Andrew W. S. Cook, Freeke van de Voort, Rüdiger Pakmor, Robert J. J. Grand
{"title":"环银河介质中物理和可观测特性的晕质量依赖性","authors":"Andrew W. S. Cook, Freeke van de Voort, Rüdiger Pakmor, Robert J. J. Grand","doi":"arxiv-2409.05578","DOIUrl":null,"url":null,"abstract":"We study the dependence of the physical and observable properties of the CGM\non its halo mass. We analyse 22 simulations from the Auriga suite of high\nresolution cosmological `zoom-in' simulations at $z=0$ with halo masses\n$10^{10}~\\text{M}_{\\odot}\\leq\\text{M}_{\\mathrm{200c}}\\leq10^{12}~\\text{M}_{\\odot}$.\nWe find a larger scatter in temperature and smaller scatter in metallicity in\nmore massive haloes. The scatter of temperature and metallicity as a function\nof radius increases out to larger radii. The median and scatter of the\nvolume-weighted density and mass-weighted radial velocity show no significant\ndependence on halo mass. Our results highlight that the CGM is more multiphase\nin haloes of higher mass. We additionally investigate column densities for HI\nand the metal ions CIV, OVI, MgII and SiII as a function of stellar mass and\nradius. We find the HI and metal ion column densities increase with stellar\nmass at sufficiently large radii ($R\\gtrsim{0.2}$R$_{\\mathrm{200c}}$). We find\ngood agreement between our HI column densities and observations outside $20$%\nof the virial radius and overpredict within $20$%. MgII and SiII are similarly\noverpredicted within $20$% of the virial radius, but drop off steeply at larger\nradii. Our OVI column densities underpredict observations for stellar masses\nbetween\n$10^{9.7}~\\text{M}_{\\odot}\\leq\\text{M}_{\\star}<10^{10.8}~\\text{M}_{\\odot}$ with\nreasonable agreement at $10^{10.8}~\\text{M}_{\\odot}$. CIV column densities\nagree with observational detections above a halo mass of\n$10^{9.7}~\\text{M}_{\\odot}$. We find that OVI (MgII) traces the highest\n(lowest) temperatures, and lowest (highest) density and metallicity. OVI and\nCIV are photo-ionized (collisionally ionized) at low (high) halo masses with a\ntransition to higher temperatures at $10^{11}~\\text{M}_{\\odot}$. However, there\nis no clear trend for the radial velocity of the ions.","PeriodicalId":501187,"journal":{"name":"arXiv - PHYS - Astrophysics of Galaxies","volume":"31 3 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"The halo mass dependence of physical and observable properties in the circumgalactic medium\",\"authors\":\"Andrew W. S. Cook, Freeke van de Voort, Rüdiger Pakmor, Robert J. J. Grand\",\"doi\":\"arxiv-2409.05578\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We study the dependence of the physical and observable properties of the CGM\\non its halo mass. We analyse 22 simulations from the Auriga suite of high\\nresolution cosmological `zoom-in' simulations at $z=0$ with halo masses\\n$10^{10}~\\\\text{M}_{\\\\odot}\\\\leq\\\\text{M}_{\\\\mathrm{200c}}\\\\leq10^{12}~\\\\text{M}_{\\\\odot}$.\\nWe find a larger scatter in temperature and smaller scatter in metallicity in\\nmore massive haloes. The scatter of temperature and metallicity as a function\\nof radius increases out to larger radii. The median and scatter of the\\nvolume-weighted density and mass-weighted radial velocity show no significant\\ndependence on halo mass. Our results highlight that the CGM is more multiphase\\nin haloes of higher mass. We additionally investigate column densities for HI\\nand the metal ions CIV, OVI, MgII and SiII as a function of stellar mass and\\nradius. We find the HI and metal ion column densities increase with stellar\\nmass at sufficiently large radii ($R\\\\gtrsim{0.2}$R$_{\\\\mathrm{200c}}$). We find\\ngood agreement between our HI column densities and observations outside $20$%\\nof the virial radius and overpredict within $20$%. MgII and SiII are similarly\\noverpredicted within $20$% of the virial radius, but drop off steeply at larger\\nradii. Our OVI column densities underpredict observations for stellar masses\\nbetween\\n$10^{9.7}~\\\\text{M}_{\\\\odot}\\\\leq\\\\text{M}_{\\\\star}<10^{10.8}~\\\\text{M}_{\\\\odot}$ with\\nreasonable agreement at $10^{10.8}~\\\\text{M}_{\\\\odot}$. CIV column densities\\nagree with observational detections above a halo mass of\\n$10^{9.7}~\\\\text{M}_{\\\\odot}$. We find that OVI (MgII) traces the highest\\n(lowest) temperatures, and lowest (highest) density and metallicity. OVI and\\nCIV are photo-ionized (collisionally ionized) at low (high) halo masses with a\\ntransition to higher temperatures at $10^{11}~\\\\text{M}_{\\\\odot}$. However, there\\nis no clear trend for the radial velocity of the ions.\",\"PeriodicalId\":501187,\"journal\":{\"name\":\"arXiv - PHYS - Astrophysics of Galaxies\",\"volume\":\"31 3 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-09\",\"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-2409.05578\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Astrophysics of Galaxies","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.05578","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
The halo mass dependence of physical and observable properties in the circumgalactic medium
We study the dependence of the physical and observable properties of the CGM
on its halo mass. We analyse 22 simulations from the Auriga suite of high
resolution cosmological `zoom-in' simulations at $z=0$ with halo masses
$10^{10}~\text{M}_{\odot}\leq\text{M}_{\mathrm{200c}}\leq10^{12}~\text{M}_{\odot}$.
We find a larger scatter in temperature and smaller scatter in metallicity in
more massive haloes. The scatter of temperature and metallicity as a function
of radius increases out to larger radii. The median and scatter of the
volume-weighted density and mass-weighted radial velocity show no significant
dependence on halo mass. Our results highlight that the CGM is more multiphase
in haloes of higher mass. We additionally investigate column densities for HI
and the metal ions CIV, OVI, MgII and SiII as a function of stellar mass and
radius. We find the HI and metal ion column densities increase with stellar
mass at sufficiently large radii ($R\gtrsim{0.2}$R$_{\mathrm{200c}}$). We find
good agreement between our HI column densities and observations outside $20$%
of the virial radius and overpredict within $20$%. MgII and SiII are similarly
overpredicted within $20$% of the virial radius, but drop off steeply at larger
radii. Our OVI column densities underpredict observations for stellar masses
between
$10^{9.7}~\text{M}_{\odot}\leq\text{M}_{\star}<10^{10.8}~\text{M}_{\odot}$ with
reasonable agreement at $10^{10.8}~\text{M}_{\odot}$. CIV column densities
agree with observational detections above a halo mass of
$10^{9.7}~\text{M}_{\odot}$. We find that OVI (MgII) traces the highest
(lowest) temperatures, and lowest (highest) density and metallicity. OVI and
CIV are photo-ionized (collisionally ionized) at low (high) halo masses with a
transition to higher temperatures at $10^{11}~\text{M}_{\odot}$. However, there
is no clear trend for the radial velocity of the ions.