Extended multi-phase gas reservoirs in the z = 4.3 protocluster SPT2349-56: Non-stellar ionisation sources?

IF 5.8 2区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS
Kevin C. Harrington, Amit Vishwas, Allison W. S. Man, Carlos De Breuck, Padelis P. Papadopoulos, Paola Andreani, Thomas. G. Bisbas
{"title":"Extended multi-phase gas reservoirs in the z = 4.3 protocluster SPT2349-56: Non-stellar ionisation sources?","authors":"Kevin C. Harrington, Amit Vishwas, Allison W. S. Man, Carlos De Breuck, Padelis P. Papadopoulos, Paola Andreani, Thomas. G. Bisbas","doi":"10.1051/0004-6361/202555071","DOIUrl":null,"url":null,"abstract":"We aim to characterise the multi-phase gas in the SPT2349-56 protocluster at <i>z<i/> = 4.3, which is known to host one of the most starbursting and Active Galactic Nuclei (AGN)-rich high redshift environments. For this purpose, we conducted Atacama Pathfinder EXperiment (APEX) single-dish observations of the [C II] 158 μm (hereafter [C II]) line towards the core and north components, which were previously imaged with the Atacama Large Millimeter/submillimeter Array (ALMA). We also present the first [O III] 88 μm (hereafter [O III]) line observations in such a high-redshift protocluster system. We obtain a [C II] line luminosity approximately 1.7 times greater than that recovered by ALMA towards the core, while we recover four times more [C II] line emission than that found in deep ALMA images towards the north component. This suggests that the most massive gas reservoirs lie in the less extreme regions of this protocluster system. A minimum ionised gas mass of M<sub>min<sub/>(<i>H<i/><sup>+<sup/>)∼3.7 × 10<sup>10<sup/> M<sub>⊙<sub/> is deduced from the [O III] line, which amounts to 30% of the molecular gas mass in the same area, indicating that a full map of the cluster is necessary for determining the large-scale value. Finally, we obtain star formation rate (SFR) estimates using the [O III] line luminosity and the corresponding ionised gas mass. These yield values that can surpass the far-infrared (IR) continuum-derived SFR under the assumption of a standard stellar Initial Mass Function (IMF), which can be reconciled only if non-stellar ionising sources contribute to the [O III] line luminosity, or if a top-heavy stellar IMF produces a larger fraction of O stars per total stellar mass. This is a distinct possibility in high-energy-particle (HEP)-dominated, rather than UV-photon-dominated, environments in clusters. Future work using far-IR fine-structure and molecular or neutral-atomic lines is necessary to determine the thermal and ionisation states of the multi-phase medium in this protocluster, to understand their maintenance, and to resolve the apparent SFR discrepancy. These line ratios must be measured over a wide range of spatial scales, from individual galaxies up to circumgalactic medium (CGM) and intracluster medium (ICM) scales, which ultimately requires combining wide-field single-dish and high-resolution interferometric observations of such lines in protocluster environments where HEP- and UV-dominated ISM phases can co-exist.","PeriodicalId":8571,"journal":{"name":"Astronomy & Astrophysics","volume":"25 1","pages":""},"PeriodicalIF":5.8000,"publicationDate":"2025-09-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Astronomy & Astrophysics","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1051/0004-6361/202555071","RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"ASTRONOMY & ASTROPHYSICS","Score":null,"Total":0}
引用次数: 0

