2024MNRAS.528.4364E


Query : 2024MNRAS.528.4364E

2024MNRAS.528.4364E - Mon. Not. R. Astron. Soc., 528, 4364-4378 (2024/March-1)

Can radial temperature profiles be inferred using NH3 (1, 1) and (2, 2) observations?

ESTALELLA R., PALAU A. and BUSQUET G.

Abstract (from CDS):

A number of works infer radial temperature profiles of envelopes surrounding young stellar objects using several rotational transitions in a pixel-by-pixel or azimuthally averaged basis. However, in many cases the assumption that the rotational temperature is constant along the line of sight is made, while this is not the case when a partially resolved envelope, assumed to be spherically symmetric, is used to obtain values of temperature for different projected radii. This kind of analysis (homogeneous analysis) is intrinsically inconsistent. By using a spherical envelope model to interpret NH3 (1,1) and (2,2) observations, we tested how robust it is to infer radial temperature profiles of an envelope. The temperature and density of the model envelope are power laws of radius, but the density can be flat for an inner central part. The homogeneous analysis was applied to obtain radial temperature profiles, and resulted that for small projected radii, where the optical depth of the lines is high, the homogeneous temperature can be much higher than the actual envelope temperature. In general, for larger projected radii, both the temperature and the temperature power-law index can be underestimated by as much as 40 per cent, and 0.15, respectively. We applied this study to the infrared dark cloud G14.225-0.506 for which the radial temperature profile was previously derived from the dust emission at submillimetre wavelengths and the spectral energy distribution. As expected, the homogeneous analysis underestimated both the temperature and the temperature power-law index.

Abstract Copyright: © The Author(s) 2024. Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): radiative transfer - techniques: spectroscopic - ISM: clouds - ISM: molecules

Simbad objects: 20

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Number of rows : 20
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 [BEP2016] Hub-N MM1b mm 18 18 12.30 -16 49 28.7           ~ 3 0
2 [BEP2016] Hub-N MM1c mm 18 18 12.32 -16 49 31.9           ~ 3 0
3 [BEP2016] Hub-N MM1a mm 18 18 12.32 -16 49 28.1           ~ 5 0
4 [BEP2016] Hub-N MM1d mm 18 18 12.33 -16 49 30.5           ~ 3 0
5 [BEP2016] Hub-N MM1e mm 18 18 12.37 -16 49 26.9           ~ 3 0
6 [BEP2016] Hub-S MM2 mm 18 18 12.43 -16 57 22.6           ~ 2 0
7 [BEP2016] Hub-S MM4 mm 18 18 12.84 -16 57 20.3           ~ 3 0
8 [BEP2016] Hub-S MM5c mm 18 18 12.90 -16 57 24.0           ~ 3 0
9 [BEP2016] Hub-N MM3 mm 18 18 13.05 -16 49 41.3           ~ 2 0
10 [PW2010] 165 Y*? 18 18 13.171 -16 57 23.30           ~ 4 0
11 [BEP2016] Hub-S MM5a mm 18 18 13.34 -16 57 24.1           ~ 4 0
12 [BEP2016] Hub-S MM6b mm 18 18 13.38 -16 57 14.4           ~ 2 0
13 [BEP2016] Hub-S MM6a mm 18 18 13.40 -16 57 12.2           ~ 2 0
14 [BEP2016] Hub-S MM7a mm 18 18 13.92 -16 57 11.7           ~ 3 0
15 [BEP2016] Hub-S MM7b mm 18 18 13.95 -16 57 15.0           ~ 2 0
16 [BEP2016] Hub-S MM7c mm 18 18 13.97 -16 57 18.0           ~ 2 0
17 [BEP2016] Hub-S MM8 mm 18 18 14.86 -16 57 14.9           ~ 2 0
18 [BEP2016] Hub-S MM9 mm 18 18 15.93 -16 57 19.2           ~ 2 0
19 NAME M17 SWex MoC 18 19.0 -16 40           ~ 62 0
20 MSXDC G034.43+00.24 MoC 18 53 18.9 +01 26 39           ~ 122 0

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