2024A&A...685A.149J


Query : 2024A&A...685A.149J

2024A&A...685A.149J - Astronomy and Astrophysics, volume 685A149 (2024/5-1)

Fractionation in young cores: Direct determinations of nitrogen and carbon fractionation in HCN.

JENSEN S.S., SPEZZANO S., CASELLI P., SIPILA O., REDAELLI E., GIERS K. and FERRER ASENSIO J.

Abstract (from CDS):

Context. Nitrogen fractionation is a powerful tracer of the chemical evolution during star and planet formation. It requires robust determinations of the nitrogen fractionation across different evolutionary stages.
Aims. We aim to determine the 14N/15N and 12C/13C ratios for HCN in six starless and prestellar cores and to compare the results between the direct method using radiative transfer modeling and the indirect double isotope method, assuming a fixed 12C/13C ratio.
Methods. We present IRAM observations of the HCN 1-0, HCN 3-2, HC15N 1-0 and H13CN 1-0 transitions toward six embedded cores. The 14N/15N ratio was derived using both the indirect double isotope method and directly through non-local thermodynamic equilibrium (NLTE) 1D radiative transfer modeling of the HCN emission. The latter also provides the 12C/13C ratio, which we compared to the local interstellar value.
Results. The derived 14N/15N ratios using the indirect method are generally in the range of 300-550. This result could suggest an evolutionary trend in the nitrogen fractionation of HCN between starless cores and later stages of the star formation process. However, the direct method reveals lower fractionation ratios of around ∼250, mainly resulting from a lower 12C/13C ratio in the range ∼20-40, as compared to the local interstellar medium value of 68.
Conclusions. This study reveals a significant difference between the nitrogen fractionation ratio in HCN derived using direct and indirect methods. This can influence the interpretation of the chemical evolution and reveal the pitfalls of the indirect double isotope method for fractionation studies. However, the direct method is challenging, as it requires well-constrained source models to produce accurate results. No trend in the nitrogen fractionation of HCN between earlier and later stages of the star formation process is evident when the results of the direct method are considered.

Abstract Copyright: © The Authors 2024

Journal keyword(s): astrochemistry - stars: formation - ISM: abundances - ISM: lines and bands

VizieR on-line data: <Available at CDS (J/A+A/685/A149): table1.dat sp/*>

Simbad objects: 22

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Number of rows : 22
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 [HKM99] B1-b cor 03 33 20.32 +31 07 21.5           ~ 242 0
2 [LM99] L1498 cor 04 10 51.5 +25 09 50           ~ 8 0
3 NAME [BM89] L1495 PoC 04 14 08.2 +28 09 31           ~ 172 0
4 NAME L1495N-A cor 04 18 31.8 +28 27 31           ~ 14 0
5 NAME [BM89] L1521E DNe 04 29 21.0 +26 14 19           ~ 116 1
6 NAME [BM89] TMC-2 PoC 04 32 44.7 +24 25 13           ~ 188 0
7 EM* LkCa 15 Or* 04 39 17.7911622816 +22 21 03.390090984   13.01 12.03 11.61   K5:Ve 792 1
8 IRAS 04368+2557 Y*O 04 39 53.97816 +26 03 09.6804           ~ 309 0
9 NAME Taurus Complex SFR 04 41.0 +25 52           ~ 4971 0
10 [LM99] CB 23 cor 04 43 31.5 +29 39 11           ~ 8 0
11 NAME [BM89] L1517B cor 04 55 18.8 +30 38 04           ~ 163 0
12 HD 31648 Ae* 04 58 46.2655706952 +29 50 36.987625680 7.84 7.78 7.62 7.76 7.43 A5Vep 612 0
13 [LM99] L1512 cor 05 04 09.7 +32 43 09           ~ 4 0
14 LDN 1544 DNe 05 04 16.6 +25 10 48           ~ 965 0
15 OMC 3 MoC 05 35 20.0 -05 01 00           ~ 301 1
16 V* TW Hya TT* 11 01 51.9053285064 -34 42 17.033218380   11.94 10.50 10.626 9.18 K6Ve 2144 1
17 LDN 183 MoC 15 54 12.2 -02 49 42           ~ 799 1
18 IRAS 16293-2422 cor 16 32 22.56 -24 28 31.8           ~ 1357 1
19 EM* AS 209 TT* 16 49 15.3034917000 -14 22 08.643317664   12.62 11.28     K4Ve 494 0
20 HD 163296 Ae* 17 56 21.2881851168 -21 57 21.871819008 7.00 6.93 6.85 6.86 6.67 A3VaekA1mA1 1301 0
21 HD 319139 SB* 18 14 10.4818675368 -32 47 34.516836060   11.47 10.68   9.11 K5+K7 423 0
22 LDN 483 DNe 18 17 35 -04 39.8           ~ 359 0

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