2025A&A...698A..64R


Query : 2025A&A...698A..64R

2025A&A...698A..64R - Astronomy and Astrophysics, volume 698A64 (2025/6-1)

Candidate bow shock stars: Spectral analysis and environment.

RUSSEIL D., ZAVAGNO A., BOURET J.C. and ADAMI C.

Abstract (from CDS):

Aims. Infrared bow shocks are arc-shaped structures located ahead of a star and generally observed at mid- to far-IR wavelengths. They are thought to result from the interaction of the stellar wind with the ambient interstellar medium and are typically (but not always) related to runaway stars. However, the formation of bow shocks seems to be dominated by local environmental factors rather than stellar motion. In this context, we aim to probe the links between bow-shock driving stars and their environment.
Methods. We observed 47 bow shock driving star candidates with the Multi-purpose InSTRument for Astronomy at Low-resolution (MISTRAL) spectro-imager at Haute-Provence Observatory (OHP) in the 420-800 nm range to perform spectral classification of the candidate stars. In parallel, we evaluated the transverse motion of stars from GAIA DR3 in order to determine whether they are runaways. We then characterised the bow shock environmental conditions.
Results. We find that among the 47 candidates we have 3 unclassifiable stars (suspected to be G- or K-type stars), 3 M- or K-type stars, 2 A-type stars, 10 O stars, and 29 B (mainly giant and supergiant) stars. We find that 17 stars (among the 37 with determined transverse velocity) are runaways, among which only 7 have their transverse velocity aligned to the bow-shock axis. This suggests that runaway is not the only origin for bow shock formation. We note the diversity of environments where bow shocks are observed: stellar associations, a cluster, and H II regions. For most stars, the origin of the bow shock is not clear; however, the 11 bow shocks observed in the Cygnus OB stellar association suggest that the ISM conditions in such regions favour bow shock observability. We also identify that the bow shock ahead of the star ionising the H II region Sh2-135 could be produced by a photoevaporated flow of about 16 km/s coming from the H II region molecular cloud's interface. Finally, for six stars we were able to identify the cluster from which they were ejected and determine the ejection process (dynamical ejection from star cluster or binary supernovae scenarios).
Conclusions. The formation of bow shocks seems to be dominated by local environmental factors rather than stellar motion.

Abstract Copyright: © The Authors 2025

Journal keyword(s): circumstellar matter - stars: general - stars: winds, outflows - HII regions

Status at CDS : All or part of tables of objects will not be ingested in SIMBAD.

