Rodrigo Córdova Rosado, Andy D. Goulding, Jenny E. Greene, Grayson C. Petter, Ryan C. Hickox, Nickolas Kokron, Michael A. Strauss, Jahmour J. Givans, Yoshiki Toba, Cassandra Starr Henderson
{"title":"HSC-SSP中红色发光星系与ML选择的AGN的交叉相关性:停留在更大质量光晕中的未被遮挡的AGN","authors":"Rodrigo Córdova Rosado, Andy D. Goulding, Jenny E. Greene, Grayson C. Petter, Ryan C. Hickox, Nickolas Kokron, Michael A. Strauss, Jahmour J. Givans, Yoshiki Toba, Cassandra Starr Henderson","doi":"arxiv-2409.08314","DOIUrl":null,"url":null,"abstract":"Active galactic nuclei (AGN) are the signposts of black hole growth, and\nlikely play an important role in galaxy evolution. An outstanding question is\nwhether AGN of different spectral types indicate different evolutionary stages\nin the coevolution of black holes and galaxies. We present the angular\ncorrelation function between an AGN sample selected from the Hyper Suprime\nCamera Subaru Strategic Program (HSC-SSP) optical + Wide-field Infrared Survey\nExplorer (WISE) mid-IR photometry, and a luminous red galaxy (LRG) sample from\nHSC-SSP. We investigate AGN clustering strength as a function of their\nluminosity and spectral features across three independent HSC fields totaling\n$\\sim600\\,{\\rm deg^{2}}$, for $z\\in0.6-1.2$ and AGN with $L_{6\\mu\nm}>3\\times10^{44}{\\rm\\,erg\\,s^{-1}}$. There are $\\sim28,500$ AGN and $\\sim1.5$\nmillion LRGs in our primary analysis. We determine the inferred average halo\nmass for the full AGN sample ($M_h \\approx 10^{12.9}h^{-1}M_\\odot$), and note\nthat it does not evolve significantly as a function of redshift (over this\nnarrow range) or luminosity. We find that, on average, unobscured AGN ($M_h\n\\approx10^{13.3}h^{-1}M_\\odot$) occupy $\\sim4.5\\times$ more massive halos than\nobscured AGN ($M_h \\approx10^{12.6}h^{-1}M_\\odot$), at $5\\sigma$ statistical\nsignificance using 1-D uncertainties, and at $3\\sigma$ using the full\ncovariance matrix, suggesting a physical difference between unobscured and\nobscured AGN, beyond the line-of-sight viewing angle. Furthermore, we find\nevidence for a halo mass dependence on reddening level within the Type I AGN\npopulation, which could support the existence of a previously claimed\ndust-obscured phase in AGN-host galaxy coevolution. However, we also find that\neven quite small systematic shifts in the redshift distributions of the AGN\nsample could plausibly explain current and previously observed differences in\n$M_{h}$.","PeriodicalId":501187,"journal":{"name":"arXiv - PHYS - Astrophysics of Galaxies","volume":"52 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Cross-correlation of Luminous Red Galaxies with ML-selected AGN in HSC-SSP: Unobscured AGN residing in more massive halos\",\"authors\":\"Rodrigo Córdova Rosado, Andy D. Goulding, Jenny E. Greene, Grayson C. Petter, Ryan C. Hickox, Nickolas Kokron, Michael A. Strauss, Jahmour J. Givans, Yoshiki Toba, Cassandra Starr Henderson\",\"doi\":\"arxiv-2409.08314\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Active galactic nuclei (AGN) are the signposts of black hole growth, and\\nlikely play an important role in galaxy evolution. An outstanding question is\\nwhether AGN of different spectral types indicate different evolutionary stages\\nin the coevolution of black holes and galaxies. We present the angular\\ncorrelation function between an AGN sample selected from the Hyper Suprime\\nCamera Subaru Strategic Program (HSC-SSP) optical + Wide-field Infrared Survey\\nExplorer (WISE) mid-IR photometry, and a luminous red galaxy (LRG) sample from\\nHSC-SSP. We investigate AGN clustering strength as a function of their\\nluminosity and spectral features across three independent HSC