Table 4
Results for the radiative transfer calculations for dust in NGC 7023 NW and in NGC 7023 E.
![]() |
n0 |
![]() |
![]() |
lPDR |
![]() |
[ cm-3 ] | [ cm-3 ] | [cm-2] | [pc] | ||
|
|||||
NGC 7023 NW | |||||
|
|||||
104 | 104 | ~0.2 | 2 × 1022 | 0.6 | – |
6 × 104 | 105 | ~ 1 | 4 × 1022 | 0.2 | 1.6 × 10-4 |
1.2 × 105 | 2 × 105 | ~ 2 | 7 × 1022 | 0.2 | 7 × 10-5 |
4 × 105 | 106 | ~ 4 | 4 × 1022 | 0.03 | 1 × 10-4 |
|
|||||
NGC 7023 E | |||||
|
|||||
5 × 103 | 104 | ~ 0.2 | 9 × 1021 | 0.6 | – |
5 × 104 | 105 | ~ 2 | 6 × 1022 | 0.4 | 3 × 10-5 |
5 × 104 | 2 × 105 | ~ 2 | 2 × 1022 | 0.15 | 1 × 10-4 |
5 × 105 | 106 | ~18 | 2 × 1023 | 0.12 | 5 × 10-6 |
Notes. is the
density at the CO emission peak, n0 is the maximum density,
is the
visual extinction perpendicular to the line of sight integrated from the edge to the
emission peak,
is the
column density along the line of sight at the emission peak, lPDR is
the length along the line of sight, and
is the 12CO
to H2
abundance ratio at the emission peak. We derive NCO from
the RADEX analysis (see Table 2) and
NH2 from
. The results for the
best fit are shown in blue. The table entries in bold face indicate results for
physically reasonable lengths along the lines of sight.
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