Physical conditions in Centaurus A's northern filaments II. Does the HCO+ emission highlight the presence of shocks?

We present the first observations of HCO$^+$(1--0) and HCN(1--0) emission in the northern filaments of Centaurus A with ALMA. HCO$^+$(1--0) is detected in nine clumps of the Horseshoe complex, with similar velocities as the CO(1--0) emission. Conversely, HCN(1--0) is not detected, and we derive upper limits on the flux. At a resolution of $ 40\: pc$, the line ratio of the velocity-integrated intensities HCO+ /I_ CO $ varies between 0.03 and 0.08, while $I_ HCO+ /I_ HCN $ is higher than unity, with an average lower limit of 1.51. These ratios are significantly higher than what is observed in nearby star-forming galaxies. Moreover, the ratio $I_ HCO+ /I_ CO $ decreases with increasing CO-integrated intensity, contrary to what is observed in the star-forming galaxies. This indicates that the HCO$^+$ emission is enhanced and may not arise from dense gas within the Horseshoe complex. This hypothesis is strengthened by the average line ratio $I_ HCN /I_ CO <0.03$, which suggests that the gas density is rather low. Using non-local thermal equilibrium, large velocity gradient modelling with RADEX, we explored two possible phases of the gas, which we call `diffuse' and `dense' and are characterised by a significant difference in the HCO$^+$ abundance relative to CO, respectively $N_ HCO+ /N_ CO $ and $N_ HCO+ /N_ CO $. The average CO(1--0) and HCO$^+$(1--0) integrated intensities and the upper limit on HCN(1--0) are compatible with both diffuse ($n_H=10^3\: $, $T_ kin =15-165\: K$) and dense gas ($n_H=10^4\: $, $T_ kin K$). The spectral setup of the present observations also covers SiO(2--1). While undetected, the upper limit on SiO(2--1) is not compatible with the RADEX predictions for the dense gas. We conclude that the nine molecular clouds detected in HCO$^+$(1--0) are likely dominated by diffuse molecular gas. While the exact origin of the HCO$^+$(1--0) emission remains to be investigated, it is likely related to the energy injection within the molecular gas that prevents gravitational collapse and star formation.

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Journal
Astronomy and Astrophysics
Published
2024-09-23
DOI
https://doi.org/10.1051/0004-6361/202450952
Primary Topic
Astrophysics and Star Formation Studies
Type
article
Field-Weighted Citation Impact
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article

Physical conditions in Centaurus A's northern filaments II. Does the HCO+ emission highlight the presence of shocks?

P. Guillard, P. Salomé, B. Godard, Q. Salomé et al.
Astronomy and Astrophysics
Astrophysics and Star Formation Studies
article

Physical conditions in Centaurus A's northern filaments II. Does the HCO+ emission highlight the presence of shocks?

P. Guillard, P. Salomé, B. Godard, Q. Salomé, A. Gusdorf
article en

Abstract

We present the first observations of HCO$^+$(1--0) and HCN(1--0) emission in the northern filaments of Centaurus A with ALMA. HCO$^+$(1--0) is detected in nine clumps of the Horseshoe complex, with similar velocities as the CO(1--0) emission. Conversely, HCN(1--0) is not detected, and we derive upper limits on the flux. At a resolution of $ 40\: pc$, the line ratio of the velocity-integrated intensities HCO+ /I_ CO $ varies between 0.03 and 0.08, while $I_ HCO+ /I_ HCN $ is higher than unity, with an average lower limit of 1.51. These ratios are significantly higher than what is observed in nearby star-forming galaxies. Moreover, the ratio $I_ HCO+ /I_ CO $ decreases with increasing CO-integrated intensity, contrary to what is observed in the star-forming galaxies. This indicates that the HCO$^+$ emission is enhanced and may not arise from dense gas within the Horseshoe complex. This hypothesis is strengthened by the average line ratio $I_ HCN /I_ CO <0.03$, which suggests that the gas density is rather low. Using non-local thermal equilibrium, large velocity gradient modelling with RADEX, we explored two possible phases of the gas, which we call `diffuse' and `dense' and are characterised by a significant difference in the HCO$^+$ abundance relative to CO, respectively $N_ HCO+ /N_ CO $ and $N_ HCO+ /N_ CO $. The average CO(1--0) and HCO$^+$(1--0) integrated intensities and the upper limit on HCN(1--0) are compatible with both diffuse ($n_H=10^3\: $, $T_ kin =15-165\: K$) and dense gas ($n_H=10^4\: $, $T_ kin K$). The spectral setup of the present observations also covers SiO(2--1). While undetected, the upper limit on SiO(2--1) is not compatible with the RADEX predictions for the dense gas. We conclude that the nine molecular clouds detected in HCO$^+$(1--0) are likely dominated by diffuse molecular gas. While the exact origin of the HCO$^+$(1--0) emission remains to be investigated, it is likely related to the energy injection within the molecular gas that prevents gravitational collapse and star formation.

Astronomy and Astrophysics
Centre National de la Recherche Scientifique (FR), University of Turku (FI), Turku Centre for Computer Science (FI), Université Paris Sciences et Lettres (FR), Observatoire de Paris (FR), Institut d'Astrophysique de Paris (FR), École Normale Supérieure - PSL (FR), Sorbonne Université (FR), École Normale Supérieure (BI), Laboratoire d’Etudes du Rayonnement et de la Matière en Astrophysique et Atmosphères (FR), Laboratoire de Physique de l'Ecole Normale Supérieure (FR), Aalto University (FI)
National Science Foundation, National Radio Astronomy Observatory, National Science Council, Korea Astronomy and Space Science Institute, National Astronomical Observatory of Japan, Observatoire de Paris, Université de Recherche Paris Sciences et Lettres, National Institutes of Natural Sciences
Openalex Percentile: Top 88%
Astrophysics and Star Formation Studies
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