2025MNRAS.539.2665M


Query : 2025MNRAS.539.2665M

2025MNRAS.539.2665M - Mon. Not. R. Astron. Soc., 539, 2665-2684 (2025/May-3)

Blast waves and reverse shocks: from ultra-relativistic GRBs to moderately relativistic X-ray binaries.

MATTHEWS J.H., COOPER A.J., RHODES L., SAVARD K., FENDER R., CAROTENUTO F., COWIE F.J., ELLEY E.L., BRIGHT J., HUGHES A.K. and MOTTA S.E.

Abstract (from CDS):

Blast wave models are commonly used to model relativistic outflows from ultra-relativistic gamma-ray bursts (GRBs), but are also applied to lower Lorentz factor ejections from X-ray binaries (XRBs). Here, we revisit the physics of blast waves and reverse shocks in these systems and explore the similarities and differences between the ultra-relativistic ($\Gamma \gg 1$) and moderately relativistic ($\Gamma \sim {\rm a~few}$) regimes. We first demonstrate that the evolution of the blast wave radius as a function of the observer frame time is recovered in the on-axis ultra-relativistic limit from a general energy and radius blast wave evolution, emphasizing that XRB ejections are off-axis, moderately relativistic cousins of GRB afterglows. We show that, for fixed blast wave or ejecta energy, reverse shocks cross the ejecta much later (earlier) on in the evolution for less (more) relativistic systems, and find that reverse shocks are much longer lived in XRBs and off-axis GRBs compared to on-axis GRBs. Reverse shock crossing should thus typically finish after $\sim$10-100 of days (in the observer frame) in XRB ejections. This characteristic, together with their moderate Lorentz factors and resolvable core separations, makes XRB ejections unique laboratories for shock and particle acceleration physics. We discuss the impact of geometry and lateral spreading on our results, explore how to distinguish between different shock components, and comment on the implications for GRB and XRB environments. Additionally, we argue that identification of reverse shock signatures in XRBs could provide an independent constraint on the ejecta Lorentz factor.

Abstract Copyright: © 2025 The Author(s). Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): acceleration of particles - hydrodynamics - shock waves - gamma-ray burst: general - ISM: jets and outflows - X-rays: binaries

