Quentin Salomé, Philippe Salomé, Benjamin Godard, Pierre Guillard, Antoine Gusdorf
{"title":"Physical conditions in Centaurus A's northern filaments II: Does the HCO$^+$ emission highlight the presence of shocks?","authors":"Quentin Salomé, Philippe Salomé, Benjamin Godard, Pierre Guillard, Antoine Gusdorf","doi":"arxiv-2409.11031","DOIUrl":null,"url":null,"abstract":"Abridged: We present the first observation of the HCO+(1-0) and HCN(1-0)\nemission in the northern filaments of Centaurus A with ALMA. HCO+(1-0) is\ndetected in 9 clumps of the Horseshoe complex, with similar velocities as the\nCO(1-0) emission. Conversely, the HCN(1-0) is not detected and we derive upper\nlimits on the flux. At a resolution of ~40 pc, the line ratio of the\nvelocity-integrated intensities I_HCO+/I_CO varies between 0.03 and 0.08, while\nI_HCO+/I_HCN is higher than unity with an average lower limit of 1.51. These\nratios are significantly higher than what is observed in nearby star-forming\ngalaxies. Moreover, the ratio I_HCO+/I_CO decreases with increasing CO\nintegrated intensity, contrary to what is observed in the star-forming\ngalaxies. This indicates that the HCO+ emission is enhanced and may not arise\nfrom dense gas within the Horseshoe complex. This hypothesis is strengthened by\nthe average line ratio I_HCN/I_CO<0.03 which suggests that the gas density is\nrather low. Using non-LTE, large velocity gradient modelling with RADEX, we\nexplored two possible phases of the gas, that we call \"diffuse\" and \"dense\",\nand are characterised by a significant difference in the HCO+ relative\nabundance to CO, respectively N_HCO+/N_CO=10^-3 and 3x10^-5. The average\nCO(1-0) and HCO+(1-0) integrated intensities and the upper limit on HCN(1-0)\nare compatible with both \"diffuse\" and \"dense\" gas. The spectral setup of the\npresent observations also covers the SiO(2-1). While undetected, the upper\nlimit on SiO(2-1) is not compatible with the RADEX predictions for the \"dense\"\ngas. We conclude that the 9 molecular clouds detected in HCO+(1-0) are likely\ndominated by diffuse molecular gas. While the exact origin of the HCO+(1-0)\nemission remains to be investigated, it is likely related to the energy\ninjection within the molecular gas that prevents gravitational collapse and\nstar formation.","PeriodicalId":501187,"journal":{"name":"arXiv - PHYS - Astrophysics of Galaxies","volume":"20 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Astrophysics of Galaxies","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.11031","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Abridged: We present the first observation of the HCO+(1-0) and HCN(1-0)
emission in the northern filaments of Centaurus A with ALMA. HCO+(1-0) is
detected in 9 clumps of the Horseshoe complex, with similar velocities as the
CO(1-0) emission. Conversely, the 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 I_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-LTE, large velocity gradient modelling with RADEX, we
explored two possible phases of the gas, that we call "diffuse" and "dense",
and are characterised by a significant difference in the HCO+ relative
abundance to CO, respectively N_HCO+/N_CO=10^-3 and 3x10^-5. The average
CO(1-0) and HCO+(1-0) integrated intensities and the upper limit on HCN(1-0)
are compatible with both "diffuse" and "dense" gas. The spectral setup of the
present observations also covers the 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 9 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.