2025A&A...696A.222M


Query : 2025A&A...696A.222M

2025A&A...696A.222M - Astronomy and Astrophysics, volume 696A222 (2025/4-1)

MeerKAT discovers a jet-driven bow shock near GRS 1915+105 How an invisible large-scale jet sculpts a microquasar's environment.

MOTTA S.E., ATRI P., MATTHEWS J.H., VAN DEN EIJNDEN J., FENDER R.P., MILLER-JONES J.C.A., HEYWOOD I. and WOUDT P.

Abstract (from CDS):

Context. Black holes, both supermassive and stellar-mass, impact the evolution of their surroundings on a large range of scales. While the role of supermassive black holes is well studied, the effects of stellar-mass black holes on their surroundings, particularly in inducing structures in the interstellar medium (ISM), remain under explored.
Aims. This study focuses on the black hole X-ray binary GRS 1915+105, renowned for its active jets, and the primary aim is to unveil and characterise the impact of GRS 1915+105 on its environment by identifying structures induced by jet-ISM interaction.
Methods. We observed GRS 1915+105 with MeerKAT for a total exposure time of 14 hr, and we obtained the deepest image of GRS 1915+105 to date. Using a previously proposed self-similar model for large-scale jets, we inferred the properties of both the jets and the ISM, providing insights into the jet-ISM interaction site.
Results. Our observations revealed a bow shock structure near GRS 1915+105, likely induced by a jet interacting with the ISM and blowing an overpressured cavity in the medium. We constrained the ISM density to 100-160 particles cm–3 while assuming a temperature range of 104-106 K, which implies a bow shock expansion velocity of $ 20\,\mathrm{km\,s}^{-1} < \dot{L} < 360\,\mathrm{km\,s}^{-1} $. We estimate that the jet responsible for the formation of the bow shock has an age between 0.09 and 0.22 Myr, and the time-averaged energy rate transferred by such jets into the ISM is constrained to 3.3 × 1037 ergs s$ ^{-1} < Q_{\mathrm{jet}}^{a} < 1.5 \times 10^{39} $ ergs s–1.
Conclusions. Our results confirm that in stellar-mass black holes, the energy dissipated through jets can be comparable to the accretion energy, and through the interaction of the jet with the ISM, such energy is transferred back to the environment. This feedback mechanism mirrors the powerful influence of supermassive black holes on their environments, underscoring the significant role a black hole's activity has in shaping its surroundings.

Abstract Copyright: © The Authors 2025

Journal keyword(s): accretion - accretion disks - binaries: general - stars: black holes - ISM: general - ISM: jets and outflows

Simbad objects: 12

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Number of rows : 12
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 NGC 300 GiG 00 54 53.4465638304 -37 41 03.168402396 8.83 8.69 8.13 7.46   ~ 1614 2
2 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
3 V* BR Cir HXB 15 20 40.8532547060 -57 10 00.206639033   21.4 21.4     B5-A0I 849 1
4 SS 433 HXB 19 11 49.5647697480 +04 58 57.827127648   16.854 14.643     A7Ib 2253 4
5 IRAS 19124+1106 IR 19 14 45 +11 12.1           ~ 26 0
6 Granat 1915+105 HXB 19 15 11.55576 +10 56 44.9052           ~ 2810 0
7 IRAS 19132+1035 Y*O 19 15 38.97768 +10 41 14.4276           ~ 51 0
8 CHIMPS 4894 MoC 19 15 51.9269 +10 46 51.192           ~ 2 0
9 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4590 0
10 MCG+07-41-003 Bla 19 59 28.35656837 +40 44 02.0972325   16.22 15.10     ~ 2537 2
11 LBN 071.58+02.86 HII 19 59 55 +35 16.6           ~ 37 0
12 NGC 7793 GiG 23 57 49.7540045856 -32 35 27.701550744 10.26 9.74 9.28 9.06 9.7 ~ 1188 2

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