Abstract

We aim to characterise the multi-phase gas in the SPT2349-56 protocluster at z = 4.3, which is known to host one of the most starbursting and Active Galactic Nuclei (AGN)-rich high redshift environments. For this purpose, we conducted Atacama Pathfinder EXperiment (APEX) single-dish observations of the [C II] 158 μm (hereafter [C II]) line towards the core and north components, which were previously imaged with the Atacama Large Millimeter/submillimeter Array (ALMA). We also present the first [O III] 88 μm (hereafter [O III]) line observations in such a high-redshift protocluster system. We obtain a [C II] line luminosity approximately 1.7 times greater than that recovered by ALMA towards the core, while we recover four times more [C II] line emission than that found in deep ALMA images towards the north component. This suggests that the most massive gas reservoirs lie in the less extreme regions of this protocluster system. A minimum ionised gas mass of Mmin(H+)∼3.7 × 1010 M is deduced from the [O III] line, which amounts to 30% of the molecular gas mass in the same area, indicating that a full map of the cluster is necessary for determining the large-scale value. Finally, we obtain star formation rate (SFR) estimates using the [O III] line luminosity and the corresponding ionised gas mass. These yield values that can surpass the far-infrared (IR) continuum-derived SFR under the assumption of a standard stellar Initial Mass Function (IMF), which can be reconciled only if non-stellar ionising sources contribute to the [O III] line luminosity, or if a top-heavy stellar IMF produces a larger fraction of O stars per total stellar mass. This is a distinct possibility in high-energy-particle (HEP)-dominated, rather than UV-photon-dominated, environments in clusters. Future work using far-IR fine-structure and molecular or neutral-atomic lines is necessary to determine the thermal and ionisation states of the multi-phase medium in this protocluster, to understand their maintenance, and to resolve the apparent SFR discrepancy. These line ratios must be measured over a wide range of spatial scales, from individual galaxies up to circumgalactic medium (CGM) and intracluster medium (ICM) scales, which ultimately requires combining wide-field single-dish and high-resolution interferometric observations of such lines in protocluster environments where HEP- and UV-dominated ISM phases can co-exist.
z = 4.3原星团SPT2349-56中的扩展多相气藏:非恒星电离源?
我们的目标是表征z = 4.3的SPT2349-56原星团中的多相气体,该原星团已知拥有最富星爆和活动星系核(AGN)的高红移环境之一。为此,我们利用阿塔卡马大型毫米波/亚毫米波阵列(ALMA)进行了阿塔卡马探路者实验(APEX)单碟观测,观测了[C II] 158 μm(以下简称[C II])向核心和北分量的线。我们还提出了在这样一个高红移原星团系统中的第一个[O III] 88 μm(以下简称[O III])谱线观测。我们获得的[C II]线亮度大约是ALMA向核心方向恢复的1.7倍,而我们恢复的[C II]线发射比在深ALMA图像中发现的向北分量多4倍。这表明,最巨大的气藏位于这个原星团系统的较不极端的区域。从[O III]谱线推断出最小电离气体质量为Mmin(H+) ~ 3.7 × 1010 M⊙,相当于同一区域内分子气体质量的30%,这表明要确定大尺度值,需要绘制星系团的全图。最后,我们使用[O III]线光度和相应的电离气体质量获得恒星形成速率(SFR)估计。在标准恒星初始质量函数(IMF)的假设下,这些产率值可以超过远红外(IR)连续衍生的SFR,这只有在非恒星电离源对[O III]线光度有贡献的情况下才能调和,或者如果一个头重头轻的恒星IMF在每颗总恒星质量中产生更大比例的O恒星。在以高能粒子(HEP)为主,而不是以紫外光子为主的集群环境中,这是一种明显的可能性。未来有必要利用远红外精细结构和分子或中性原子谱线来确定该原团簇中多相介质的热和电离状态,了解它们的维持情况,并解决明显的SFR差异。这些谱线比率必须在广泛的空间尺度上测量,从单个星系到环星系介质(CGM)和星系团内介质(ICM)尺度,最终需要在HEP和uv主导的ISM相位共存的原星系团环境中结合宽视场单碟和高分辨率干涉观测。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
Astronomy & Astrophysics
Astronomy & Astrophysics 地学天文-天文与天体物理
CiteScore
10.20
自引率
27.70%
发文量
2105
审稿时长
1-2 weeks
期刊介绍: Astronomy & Astrophysics is an international Journal that publishes papers on all aspects of astronomy and astrophysics (theoretical, observational, and instrumental) independently of the techniques used to obtain the results.
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:604180095
Book学术官方微信