fields totaling\\n$\\\\sim600\\\\,{\\\\rm deg^{2}}$, for $z\\\\in0.6-1.2$ and AGN with $L_{6\\\\mu\\nm}>3\\\\times10^{44}{\\\\rm\\\\,erg\\\\,s^{-1}}$. There are $\\\\sim28,500$ AGN and $\\\\sim1.5$\\nmillion LRGs in our primary analysis. We determine the inferred average halo\\nmass for the full AGN sample ($M_h \\\\approx 10^{12.9}h^{-1}M_\\\\odot$), and note\\nthat it does not evolve significantly as a function of redshift (over this\\nnarrow range) or luminosity. We find that, on average, unobscured AGN ($M_h\\n\\\\approx10^{13.3}h^{-1}M_\\\\odot$) occupy $\\\\sim4.5\\\\times$ more massive halos than\\nobscured AGN ($M_h \\\\approx10^{12.6}h^{-1}M_\\\\odot$), at $5\\\\sigma$ statistical\\nsignificance using 1-D uncertainties, and at $3\\\\sigma$ using the full\\ncovariance matrix, suggesting a physical difference between unobscured and\\nobscured AGN, beyond the line-of-sight viewing angle. Furthermore, we find\\nevidence for a halo mass dependence on reddening level within the Type I AGN\\npopulation, which could support the existence of a previously claimed\\ndust-obscured phase in AGN-host galaxy coevolution. However, we also find that\\neven quite small systematic shifts in the redshift distributions of the AGN\\nsample could plausibly explain current and previously observed differences in\\n$M_{h}$.\",\"PeriodicalId\":501187,\"journal\":{\"name\":\"arXiv - PHYS - Astrophysics of Galaxies\",\"volume\":\"52 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-12\",\"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-2409.08314\",\"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-2409.08314","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Cross-correlation of Luminous Red Galaxies with ML-selected AGN in HSC-SSP: Unobscured AGN residing in more massive halos
Active galactic nuclei (AGN) are the signposts of black hole growth, and
likely play an important role in galaxy evolution. An outstanding question is
whether AGN of different spectral types indicate different evolutionary stages
in the coevolution of black holes and galaxies. We present the angular
correlation function between an AGN sample selected from the Hyper Suprime
Camera Subaru Strategic Program (HSC-SSP) optical + Wide-field Infrared Survey
Explorer (WISE) mid-IR photometry, and a luminous red galaxy (LRG) sample from
HSC-SSP. We investigate AGN clustering strength as a function of their
luminosity and spectral features across three independent HSC fields totaling
$\sim600\,{\rm deg^{2}}$, for $z\in0.6-1.2$ and AGN with $L_{6\mu
m}>3\times10^{44}{\rm\,erg\,s^{-1}}$. There are $\sim28,500$ AGN and $\sim1.5$
million LRGs in our primary analysis. We determine the inferred average halo
mass for the full AGN sample ($M_h \approx 10^{12.9}h^{-1}M_\odot$), and note
that it does not evolve significantly as a function of redshift (over this
narrow range) or luminosity. We find that, on average, unobscured AGN ($M_h
\approx10^{13.3}h^{-1}M_\odot$) occupy $\sim4.5\times$ more massive halos than
obscured AGN ($M_h \approx10^{12.6}h^{-1}M_\odot$), at $5\sigma$ statistical
significance using 1-D uncertainties, and at $3\sigma$ using the full
covariance matrix, suggesting a physical difference between unobscured and
obscured AGN, beyond the line-of-sight viewing angle. Furthermore, we find
evidence for a halo mass dependence on reddening level within the Type I AGN
population, which could support the existence of a previously claimed
dust-obscured phase in AGN-host galaxy coevolution. However, we also find that
even quite small systematic shifts in the redshift distributions of the AGN
sample could plausibly explain current and previously observed differences in
$M_{h}$.