{"title":"阿斯特丽德模拟:黑洞和星系演化至 z=0.5 以及星系淬火的不同演化途径","authors":"Yueying Ni, Nianyi Chen, Yihao Zhou, Minjung Park, Yanhui Yang, Tiziana DiMatteo, Simeon Bird, Rupert Croft","doi":"arxiv-2409.10666","DOIUrl":null,"url":null,"abstract":"We present new results from the ASTRID simulation from $z=3$ to $z=0.5$,\ncovering the epoch of cosmic noon. The galaxy stellar mass function, as well as\nthe black hole mass and luminosity functions in ASTRID, exhibit good agreement\nwith recent observational constraints. We study the $M_{\\rm BH}$-$M_*$ scaling\nrelation and its connections to AGN luminosity, galaxy color, and star\nformation rate, demonstrating that AGN feedback plays a crucial role in the\nquenching of massive galaxies ($M_*>10^{10.5} M_{\\odot}$). Although AGN\nfeedback suppresses star formation through quenching, AGN-host galaxies still\nexhibit statistically higher levels of star formation compared to inactive\nones, due to the positive correlation between AGN activity and star formation,\nboth fueled by a shared gas reservoir. The fraction of quiescent galaxies in\nASTRID increases with both galaxy mass and redshift evolution, aligning well\nwith observational trends. We find that different quenching mechanisms can\nleave distinct morphological imprints on quenched galaxies. Massive, compact\nquiescent galaxies typically experience shorter quenching timescales, have\nyounger central regions, and host overmassive black holes. This is usually due\nto a compaction-like quenching mechanism that funnels gas into the galaxy\ncenter, leading to starbursts and triggering AGN kinetic feedback. In contrast,\nquiescent galaxies with more diffuse morphologies generally experience\n`inside-out' quenching, which is characterized by older central regions\ncompared to the outskirts. These galaxies typically experience longer quenching\ntimescales due to quenching processes operating on a larger halo scale, which\ngradually deplete the galactic star-forming gas. Data of the \\astrid simulation\ndown to $z=0.5$ is available at \\url{https://astrid.psc.edu}.","PeriodicalId":501187,"journal":{"name":"arXiv - PHYS - Astrophysics of Galaxies","volume":"35 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"The Astrid Simulation: Evolution of black holes and galaxies to z=0.5 and different evolution pathways for galaxy quenching\",\"authors\":\"Yueying Ni, Nianyi Chen, Yihao Zhou, Minjung Park, Yanhui Yang, Tiziana DiMatteo, Simeon Bird, Rupert Croft\",\"doi\":\"arxiv-2409.10666\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We present new results from the ASTRID simulation from $z=3$ to $z=0.5$,\\ncovering the epoch of cosmic noon. The galaxy stellar mass function, as well as\\nthe black hole mass and luminosity functions in ASTRID, exhibit good agreement\\nwith recent observational constraints. We study the $M_{\\\\rm BH}$-$M_*$ scaling\\nrelation and its connections to AGN luminosity, galaxy color, and star\\nformation rate, demonstrating that AGN feedback plays a crucial role in the\\nquenching of massive galaxies ($M_*>10^{10.5} M_{\\\\odot}$). Although AGN\\nfeedback suppresses star formation through quenching, AGN-host galaxies still\\nexhibit statistically higher levels of star formation compared to inactive\\nones, due to the positive correlation between AGN activity and star formation,\\nboth fueled by a shared gas reservoir. The fraction of quiescent galaxies in\\nASTRID increases with both galaxy mass and redshift evolution, aligning well\\nwith observational trends. We find that different quenching mechanisms can\\nleave distinct morphological imprints on quenched galaxies. Massive, compact\\nquiescent galaxies typically experience shorter quenching timescales, have\\nyounger central regions, and host overmassive black holes. This is usually due\\nto a compaction-like quenching mechanism that funnels gas into the galaxy\\ncenter, leading to starbursts and triggering AGN kinetic feedback. In contrast,\\nquiescent galaxies with more diffuse morphologies generally experience\\n`inside-out' quenching, which is characterized by older central regions\\ncompared to the outskirts. These galaxies typically experience longer quenching\\ntimescales due to quenching processes operating on a larger halo scale, which\\ngradually deplete the galactic star-forming gas. Data of the \\\\astrid simulation\\ndown to $z=0.5$ is available at \\\\url{https://astrid.psc.edu}.\",\"PeriodicalId\":501187,\"journal\":{\"name\":\"arXiv - PHYS - Astrophysics of Galaxies\",\"volume\":\"35 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-16\",\"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-2409.10666\",\"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-2409.10666","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
The Astrid Simulation: Evolution of black holes and galaxies to z=0.5 and different evolution pathways for galaxy quenching
We present new results from the ASTRID simulation from $z=3$ to $z=0.5$,
covering the epoch of cosmic noon. The galaxy stellar mass function, as well as
the black hole mass and luminosity functions in ASTRID, exhibit good agreement
with recent observational constraints. We study the $M_{\rm BH}$-$M_*$ scaling
relation and its connections to AGN luminosity, galaxy color, and star
formation rate, demonstrating that AGN feedback plays a crucial role in the
quenching of massive galaxies ($M_*>10^{10.5} M_{\odot}$). Although AGN
feedback suppresses star formation through quenching, AGN-host galaxies still
exhibit statistically higher levels of star formation compared to inactive
ones, due to the positive correlation between AGN activity and star formation,
both fueled by a shared gas reservoir. The fraction of quiescent galaxies in
ASTRID increases with both galaxy mass and redshift evolution, aligning well
with observational trends. We find that different quenching mechanisms can
leave distinct morphological imprints on quenched galaxies. Massive, compact
quiescent galaxies typically experience shorter quenching timescales, have
younger central regions, and host overmassive black holes. This is usually due
to a compaction-like quenching mechanism that funnels gas into the galaxy
center, leading to starbursts and triggering AGN kinetic feedback. In contrast,
quiescent galaxies with more diffuse morphologies generally experience
`inside-out' quenching, which is characterized by older central regions
compared to the outskirts. These galaxies typically experience longer quenching
timescales due to quenching processes operating on a larger halo scale, which
gradually deplete the galactic star-forming gas. Data of the \astrid simulation
down to $z=0.5$ is available at \url{https://astrid.psc.edu}.