to the medium the pulsars are located in.
Aims. We aim at understanding the type of medium pulsars probe over their lifetime.
Methods. We developed a model for the environment probed by moving pulsars, from their birth in core-collapse explosions - where they receive a natal kick - until their entry into the interstellar medium. The model involves: (i) a Monte-Carlo sampling of the properties of the massive-star progenitors of pulsars; (ii) a calculation of the structure of the surrounding medium shaped by these progenitors for the two cases of isolated stars and star clusters; and (iii) a computation of the evolution of supernova remnants in these parent environments. Ultimately, from a distribution of neutron star kick velocities, we assess the medium in which pulsars are located as a function of time. We first derived the statistical properties of a fully synthetic Galactic population and then applied the model to a selection of known pulsars to assess the likely nature of their environment.
Results. We show that pulsars escape into the interstellar medium at around 300 kyr, significantly later than assumed in the literature. Given our assumptions, all known pulsars with a confirmed TeV halo have high probabilities of still being in their parent environment, which suggests that efficient pair confinement is connected to the region influenced by progenitor stars. To test this, we provide the probability that known pulsars still reside in their parent environment for a list of known pulsars.

Abstract Copyright: © The Authors 2026

Journal keyword(s): astroparticle physics - pulsars: general - ISM: bubbles - ISM: supernova remnants

Simbad objects: 56

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Number of rows : 56
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 B0114+58 Psr 01 17 38.661 +59 14 38.39           ~ 96 0
2 PSR J0212+5222 Psr 02 12 52.136 +52 22 49.50           ~ 12 0
3 PSR J0248+6021 Psr 02 48 18.642 +60 21 34.70           ~ 63 1
4 PSR J0357+32 Psr 03 57 52.161 +32 05 23.63           ~ 104 0
5 PSR B0355+54 Psr 03 58 53.7165 +54 13 13.727           ~ 465 1
6 PSR J0426+4933 Psr 04 26 06.813 +49 33 38.46           ~ 9 0
7 PSR J0538+2813 Psr 05 38 25.06 +28 17 11.0           ~ 224 1
8 SNR G180.0-01.7 SNR 05 39 00.000 +27 50 00.00           ~ 294 2
9 PSR B0540+23 Psr 05 43 09.65 +23 29 06.1     14.40     ~ 278 0
10 PSR J0554+3107 Psr 05 54 04.83 +31 07 41.7           ~ 27 0
11 PSR J0622+3749 Psr 06 22 10.411 +37 49 14.60           ~ 58 0
12 PSR J0631+10 Psr 06 31 27.369 +10 37 05.63           ~ 152 0
13 PSR J0633+0632 Psr 06 33 44.136 +06 32 29.48           ~ 93 1
14 PSR J0633+1746 Psr 06 33 54.153 +17 46 12.91           ~ 1308 0
15 NAME MONOGEM SNR SNR 06 58 50 +13 55.9           ~ 124 0
16 PSR B0656+14 Psr 06 59 48.18800 +14 14 19.2000   24.85 24.90     ~ 943 1
17 PSR B0727-18 Psr 07 29 32.2900 -18 36 42.210           ~ 102 0
18 PSR B0740-28 Psr 07 42 49.0730 -28 22 43.510           ~ 445 0
19 PSR J0835-3707 Psr 08 35 03.08 -37 07 51.5           ~ 17 0
20 PSR J0905-5127 Psr 09 05 51.922 -51 27 48.71           ~ 51 0
21 PSR B0906-49 Psr 09 08 35.46000 -49 13 05.0000           ~ 168 0
22 PSR B0919+06 Psr 09 22 13.85000 +06 38 19.0000           ~ 329 1
23 PSR B0922-52 Psr 09 24 08.72200 -53 02 42.6000           ~ 48 0
24 PSR J0940-5428 Psr 09 40 58.22 -54 28 40.6           ~ 61 0
25 PSR B0940-55 Psr 09 42 14.88000 -55 52 55.1000           ~ 101 0
26 PSR B0941-56 Psr 09 42 54.42200 -56 57 43.2100           ~ 54 0
27 PSR J0954-5430 Psr 09 54 06.04 -54 30 53.5           ~ 34 0
28 PSR B0959-54 Psr 10 01 37.85000 -55 07 07.8000           ~ 113 0
29 PSR J1028-5819 Psr 10 28 27.888 -58 19 06.14           ~ 122 1
30 PSR J1044-5737 Psr 10 44 32.791 -57 37 19.39           ~ 44 0
31 PSR B1055-52 Psr 10 57 59.0450 -52 26 56.330           ~ 757 0
32 PSR B1133-55 Psr 11 36 02.23540 -55 25 06.8430           ~ 56 0
33 PSR J1152-6012 Psr 11 52 53.8 -60 12 21           ~ 7 0
34 PSR J1301-6310 Psr 13 01 28.30 -63 10 40.5           ~ 14 1
35 PSR J1429-5911 Psr 14 29 58.564 -59 11 36.02           ~ 37 1
36 PSR J1459-60 Psr 14 59 30.1228633008 -60 53 20.536602864           ~ 60 0
37 PSR J1530-5327 Psr 15 30 26.87 -53 27 56.3           ~ 32 0
38 PSR J1549-4848 Psr 15 49 21.02700 -48 48 36.1000           ~ 55 0
39 PSR B1727-47 Psr 17 31 42.21000 -47 44 38.7000           ~ 166 0
40 PSR J1732-31 Psr 17 32 33.551 -31 31 20.85           ~ 78 0
41 PSR J1740+1000 Psr 17 40 25.91 +10 00 06.0           ~ 110 0
42 PSR J1741-2054 Psr 17 41 57.282 -20 54 04.11           ~ 123 1
43 PSR B1742-30 Psr 17 45 56.30810 -30 40 23.3000           ~ 182 0
44 SNR G007.5-01.7 SNR 18 09 -23.3           ~ 15 0
45 PSR J1809-2332 Psr 18 09 50.250 -23 32 22.68     21.47 19.61 17.48 M5 103 0
46 PSR B1822-09 Psr 18 25 30.62000 -09 35 22.0000           ~ 382 0
47 PSR J1846+0919 Psr 18 46 25.864 +09 19 48.99           ~ 40 0
48 PSR J1848+0651 Psr 18 48 56.01 +06 47 31.7           ~ 10 0
49 PSR B1847-03.3 Psr 18 49 57.85 -03 17 31.0           ~ 15 0
50 PSR B1916+14 Psr 19 18 23.638 +14 45 06.00           ~ 130 0
51 PSR J1954+2836 Psr 19 54 19.144 +28 36 04.84           ~ 62 0
52 PSR J1957+5033 Psr 19 57 38.391 +50 33 21.24           ~ 45 0
53 PSR J2017-2737 Psr 20 17 01.63 -27 30 49.2           ~ 2 0
54 PSR J2030+4415 Psr 20 30 51.396 +44 15 38.73           ~ 68 0
55 [MT91] 213 Psr 20 32 13.1247390384 +41 27 24.346666440 13.12 13.08 11.266     B0Vp 334 0
56 PSR B2334+61 Psr 23 37 05.779 +61 51 01.69           ~ 206 1

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