2021RAA....21..207H


Query : 2021RAA....21..207H

2021RAA....21..207H - Research in Astron. and astroph., 21, 207 (2021/August-0)

Evolutions of CH3CN abundance in molecular clumps.

HE Z.-Z., LI G.-X. and ZHANG C.

Abstract (from CDS):

To investigate the effects of massive star evolution on surrounding molecules, we select nine massive clumps previously observed with the Atacama Pathfinder Experiment (APEX) telescope and the Submillimeter Array (SMA) telescope. Based on the observations of APEX, we obtain luminosity to mass ratios Lclump/Mclump that range from 10 to 154 L☉/M☉, where some of them embedded ultra compact (UC) HII region. Using the SMA, CH3CN (12K-11K) transitions were observed toward nine massive star-forming regions. We derive the CH3CN rotational temperature and column density using the XCLASS program, and calculate its fractional abundance. We find that CH3CN temperature seems to increase with the increase of Lclump/Mclump when the ratio is between 10 to 40 L☉/M☉, then decrease when Lclump/Mclump >= 40 L☉/M☉. Assuming that the CH3CN gas is heated by radiation from the central star, the effective distance of CH3CN relative to the central star is estimated. The distance ranges from ∼ 0.003 to ∼ 0.083 pc, which accounts for ∼ 1/100 to ∼ 1/1000 of clump size. The effective distance increases slightly as Lclump/Mclump increases (Reff ∼ (Lclump/Mclump)0.5±0.2). Overall, the CH3CN abundance is found to decrease as the clumps evolve, e.g., XCH3CN ∼ (Lclump/Mclump)-1.0 ± 0.7. The steady decline of CH3CN abundance as the clumps evolution can be interpreted as a result of photodissociation.

Abstract Copyright: © 2021 National Astronomical Observatories

Journal keyword(s): line: identification - stars: evolution - stars: formation - ISM: molecules - submillimeter: ISM

Simbad objects: 21

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Number of rows : 21
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 MPCM J022530.99+620620.9 HII 02 25 31.18 +62 06 24.5           O8V-B0.5V 107 1
2 3C 273 BLL 12 29 06.6998257176 +02 03 08.597629980   13.05 14.830 14.11   ~ 6022 1
3 3C 279 Bla 12 56 11.16657958 -05 47 21.5251510   18.01 17.75 15.87   ~ 3205 2
4 PMN J1604-4227 cm 16 04 47.59969 -42 28 09.4607           ~ 10 1
5 IRAS 16547-4247 Y*O 16 58 17.208 -42 52 08.16           ~ 187 0
6 QSO B1730-130 Bla 17 33 02.70578907 -13 04 49.5482119   18 19.50 18.78 17.39 ~ 1198 1
7 PSR J1745-2900 Psr 17 45 40.1640 -29 00 29.818           ~ 358 0
8 4C 09.57 BLL 17 51 32.81857326 +09 39 00.7284066   17.46 16.78 15.57   ~ 1007 1
9 RAFGL 2046 HII 18 00 32.1 -24 04 03           ~ 380 0
10 RAFGL 5436 HII 18 06 19.027 -21 37 32.32           ~ 108 0
11 W 31c HII 18 10 29.1 -19 56 05           ~ 357 0
12 EGO G016.59-0.05 HII 18 21 07.9 -14 31 53           ~ 129 0
13 ICRF J183005.9+061915 Bla 18 30 05.93984953 +06 19 15.9522412       19.5   ~ 124 1
14 AGAL G028.199-00.049 cor 18 42 58 -04 14.0           ~ 46 0
15 IRAS 18566+0408 Y*O 18 59 09.95520 +04 12 15.6240           ~ 143 0
16 QSO B1908-202 Bla 19 11 09.65289294 -20 06 55.1090664   18.21   18.14   ~ 306 1
17 IRAS 19110+1045 Y*O 19 13 22.0427 +10 50 53.336           ~ 132 0
18 [UHP2009] VLA G045.4657+00.0453 HII 19 14 25.7 +11 09 26           ~ 31 1
19 QSO B1921-293 BLL 19 24 51.05595254 -29 14 30.1210248   18.71 18.21 15.07   ~ 918 1
20 ICRF J192559.6+210626 BLL 19 25 59.60535459 +21 06 26.1620257           ~ 212 1
21 3C 454.0 QSO 22 51 34.7277468096 +18 48 40.087264428   18.52 18.4     ~ 232 2

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