2020ApJS..249....6Z


Query : 2020ApJS..249....6Z

2020ApJS..249....6Z - Astrophys. J., Suppl. Ser., 249, 6-6 (2020/July-0)

A systematic observational study on Galactic interstellar ratio 18O/17O. I. C18O and C17O J = 1-0 data analysis.

ZHANG J.S., LIU W., YAN Y.T., YU H.Z., LIU J.T., ZHENG Y.H., ROMANO D., ZHANG Z.-Y., WANG J.Z., CHEN J.L., WANG Y.X., ZHANG W.J., LU H.H., CHEN L.S., ZOU Y.P., YANG H.Q., WEN T. and LU F.S.

Abstract (from CDS):

The interstellar oxygen isotopic ratio of 18O/17O can reflect the relative amount of the secular enrichment by ejecta from high-mass versus intermediate-mass stars. Previous observations found a Galactic gradient of 18O/17O, i.e., low ratios in the Galactic center and large values in the Galactic disk, which supports the inside-out formation scenario of our Galaxy. However, there are not many observed objects and, in particular, there are not many at large galactocentric distances. For this reason, we started a systematic study on Galactic interstellar 18O/17O, through observations of C18O and C17O multi-transition lines toward a large sample of 286 sources (at least one order of magnitude larger than previous ones), from the Galactic center region to the far outer Galaxy (∼22 kpc). In this article, we present our observations of J = 1-0 lines of C18O and C17O, with the 12 m antenna of the Arizona Radio Observatory (ARO 12 m) and the Institut de Radio Astronomie Millimetrique (IRAM) 30 m telescopes. Among our IRAM 30 m sample of 50 targets, we detected successfully both C18O and C17O 1-0 lines for 34 sources. Similarly, our sample of 260 targets for ARO 12 m observations resulted in the detection of both lines for 166 sources. The C18O optical depth effect on our ratio results, evaluated by fitting results of C17O spectra with hyperfine components (assuming τC18O=4τC17O) and our radiative transfer and excitation model nonlocal thermodynamic equilibrium (non-LTE) model calculation for the strongest source, was found to be insignificant. Beam dilution does not seem to be a problem either, which was supported by the fact that there is no systematic variation between the isotopic ratio and the heliocentric distance, and ratios are consistently measured from two telescopes for most of those detected sources. With this study we obtained 18O/17O isotopic ratios for a large sample of molecular clouds with different galactocentric distances. Our results, though there are still very few detections made for sources in the outer Galaxy, confirm the apparent 18O/17O gradient of 18O/17O=(0.10 ± 0.03)RGC+(2.95 ± 0.30), with a Pearson's rank correlation coefficient of R = 0.69. This is supported by the newest Galactic chemical evolution model including the impact of massive stellar rotators and novae. Our future J = 2-1 and J = 3-2 observations of C18O and C17O toward the same sample would be important to determine their physical parameters (opacities, abundances, etc.) and further accurately determine the Galactic radial gradient of the isotopic ratio 18O/17O.

Abstract Copyright: © 2020. The American Astronomical Society. All rights reserved.

Journal keyword(s): Interstellar molecules - Radio sources - Isotopic abundances - Galaxy chemical evolution - Milky Way evolution

VizieR on-line data: <Available at CDS (J/ApJS/249/6): sources.dat table1.dat table2.dat>

Status at CDS : All or part of tables of objects could be ingested in SIMBAD with priority 2.

Simbad objects: 31

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Number of rows : 31
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 GM 1-33 HH 00 36 47.5 +63 29 02           ~ 124 0
2 RAFGL 5085 Y*O 02 50 08.5608261912 +61 59 51.902005956           ~ 44 0
3 NAME AFGL 4029 IRS 1 Y*O 03 01 29.2 +60 29 12           ~ 112 1
4 2MASX J03172875+6032259 G 03 17 28.7557604880 +60 32 25.515551616           ~ 9 0
5 NAME Per Arm PoG 03 30 +45.0           ~ 1672 0
6 2MASX J04041342+5122587 G 04 04 13.4464505640 +51 22 58.539784476           ~ 11 0
7 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 16269 0
8 NAME Sgr B2 MoC 17 47 20.4 -28 23 07           ~ 2443 1
9 NAME 1.5 Complex MoC 17 48 22 -27 48.3           ~ 16 0
10 IRAS 20567+4821 IR 20 58 23.0 +48 32 48           ~ 6 0
11 IRAS 21003+4750 IR 21 02 01.9 +48 02 08           ~ 5 0
12 IRAS 21260+4938 IR 21 27 45.3 +49 51 51           ~ 6 0
13 IRAS 21445+5712 Or* 21 46 07.1269843296 +57 26 31.628449824           ~ 55 0
14 LBN 102.79-00.92 HII 22 19 09.0 +56 04 45           ~ 109 0
15 IRAS 22172+5549 Y*O 22 19 09.14787 +56 05 00.0380           ~ 105 0
16 IRAS 22176+6303 Y*O 22 19 18.23 +63 18 47.5           ~ 600 0
17 IRAS 22246+5750 IR 22 26 29.2712501808 +58 05 39.946383492           ~ 8 0
18 IRAS 22267+6244 HII 22 28 29.3 +62 59 44           ~ 30 0
19 LDN 1206 DNe 22 28 52.2 +64 13 43           ~ 70 0
20 SH 2-138 HII 22 32 45.7 +58 28 20           ~ 115 2
21 GLMP 1062 HII 22 35 00.7 +58 24 41           ~ 18 0
22 IRAS 22334+6525 MIR 22 35 08.70768 +65 41 33.4572           ~ 6 0
23 IRAS 22451+6154 * 22 47 02.1 +62 10 11           B 22 0
24 IRAS 23068+6117 HII 23 08 55.66 +61 34 06.2           ~ 16 0
25 IRAS 23071+6033 mul 23 09 14.1 +60 49 17           ~ 12 0
26 IRAS 23088+6014 LP* 23 11 07.0286952072 +60 31 43.602216204           ~ 16 1
27 JCMTSF J231256.2+594437 * 23 12 56.6 +59 44 30           B 12 0
28 SH 2-159 Y*O 23 15 31.2384366062 +61 07 10.181362705           ~ 188 1
29 IRAS 23134+6131 MIR 23 15 33.73440 +61 47 50.8632           ~ 16 0
30 CPM 39 Y*O 23 17 09.9467708640 +61 31 09.246087444           ~ 10 0
31 IRAS 23545+6508 * 23 57 05.2 +65 25 11           B 52 0

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