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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 Cki=βΩki(T)/(gkT)${C_{ki}} = \beta {\Omega _{ki}}\left( T \right)/\left( {{g_k}\,\sqrt T } \right)$ 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 (ki) transitions from level k.

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