Simbad objects: 60

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Number of rows : 60
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 * 5 Per s*b 02 11 29.1934233120 +57 38 43.964680956 6.23 6.68 6.35 6.02 5.75 B5Ia 191 0
2 NAME Per Arm PoG 03 30 +45.0           ~ 1672 0
3 * lam Lep ** 05 19 34.5223081894 -13 10 36.369844928 3.03 4.04 4.29 4.41 4.69 B0.5V 322 0
4 LHA 120-N 131 HII 05 22 52.7 -69 50 58           ~ 11 0
5 * sig Ori Y*O 05 38 44.7653828520 -02 36 00.283179888 2.54 3.58 3.79 3.87 4.11 O9.5V+B0.2V(n) 855 0
6 IC 434 HII 05 41 -02.5           ~ 97 1
7 LDN 1630 DNe 05 45.5 -00 59           ~ 392 0
8 * alf Ori s*r 05 55 10.30536 +07 24 25.4304 4.38 2.27 0.42 -1.17 -2.45 M1-M2Ia-Iab 1789 0
9 HD 41161 * 06 05 52.4562749544 +48 14 57.417890532 5.66 6.658 6.764     O8Vn 139 0
10 HD 46223 Y*O 06 32 09.3068103600 +04 49 24.705695568 6.73 7.50 7.28 6.95 6.79 O4V((f)) 406 0
11 * 29 CMa SB* 07 18 40.3789353696 -24 33 31.318248528 3.80 4.80 4.95 4.95 5.08 O7Iafpvar 433 0
12 * tau CMa SB* 07 18 42.4849951654 -24 57 15.700749738 3.26 4.25 4.40 4.44 4.62 O9II 439 0
13 Cl Westerlund 2 OpC 10 23 58.1 -57 45 49           ~ 400 0
14 GUM 29 HII 10 24 14.6 -57 46 58           ~ 219 0
15 Cl Trumpler 14 OpC 10 43 56.0 -59 33 07   5.70 5.5     ~ 547 0
16 RCW 82 HII 13 59.3 -61 27           ~ 33 0
17 HD 135485 SB* 15 15 45.2566709328 -14 41 34.523913444 7.57 8.05 8.13     B3V 126 0
18 HD 138764 Pu* 15 34 26.5142062512 -09 11 00.380211288 4.63 5.08 5.17 5.21 5.33 B5V 167 0
19 HD 147550 * 16 22 38.9052134400 -02 04 47.519268672   6.288 6.241     B9V 124 0
20 SH 2-3 HII 17 12.4 -38 28           ~ 234 1
21 * iot Her bC* 17 39 27.8868980278 +46 00 22.792978043 2.940 3.630 3.800     B3IV 470 1
22 HD 164432 * 18 00 52.8589485000 +06 16 05.857908564 5.5 6.238 6.350     B2IV 95 0
23 NGC 6618 OpC 18 20 47 -16 10.3           ~ 1700 0
24 HRDS G027.334+00.176 HII 18 40 34.5 -04 54 01           ~ 4 0
25 GRS G030.44 +00.44 MoC 18 45.3 -02 01           ~ 2 0
26 LBN 030.54+00.41 HII 18 45.5 -02 00           ~ 11 0
27 [KC2019] Theia 12 As* 18 46 48.414 -01 24 32.44           ~ 3 0
28 HD 174959 * 18 51 36.5174494224 +36 32 20.696423316 5.48 5.983 6.082     B6IV 77 0
29 HD 176301 * 18 58 45.0554475960 +19 47 39.817621824   6.457 6.494     B7III-IV 70 0
30 GB6 B1907+0809 Rad 19 10 12.5 +08 14 42           ~ 1 0
31 * eta Lyr SB* 19 13 45.4884201191 +39 08 45.477640475 3.58 4.243 4.398     B6 166 0
32 Cl Berkeley 45 OpC 19 19 06.3 +15 43 02           ~ 28 0
33 [BDS2003] 139 Cl* 19 22 26 +14 06.9           ~ 8 0
34 [BDS2003] 141 Cl* 19 22 53 +14 09.4           ~ 7 0
35 W 51 SNR 19 23 50 +14 06.0           ~ 1352 1
36 GAL 054.4+01.0 ? 19 28.4 +19 30           ~ 2 0
37 SNR G053.4+00.0 SNR 19 29 58 +18 09.6           ~ 16 0
38 SNR G055.0+00.3 SNR 19 32.0 +19 50           ~ 31 0
39 Kronberger 79 OpC 19 33 55.0 +18 31 12           ~ 15 0
40 V* V1671 Cyg Ro* 19 35 32.0102348112 +31 16 35.933414736 6.44 7.29 7.44     B2V 136 0
41 SNR G056.56-00.75 SR? 19 39 22 +20 31.8           ~ 5 0
42 NGC 6823 OpC 19 43 11.3 +23 18 32   7.71 7.1     ~ 279 2
43 LBN 059.38-00.15 HII 19 43 12 +23 15.0           ~ 25 1
44 Ass Vul OB 1 As* 19 44.0 +24 13           ~ 100 0
45 SH 2-87 bub 19 46 20.69 +24 35 15.4           ~ 161 2
46 V* V380 Cyg SB* 19 50 37.3267754400 +40 35 59.135141652 4.86 5.613 5.680     B1.1III+B2.5/3V: 305 0
47 2MASS J19533020+2808216 NIR 19 53 30.20376 +28 08 21.6709           ~ 1 0
48 2MASS J19533053+2808202 * 19 53 30.539 +28 08 20.30           ~ 2 0
49 NAME Cyg X Cld 20 30 04.7973633 +40 51 36.002197           ~ 962 1
50 NAME Cyg Complex reg 20 32 +45.0           ~ 667 0
51 Ass Cyg OB 2 As* 20 33.2 +41 19           ~ 1023 0
52 * 9 Cep s*b 21 37 55.2241394424 +62 04 54.990376788 4.49 5.03 4.73 4.42 4.24 B2Ib 315 0
53 * 19 Cep * 22 05 08.7897533088 +62 16 47.332569936 4.36 5.19 5.11 4.95 4.92 O9Ib 397 0
54 UBC 1169 OpC 22 21 08.5 +54 55 35           ~ 4 0
55 LBN 104.39+01.32 HII 22 22 11.6 +58 44 18           ~ 39 0
56 HD 240015 * 22 39 17.7273490320 +59 01 00.580609488   10.61 10.04     B0.5II 21 0
57 HD 240016 * 22 39 22.5468294360 +59 00 25.787315088   10.29 9.74     B1.5II 23 0
58 Cl Berkeley 97 OpC 22 39 23.1 +59 00 23           ~ 29 0
59 DSH J2247.4+5946 OpC 22 47 25.9 +59 46 52           ~ 17 0
60 HD 216898 Pu* 22 55 42.4584233736 +62 18 22.821300252 8.10 8.58 8.04     O9V 161 0

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