Table 3
Modelling results.
Star | SiS | CS | ||||||||
---|---|---|---|---|---|---|---|---|---|---|
f0 | Re | n | ![]() |
NSiS | f0 | Re | n | ![]() |
NCS | |
(×10−6) | (× 1015 cm) | (cm−2) | (×10−6) | (× 1015 cm) | (cm−2) | |||||
Carbon stars | ||||||||||
R Lep | ... | ... | 0 | ... | ... | ![]() |
![]() |
2 | 0.00 | 1.2 × 1017 |
V1259 Ori | ![]() |
13 ± 3 | 5 | 3.4 | 1.1 × 1018 | ![]() |
![]() |
3 | 0.59 | 1.7 × 1018 |
AI Vol | ![]() |
![]() |
7 | 3.2 | 1.2 × 1018 | ![]() |
![]() |
2 | 0.03 | 8.9 × 1017 |
X TrA | ... | ... | 0 | ... | ... | 11 ± 7 | ![]() |
2 | 0.01 | 3.2 × 1017 |
V821 Her | 9.4 ± 2.6 | 5.7 ± 1.0 | 5 | 2.9 | 2.8 × 1017 | ![]() |
![]() |
3 | 0.54 | 9.9 × 1016 |
U Hya | ... | ... | 0 | ... | ... | ![]() |
![]() |
3 | 7.1 | 1.1 × 1015 |
RV Aqr | 11 ± 6 | ![]() |
3 | 0.71 | 2.5 × 1017 | ![]() |
![]() |
2 | 0.00 | 1.7 × 1017 |
Oxygen-rich stars | ||||||||||
IK Tau | 1.7 ± 0.4 | 5.3 ± 1.0 | 7 | 1.1 | 1.1 × 1017 | 0.11 ± 0.04 | ![]() |
2 | 0.02 | 6.1 × 1015 |
GX Mon | 0.53 ± 0.12 | 13 ± 4 | 5 | 2.0 | 3.5 × 1016 | ![]() |
≳ 200b | 2 | 0.36 | 5.6 × 1015 |
V1300 Aql | 1.1 ± 0.3 | 12 ± 3 | 5 | 1.4 | 7.6 × 1016 | 0.029 ± 0.023 | ![]() |
2 | 0.00 | 2.5 × 1015 |
S-type stars | ||||||||||
R And | ... | ... | 0 | ... | ... | 0.15 ± 0.5 | ![]() |
2 | 0.01 | 1.4 × 1015 |
S Cas | ![]() |
3.6b | 2 | 1.1 | 2.4 × 1016 | ![]() |
![]() |
2 | 0.0 | 1.7 × 1016 |
IRC-10401 | 0.60 ± 0.12 | 3.0b | 1 | ... | 3.7 × 1015 | ... | ... | 0 | ... | ... |
S Lyr | ... | ... | 0 | ... | ... | ![]() |
19b | 1 | ... | 3.4 × 1017 |
W Aqlc | 1.5 ± 0.05 | 6.0 | ... | ... | 5.9 × 1016 | 1.2 ± 0.05 | 7.0 | ... | ... | 4.7 × 1016 |
EP Vul | ... | ... | 0 | ... | ... | 0.18 ± 0.04 | 8.6b | 1 | ... | 1.1 × 1015 |
χ Cyg | 0.18 ± 0.06 | 2.5b | 2 | 1.4 | 1.5 × 1015 | 0.10 ± 0.03 | ![]() |
2 | 0.01 | 5.7 × 1014 |
RZ Sgr | 0.28 ± 0.06 | 7.2b | 1 | ... | 1.0 × 1016 | ... | ... | 0 | ... | ... |
Notes. f0 is the peak abundance relative to H2 and Re is the e-folding radius. n is the number of observed lines included in our radiative transfer analysis. N is the column density obtained from our radiative transfer modelling. (a)indicates models for which upper limits cannot be placed on the uncertainties due to optical depth effects that come into play at higher abundances of CS. (b)indicates models which cannot be radially constrained with the available data. Where only one observed line is available, Re is calculated from whichever is applicable out of Eqs. (3) and (4). (c) W Aql is originally modelled in Brunner et al. (2018), based in part on ALMA observations, and is only included here for completion. Hence, uncertainties, N and are omitted for this source since the fit to a radial profile derived from an ALMA image is not comparable to fits based only on single-dish data.
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