Table 2
Estimation of ne based on size and brightness of bow shock (or RMS noise level of the map for non-detections) using Eq. (2).
| Source | d (kpc) | Method | R0 (pc) | RMS (mJy beam−1) | Iν (mJy beam−1) | UL? | ne (cm−3) |
|---|---|---|---|---|---|---|---|
| G119.4436-00.9208 | 2.27 | GSP-Phot | 0.19 | 0.02 | <0.06 | Yes | <51.9 |
| EB01: HIP 2036 | 1.18 | GSP-Phot | 0.29 | 0.01 | <0.03 | Yes | <28.9 |
| EB29: SER6 | 2.35 | para | 0.34 | 0.2 | <0.60 | Yes | <124 |
| G133.1567+00.0432 | 2.10 | para | 0.37 | 0.009 | <0.027 | Yes | <19.5 |
| G134.3552+00.8182 | 1.98 | para | 0.13 | 0.05 | <0.15 | Yes | <75.6 |
| G137.4203+01.2792 | 1.09 | GSP-Phot | 0.39 | 0.01 | <0.03 | Yes | <28.4 |
| G151.0318-00.8271 | 1.77 | GSP-Phot | 0.44 | 0.02 | <0.06 | Yes | <38.7 |
| EB09: HIP 26397 | 1.19 | GSP-Phot | 0.35 | 0.004 | <0.012 | Yes | <12.9 |
| EB12: HIP 31766 | 1.08 | GSP-Phot | 0.63 | 0.015 | <0.045 | Yes | <15.4 |
| EB31: HD 57682 | 0.71 | GSP-Phot | 0.06 | 0.01 | <0.030 | Yes | <41.3 |
| ζ Oph | 0.135 | (2) | 0.13 | 0.018 | <0.054 | Yes | <39.7 |
| EB23: HIP 88652 | 1.46 | para | 0.67 | 0.04 | 0.4 | No | <43.5 |
| G018.2660-00.2988 | 4.14 | para | 0.30 | 0.5 | 15 | No | <411 |
| G026.5272+00.3808 | n/a | n/a | n/a | 0.5 | <1.5 | Yes | n/a |
| G026.1437-00.0420 | n/a | n/a | n/a | 0.12 | 1.5 | No | n/a |
| G031.6770+00.1775 | n/a | n/a | n/a | 0.04 | 0.2 | No | n/a |
| G039.2486-00.0647 | n/a | n/a | n/a | 1.5 | 40 | No | n/a |
| G049.7065-00.1722 | n/a | n/a | n/a | 0.19 | 2.0 | No | n/a |
| G075.1730-00.5964 | 2.85 | GSP-Phot | 0.13 | 0.01 | 0.05 | No | <62.3 |
| G078.2889+00.7829 | 1.79 | GSP-Phot | 0.22 | 0.08 | <0.24 | Yes | <60.9 |
| BD+43° 3654 | 1.72 | (1) | 1.61 | 0.07 | 1.4 | No | <69.5 |
| G107.1371-00.6974 | 2.64 | para | 0.54 | 0.014 | 0.07 | No | <26.7 |
| G108.0269-00.3497 | 3.03 | para | 0.52 | 0.013 | 0.13 | No | <37.0 |
| BD+60° 2522 | 3.0 | (1) | 0.60 | 0.2 | 5.0 | No | <252 |
Notes. (1) Paper I; (2) Green et al. (2022). The column ‘method’ refers to how the distance was estimated: numbers refer to cited references, ‘GSP-Phot’ refers to Gaia DR3 GSP-Phot distance estimate where available, ‘para’ refers to inverted parallax when the ‘GSP-Phot’ distance is not available and the relative uncertainty on the parallax is <1/8, and ‘n/a’ is quoted where the distance is unknown and no estimate for R0 or ne was attempted. The angular estimate for R0 is taken from Kobulnicky et al. (2016) and Peri et al. (2015), depending on which catalogue the bow-shock candidate is located in, and converted to a linear size using the distance estimate. The intensity around the apex of the bow shock, Iν, is measured from the observations, or a 3σ upper limit is taken for non-detections using the RMS level of the map (column 5). The estimated electron density, ne, is calculated from Eq. (2) and is always an upper limit because part of the emission could be synchrotron and not bremsstrahlung.
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