Table 2:
Conversion factors of the line
intensity in erg s-1 cm-2 into the velocity integrated
main beam temperature
observed at the IRAM and JCMT telescopes respectively,
for the five lines observed towards IRAS 16293-2422 (Parise et al. 2005).
Last column quotes the
observed towards IRAS 16293-2422 (Parise et al. 2005).a Predicted flux
from the model simply converted into K km s-1 using the conversion factor.
b Predicted flux derived using an accurate convolution of the signal with the
telescope beam.
|
Transition |
Frequency |
Telescope |
Conversion coeff |
IRAS 16293-2422 |
| |
(GHz) |
|
1 K km s-1 (
) |
(K km s-1) |
(K km s-1) |
(K km s-1) |
| |
|
|
(erg s-1 cm-2) |
Conversiona |
Convolutionb |
Obsc |
|
11,0-11,1 |
80.578 |
IRAM |
1.4 10-17 |
0.19 |
0.21 |
0.40 |
|
31,2-22,1 |
225.897 |
IRAM |
4.1 10-17 |
1.7 |
1.8 |
1.7 |
|
21,1-21,2 |
241.561 |
IRAM |
4.4 10-17 |
1.5 |
1.5 |
2.0 |
|
22,0-31,3 |
266.161 |
IRAM |
4.9 10-17 |
0.20 |
0.22 |
0.21 |
|
10,1-00,0 |
464.924 |
JCMT |
4.0 10-16 |
6.3 |
5.4 |
5.5 |
Source LaTeX |
All tables |
In the text