Table 1.
Parameters measured and inferred in this work.
Source-related parameters | ||
Distancem | 9.4 ± 0.7 kpc | |
Jet inclination anglemi | 60 ± 5 deg | |
Jet opening anglemθ | 1–10 deg | |
Thermal Bremsstrahlung region (IRAS 19132+1035) – the IRAS region | ||
Diameterm | 36 arcsec | 1.6 pc |
Volumei | 6.6 × 1055 cm3 | |
Integrated flux densitym | 60 ± 6 mJy | |
Electron temperaturea | 104–3 × 106 K | |
Shock-compressed gas electron densityi | 395–630 particles/cm3 | |
ISM gas densityi | 100–160 particles/cm3 | |
Shock front velocity | 21–363 Km s−1 | |
Region gas pressurei (ideal gas) | 2.5 × 10−10–7.7 × 10−8 [erg/cm3] | |
Non-thermal emission region (cylindrical hot spot) – the northern feature | ||
Flux densitym | 5.2 ± 0.5 mJy | |
Luminosity | 2 × 10+29 erg s−1 | |
Radiusm | 3.9 arcsec | 0.18 pc |
Lengthm | 17.4 arcsec | 0.9 pc |
Volumei | 2.6 × 1054 cm3 | |
Cylinder pressurei (minimum energy) | > 1.5 × 10−11 erg/cm3 | |
Cylinder magnetic density ![]() |
> 2.18 × 10−5 Gauss | |
The lobe and the bow shock structure | ||
Bow shock structure flux densitym | 0.15 ± 0.01 mJy | |
Bow shock distance from binarym (cavity major axis) | 17 arcmin | 46 pc |
Lobe minor axism | 10 arcmin | 27 pc |
Bow shock structure thicknessm | 60 arcsec | 2.7 pc |
Lobe volumei | 6 × 1059 cm3 | |
Lobe pressurei (equi-partition) | > 1.3 × 10−12 erg/cm3 | |
Lobe magnetic fieldi (synchrotron emission) | > 6.4 × 10−6 Gauss | |
Jet energetics | ||
Jet agei | 0.09–0.22 Myr | |
Jet pressurei (self-similar model) | 2.8 × 10−11 – 7.8 × 10−10 [erg/cm3] | |
One-sided power transferred (self-similar)i | 3.3 × 1037–1.5 × 1039 erg s−1 | |
One-sided power transferred (Enthalpy)i | > 1.2 × 1037 erg s−1 | |
One-sided power transferred (Hot spot)i | > 1.7 × 1036 erg s−1 | |
Pseudo-constant C1i | 3.3–9 |
Notes. The table including the parameters measured (denoted with m) or inferred (denoted with i) in this work. Parameters have been divided based on the region they refer to. Where lengths are given in angular units and physical units, we intend the former as apparent, and the latter as corrected for projection effects, when appropriate.
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