Extended multi-phase gas reservoirs in the z=4.3 protocluster SPT2349-56: non-stellar ionisation sources?
Kevin C. Harrington, Amit Vishwas, Allison W. S. Man, Carlos De Breuck, Padelis P. Papadopoulos, Paola Andreani, Thomas G. Bisbas
公開日: 2025/7/30
Abstract
We aim to characterize the multi-phase gas in the SPT2349-56 protocluster at z=4.3, known to host one of the most starbursting and AGN-rich high redshift environments.For this purpose we conducted APEX single dish observations of the [CII]158 micron (hereafter [CII]) line towards the Core and North components, previously imaged with the ALMA 12-m array. We also present the first [OIII]88 micron (hereafter [OIII]) line observations in such high redshift protocluster system. We obtain a [CII] line luminosity $\sim$1.7$\times$ more than the one recovered by ALMA towards the Core, while remarkably we recover 4$\times$ more [CII] line emission than the one found in deep ALMA images towards the North component, suggesting that the most massive gas reservoirs lie in the less extreme regions of this protocluster system. A minimum ionised gas mass of $\mathrm M_{\rm min}(H^+)$$ \sim$$3.7\times 10^{10}$\,\Msun\, is deduced from the [OIII] line, amounting to 30\% of the molecular gas mass in the same area. Finally we obtain star formation rate (SFR) estimates using the [OIII] line luminosity, and the corresponding ionised gas mass. These yield values that can surpass the far-IR continuum-derived SFR (under the assumption of a standard stellar IMF), which can be reconciled only if non-stellar ionising sources contribute to the [OIII] line luminosity, or a top-heavy stellar IMF produces a larger fraction of O stars per total stellar mass, a distinct possibility in High-Energy-Particle (HEP) rather than (UV-photon)-dominated environments in clusters. Future work using far-IR fine-structure and molecular/neutral-atomic lines is necessary for determining the thermal/ionisation states of the multi-phase medium and these line ratios must be measured over a wide range of spatial scales, which ultimately requires combining wide-field single-dish and high resolution interferometric observations.