Simbad objects: 73

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Number of rows : 73
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 GRB 060912A gB 00 21 08.11 +20 58 18.9           ~ 116 1
2 GRB 071031 gB 00 25 37.40 -58 03 33.9           ~ 184 0
3 GRB 050904 gB 00 54 50.794 +14 05 09.42           ~ 496 0
4 GRB 201216C gB 01 05 28.88 +16 30 58.0           ~ 89 0
5 GRB 100906A gB 01 54 44.19 +55 37 49.8           ~ 233 0
6 GRB 191016A gB 02 01 04.67 +24 30 35.3           ~ 31 0
7 GRB 060908 gB 02 07 18.360 +00 20 31.20 16.99 18.34 16.85     ~ 217 0
8 GRB 070721B gB 02 12 32.98 -02 11 39.8           ~ 128 0
9 GRB 071112C gB 02 36 50.89 +28 22 16.9           ~ 164 0
10 GRB 060906 gB 02 43 00.900 +30 21 42.12     19.84     ~ 147 0
11 GRB 070318 gB 03 13 56.830 -42 56 46.30 18.27 16.23 15.49     ~ 170 0
12 GRB 060115 gB 03 36 08.400 +17 20 43.00           ~ 179 0
13 GRB 190114C gB 03 38 01.18 -26 56 47.8           ~ 343 0
14 GRB 060210 gB 03 50 57.370 +27 01 34.40   20.27       ~ 275 0
15 GRB 121024A gB 04 41 53.31 -12 17 26.1           ~ 143 0
16 GRB 060124 gB 05 08 25.900 +69 44 26.98   18.91 17.35     ~ 280 0
17 GRB 110801A gB 05 57 44.87 +80 57 21.1           ~ 90 0
18 Fermi bn080928628 gB 06 20 16.85 -55 11 59.3           ~ 187 0
19 GRB 060729 gB 06 21 31.850 -62 22 12.69           ~ 303 0
20 SN 2002lt SN* 08 08 59.858 +06 43 37.52           SNIc: 363 1
21 GRB 051016B gB 08 48 27.810 +13 39 20.00 20.45         ~ 153 0
22 GRB 061021 gB 09 40 36.120 -21 57 05.40 18.21 19.20 16.82     ~ 160 0
23 GRB 070306 gB 09 52 23.220 +10 28 55.20           ~ 222 1
24 GRB 071010B gB 10 02 09.20 +45 43 52.2           ~ 173 0
25 GRB 050319 gB 10 16 47.900 +43 32 53.80   18.02 17.01     ~ 274 0
26 GRB 100219A gB 10 16 48.48 -12 34 00.0           ~ 130 0
27 SN 2003dh SN* 10 44 50.030 +21 31 18.15     16.2     SNIcpec 1261 1
28 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
29 GRB 140515A gB 12 24 15.48 +15 06 17.7           ~ 90 0
30 GRB 050416 gB 12 33 54.600 +21 03 26.69     19.12     ~ 300 1
31 Fermi bn121211574 gB 13 02 07.99 +30 08 54.6           ~ 99 0
32 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
33 GRB 070208 gB 13 11 32.607 +61 57 54.37 20.79 20.79 19.86     ~ 119 0
34 MAXI J1348-630 HX? 13 48 12.7388336424 -63 16 29.709083208           ~ 201 0
35 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 508 0
36 GRB 050802 gB 14 37 05.820 +27 47 12.62 16.85 17.38 16.97     ~ 186 0
37 GRB 060814 gB 14 45 21.480 +20 35 11.80           ~ 241 0
38 GRB 060714 gB 15 11 26.450 -06 33 58.30   20.21 18.54     ~ 209 0
39 GRB 990123 gB 15 25 29 +44 45.0     8.95     ~ 1012 1
40 GRB 060526 gB 15 31 18.360 +00 17 04.90   18.31 17.16     ~ 288 0
41 MAXI J1535-571 XB* 15 35 19.73 -57 13 48.1           ~ 214 0
42 GRB 060418 gB 15 45 42.600 -03 38 20.00 15.73 16.19 14.98     ~ 389 0
43 V* IL Lup HXB 15 47 08.2768672752 -47 40 10.284587760         15.624 ~ 532 1
44 V* V381 Nor HXB 15 50 58.6637920704 -56 28 35.258385000           K3III 1254 0
45 GRB 140629A gB 16 35 54.44 +41 52 36.7           ~ 89 0
46 GRB 130606A gB 16 37 35.12 +29 47 46.4           ~ 185 0
47 GRB 080210 gB 16 45 04.03 +13 49 36.3           ~ 121 0
48 GRB 080319C gB 17 15 55.48 +55 23 31.7           ~ 174 0
49 GRB 050814 gB 17 36 45.390 +46 20 21.60           ~ 166 0
50 XTE J1752-223 LXB 17 52 15.090 -22 20 32.36           ~ 229 0
51 V* V4641 Sgr HXB 18 19 21.6343259256 -25 24 25.849595952     13.654 13.479 13.139 B9III 530 0
52 MAXI J1820+070 LXB 18 20 21.9423816480 +07 11 07.284859440           ~ 511 0
53 SN 2005nc SN* 18 32 32.560 +26 20 22.34           SNIc: 400 1
54 Fermi bn081008832 gB 18 39 52.40 -57 25 58.8           ~ 224 0
55 Fermi bn110731465 gB 18 42 00.99 -28 32 13.8           ~ 193 0
56 AX J1848.8-0129 X 18 48 48 -01 29.2           ~ 27 0
57 SS 433 HXB 19 11 49.5647697480 +04 58 57.827127648   16.854 14.643     A7Ib 2253 4
58 GRB 221009A gB 19 13 03.85 +19 46 22.7           ~ 433 0
59 Granat 1915+105 HXB 19 15 11.55576 +10 56 44.9052           ~ 2810 0
60 Fermi bn140512814 gB 19 17 28.81 -15 05 39.5           ~ 133 0
61 GRB 071003A gB 20 07 25 +10 56.9           ~ 7 0
62 GRB 160625B gB 20 34 23.67 +06 55 11.1           ~ 235 0
63 Fermi bn160509374 gB 20 47 00.90 +76 06 30.1           ~ 141 0
64 GRB 130427B gB 20 59 36.00 -22 32 51.6           ~ 60 0
65 GRB 050922C gB 21 09 33.000 -08 45 30.10 15.15 15.86 14.69     ~ 301 0
66 GRB 181201A gB 21 17 11.20 -12 37 50.9           ~ 60 0
67 LEDA 68751 Sy1 22 23 49.5398449645 -02 06 12.856394895   16.93 15.77 16.02   ~ 511 2
68 GRB 050820A gB 22 29 38.110 +19 33 37.10 18.33 19.00 18.47     ~ 409 0
69 GRB 081029A gB 23 07 05.35 -68 09 19.8           ~ 5 0
70 GRB 051111A gB 23 12 33.170 +18 22 28.80 19.77 20.08 19.50     ~ 223 0
71 GRB 201015A gB 23 37 16.43 +53 24 57.6           ~ 74 0
72 Fermi bn080810549 gB 23 47 08.00 +00 18 35.1           ~ 240 0
73 GRB 060707 gB 23 48 19.000 -17 54 17.00     19.79     ~ 170 0

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