Back to Search
Start Over
Tracing the contraction of the pre-stellar core L1544 with HC17O+J = 1–0 emission.
- Source :
- Astronomy & Astrophysics / Astronomie et Astrophysique; 11/17/2022, Vol. 667, p1-32, 32p
- Publication Year :
- 2022
-
Abstract
- Context. Spectral line profiles of several molecules observed towards the pre-stellar core L1544 appear double-peaked. For abundant molecular species this line morphology has been linked to self-absorption. However, the physical process behind the double-peaked morphology for less abundant species is still under debate. Aims. In order to understand the cause behind the double-peaked spectra of optically thin transitions and their link to the physical structure of pre-stellar cores, we present high-sensitivity and high spectral resolution HC<superscript>17</superscript>O<superscript>+</superscript>J =1−0 observations towards the dust peak in L1544. Methods. We observed the HC<superscript>17</superscript>O<superscript>+</superscript>(1−0) spectrum with the Institut de Radioastronomie Millimétrique (IRAM) 30 m telescope. By using state-of-the-art collisional rate coefficients, a physical model for the core and the fractional abundance profile of HC<superscript>17</superscript>O<superscript>+</superscript>, the hyperfine structure of this molecular ion is modelled for the first time with the radiative transfer code loc applied to the predicted chemical structure of a contracting pre-stellar core. We applied the same analysis to the chemically related C<superscript>17</superscript>O molecule. Results. The observed HC<superscript>17</superscript>O<superscript>+</superscript>(1−0) and C<superscript>17</superscript>O(1−0) lines were successfully reproduced with a non-local thermal equilibrium (LTE) radiative transfer model applied to chemical model predictions for a contracting pre-stellar core. An upscaled velocity profile (by 30%) is needed to reproduce the HC<superscript>17</superscript>O<superscript>+</superscript>(1−0) observations. Conclusions. The double peaks observed in the HC<superscript>17</superscript>O<superscript>+</superscript>(1−0) hyperfine components are due to the contraction motions at densities close to the critical density of the transition (~10<superscript>5</superscript> cm<superscript>−3</superscript>) and to the decreasing HCO<superscript>+</superscript> fractional abundance towards the centre. [ABSTRACT FROM AUTHOR]
Details
- Language :
- English
- ISSN :
- 00046361
- Volume :
- 667
- Database :
- Complementary Index
- Journal :
- Astronomy & Astrophysics / Astronomie et Astrophysique
- Publication Type :
- Academic Journal
- Accession number :
- 160457303
- Full Text :
- https://doi.org/10.1051/0004-6361/202243927