Table 3
Properties of the radio continuum emission using uGMRT and GLOSTAR data.
| Sν (1.35 GHz) | Source name | Sν (5.79 GHz) | Sν (5.85 GHz) | log(NLy) | log(NLy) | ZAMS | τe | DUC | αUC | αp | α |
|---|---|---|---|---|---|---|---|---|---|---|---|
| (Jy) | (Jy) | (Jy) | (1.35 GHz) | (5.85 GHz) | (K) | (pc) | |||||
| (*)G19.68−0.13 | 0.622 ± 0.012 | 0.481 ±0.018 | 0.57 ± 0.07 | 48.82 | 48.85 | O6.5 | 9627 | — | — | −0.070 | −0.098 |
| (*)G20.99+0.09 | 1.344 ±0.014 | 0.630 ± 0.017 | 1.17 ± 0.10 | 47.54 | 47.55 | B0 | 9162 | — | — | −0.132 | −0.156 |
| G22.76−0.48 | 1.788 ± 0.025 | 0.672 ± 0.013 | 1.81 ± 0.11 | 48.56 | 48.63 | O7 | 8216 | 0.08 | 1.97 ±2.19 | −0.136 | −0.144 |
| G24.47+0.49 | 3.178 ±0.006 | 3.502 ± 0.012 | 3.76 ± 0.15 | 48.98 | 49.12 | O6 | 7956 | 0.11 | 1.96 ± 1.98 | −0.121 | −0.129 |
| G25.69+0.03 | 0.883 ± 0.016 | 0.533 ± 0.019 | 0.83 ± 0.06 | 49.02 | 49.06 | O6 | 7680 | 0.04 | 1.66 ±0.38 | −0.126 | −0.137 |
| (*)G27.49+0.19 | 1.701 ± 0.014 | 0.785 ±0.011 | 1.47 ± 0.08 | 47.87 | 47.87 | O9.5 | 7213 | — | — | −0.139 | −0.151 |
| G28.30−0.39 | 0.820 ± 0.015 | 0.654 ± 0.010 | 0.71 ± 0.07 | 48.80 | 48.80 | O6.5 | 8829 | 0.11 | 1.21 ± 5.60 | −0.113 | −0.132 |
| (*)G28.81+0.17 | 1.462 ± 0.012 | 0.971 ± 0.014 | 1.30 ± 0.09 | 48.89 | 48.90 | O6.5 | 8276 | — | — | −0.125 | −0.147 |
Notes. (*)sources comprise of multiple fragments of compact emission, Duc = size of the UCHR (excluding the extended emission) using the GLOSTAR-B data, αUC = spectral index of the UCHR (excluding the extended emission) using the GLOSTAR-B data, αp = spectral index using the in-band GLOSTAR-D flux densities within a grid of 3 × 3 pixels centered at the pixel with the peak emission, α = spectral index estimated using the uGMRT and GLOSTAR-D integrated flux densities.
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