Table 2
Parameter space covered with UCLCHEM models.
| Parameter | Unit | Values | Notes | |
|---|---|---|---|---|
| Stage 1: Collapse | nH, final(a) | cm−3 | 104, 105, 106, 107, 108 | nH, init = 102 cm−3 |
| Tinit (gas, dust) | K | 15, 20, 25, 30, 35 | ... | |
| ζ/ζ0 | − | 101, 102, 103, 104 | ζ0 = 1.31 × 10−17 s−1 | |
| G0 | Habing | 101, 102, 103, 104 | ... | |
| AV, start | mag | 2 | ... | |
| X(Si)(b) | − | 1.78 × 10−8, 1.78 × 10−6† | †X(Si)⊙ (Jenkins 2009) | |
![]() |
pc | 0.5 | ... | |
| Stage 2: Protostellar Objects | nH(a) | cm−3 | 106, 107, 108 | ... |
| G0 | Habing | 103, 104 | ... | |
| Tfinal (gas,dust) | K | 100, 150, 200, 250, 300, 350, 400, 450, 500 | ... | |
| M | M⊙ | 10, 25 | ... | |
| Stage 2: Shocks | nH, pre–shock(a) | cm−3 | 104, 105, 106 | ... |
| G0 | Habing | 101, 102, 103, 104 | ... | |
| vs | km s−1 | 10, 15, 20, 25, 30, 35, 40 | ... | |
![]() |
μG | 140, 450, 1400 | ![]() |
|
Notes. (a) Proton density, nH, is defined as n(H) + 2n(H2). (b) The models of protostellar objects utilize collapse models with depleted Si abundance with respect to the Solar abundance (e.g., Savage & Sembach 1996), while the shock models rely on those with the standard value of 1.78 × 10−6 (Jenkins 2009). (c) For consistency across models, we adopted a single radius. However, to evaluate the full impact of Rfinal on the chemistry of protostellar objects, we conducted an additional test with Rfinal = 0.05 pc (see Sect. 2.2.3). The results of this test suggest that our protostellar object models are also applicable to smaller objects, with R ≳ 0.05 pc. (d) Values of B0 were not varied, as they depend on pre-shock densities. This work adopts bm0 of 1.4 (Jiménez-Serra et al. 2008). The dagger signify the standard value and it’s origin.
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![$\[R_{\text {final}}^{(c)}\]$](/articles/aa/full_html/2025/11/aa56188-25/aa56188-25-eq3.png)
![$\[B_{0}^{(d)}\]$](/articles/aa/full_html/2025/11/aa56188-25/aa56188-25-eq4.png)
![$\[B_{0}=b m_{0} \sqrt{n_{\mathrm{H}}}\]$](/articles/aa/full_html/2025/11/aa56188-25/aa56188-25-eq5.png)