1995A&A...295..194D


Query : 1995A&A...295..194D

1995A&A...295..194D - Astronomy and Astrophysics, volume 295194-198 (1995/3-1)

The nitrogen isotope abundance in the Galaxy. I. The Galactic disk gradient.

DAHMEN G., WILSON T.L. and MATTEUCCI F.

Abstract (from CDS):

We present high quality data of HCN double isotopomer ratios observed in the J=1-0 line of 11 warm, dense molecular clouds in the galactic disk. After fitting 12C/13C ratios from published data as a function of galactocentric distance, we obtained the 14N/15N ratios. From these results and previously published data, we have determined the galactic disk gradient of the nitrogen isotope ratio using a linear regression. We have obtained a gradient of 19.7±8.9kpc–1. We have compared our result with the theoretical model of Matteucci & D'Antona (1991A&A...247L..37M) and conclude that 15N is a purely secondary element; 14N must also be secondary, but with a significant primary contribution. We briefly discuss the production of nitrogen isotopes involving massive stars; however, it may be difficult to fit the 12C/13C gradient into this scenario.

Abstract Copyright: ∼

Journal keyword(s): ISM: abundances, molecules - Galaxy: abundances, evolution - radio lines: ISM

Simbad objects: 11

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Number of rows : 11
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 IRAS 08303-4303 HII 08 32 07.5 -43 13 46           ~ 26 0
2 IRAS 15520-5234 HII 15 55 48.336 -52 43 10.20           ~ 59 1
3 IRAS 15567-5236 HII 16 00 32.9 -52 44 45           ~ 35 0
4 IRAS 16065-5158 HII 16 10 21.8 -52 06 04           ~ 39 0
5 IRAS 16172-5028 HII 16 21 00.4 -50 35 21           ~ 50 0
6 IRAS 16562-3959 SFR 16 59 42.257 -40 03 45.17           ~ 77 0
7 IRAS 17009-4042 HII 17 04 29.5 -40 46 27           ~ 33 0
8 IRAS 17059-4132 HII 17 09 31.3 -41 35 56           ~ 30 0
9 GAL 350.10+00.09 HII 17 19 26.1 -37 10 54           ~ 43 0
10 GAL 351.58-00.35 HII 17 25 25.2 -36 12 46           ~ 40 0
11 IRAS 17233-3606 HII 17 26 42.8 -36 09 17           ~ 98 0

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