Table A.1
Spectroscopic properties of [Fe II] lines observed in TMC1A.
| λ (µm) | Termk | Jk | ɡk | Energyk k (K) | Termi | Ji | ɡi | Energyi/k (K) | Tex (K) | Aki (s−1) | ncrit (cm−3) |
|---|---|---|---|---|---|---|---|---|---|---|---|
| 25.988 | a6D | 7/2 | 8 | 554 | a6D | 9/2 | 10 | 0 | 554 | 2.05e-03 | 2.77e+04 |
| 5.340 | a4F | 9/2 | 10 | 2694 | a6D | 9/2 | 10 | 0 | 2694 | 5.35e-05 | 1.33e+03 |
| 17.936 | a4F | 7/2 | 8 | 3496 | a4F | 9/2 | 10 | 2694 | 802 | 6.01e-03 | 3.46e+04 |
| 24.519 | a4F | 5/2 | 6 | 4083 | a4F | 7/2 | 8 | 3496 | 587 | 4.17e-03 | 2.22e+04 |
| 1.257 | a4D | 7/2 | 8 | 11446 | a6D | 9/2 | 10 | 0 | 11446 | 5.18e-03 | 6.05e+04 |
| 1.321 | a4D | 7/2 | 8 | 11446 | a6D | 7/2 | 8 | 554 | 10892 | 1.44e-03 | 6.05e+04 |
| 1.372 | a4D | 7/2 | 8 | 11446 | a6D | 5/2 | 6 | 961 | 10485 | 8.93e-04 | 6.05e+04 |
| 1.644 | a4D | 7/2 | 8 | 11446 | a4F | 9/2 | 10 | 2694 | 8752 | 5.73e-03 | 6.05e+04 |
| 1.810 | a4D | 7/2 | 8 | 11446 | a4F | 7/2 | 8 | 3496 | 7950 | 1.25e-03 | 6.05e+04 |
| 1.249 | a4D | 5/2 | 6 | 12074 | a6D | 7/2 | 8 | 554 | 11520 | 4.62e-04 | 5.11e+04 |
| 1.295 | a4D | 5/2 | 6 | 12074 | a6D | 5/2 | 6 | 961 | 11113 | 2.23e-03 | 5.11e+04 |
| 1.328 | a4D | 5/2 | 6 | 12074 | a6D | 3/2 | 4 | 1241 | 10833 | 1.30e-03 | 5.11e+04 |
| 1.534 | a4D | 5/2 | 6 | 12074 | a4F | 9/2 | 10 | 2694 | 9380 | 3.00e-03 | 5.11e+04 |
| 1.677 | a4D | 5/2 | 6 | 12074 | a4F | 7/2 | 8 | 3496 | 8578 | 2.38e-03 | 5.11e+04 |
| 1.801 | a4D | 5/2 | 6 | 12074 | a4F | 5/2 | 6 | 4083 | 7991 | 1.72e-03 | 5.11e+04 |
| 1.279 | a4D | 3/2 | 4 | 12489 | a6D | 3/2 | 4 | 1241 | 11248 | 2.80e-03 | 7.32e+04 |
| 1.298 | a4D | 3/2 | 4 | 12489 | a6D | 1/2 | 2 | 1406 | 11083 | 1.23e-03 | 7.32e+04 |
| 1.600 | a4D | 3/2 | 4 | 12489 | a4F | 7/2 | 8 | 3496 | 8993 | 4.03e-03 | 7.32e+04 |
| 1.712 | a4D | 3/2 | 4 | 12489 | a4F | 5/2 | 6 | 4083 | 8406 | 1.13e-03 | 7.32e+04 |
| 1.798 | a4D | 3/2 | 4 | 12489 | a4F | 3/2 | 4 | 4485 | 8004 | 2.00e-03 | 7.32e+04 |
| 1.271 | a4D | 1/2 | 2 | 12729 | a6D | 1/2 | 2 | 1406 | 11323 | 3.82e-03 | 4.34e+04 |
| 1.664 | a4D | 1/2 | 2 | 12729 | a4F | 5/2 | 6 | 4083 | 8645 | 4.56e-03 | 4.34e+04 |
Notes: Critical densities (ncrit) for the Cloudy excitation model are calculated using Einstein A-coefficients and collisional strengths from Verner et al. (1999), evaluated at T = 7000 K for consistency with previous shock studies (e.g., Koo et al. 2016). The critical density is defined as ncrίt = Σ Aki/ Σ Cki, where Aki is the spontaneous emission rate and
is the collisional de-excitation rate. Here, Ωki(T) is the collision strength, ɡk the statistical weight of the upper level, and β = 8.63 × 10−6 a constant. The sums run over all radiative (k > i) and collisional (k ≠ i) transitions from level k.
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