Yang Sun, Jianwei Lyu, George H. Rieke, Zhiyuan Ji, Fengwu Sun, Yongda Zhu, Andrew J. Bunker, Phillip A. Cargile, Chiara Circosta, Francesco D'Eugenio, Eiichi Egami, Kevin Hainline, Jakob M. Helton, Pierluigi Rinaldi, Brant E. Robertson, Jan Scholtz, Irene Shivaei, Meredith A. Stone, Sandro Tacchella, Christina C. Williams, Christopher N. A. Willmer, Chris Willott
{"title":"No evidence for a significant evolution of $M_{\\bullet}$-$M_*$ relation up to z$\\sim$4","authors":"Yang Sun, Jianwei Lyu, George H. Rieke, Zhiyuan Ji, Fengwu Sun, Yongda Zhu, Andrew J. Bunker, Phillip A. Cargile, Chiara Circosta, Francesco D'Eugenio, Eiichi Egami, Kevin Hainline, Jakob M. Helton, Pierluigi Rinaldi, Brant E. Robertson, Jan Scholtz, Irene Shivaei, Meredith A. Stone, Sandro Tacchella, Christina C. Williams, Christopher N. A. Willmer, Chris Willott","doi":"arxiv-2409.06796","DOIUrl":null,"url":null,"abstract":"Over the past two decades, tight correlations between black hole masses\n($M_\\bullet$) and their host galaxy properties have been firmly established at\nlow-$z$ ($z<1$), indicating coevolution of supermassive black holes and\ngalaxies. However, the situation at high-$z$, especially beyond cosmic noon\n($z\\gtrsim2.5$), is controversial. With a combination of \\emph{JWST}\nNIRCam/wide field slitless spectroscopy (WFSS) from FRESCO, CONGRESS and deep\nmulti-band NIRCam/image data from JADES in the GOODS fields, we study the black\nhole to galaxy mass relation at z$\\sim$1--4. After identifying 18 broad-line\nactive galactic nuclei (BL AGNs) at $0.9<z<3.6$ (with 8 at $z>2.5$) from the\nWFSS data, we measure their black hole masses based on broad near-infrared\nlines (Pa $\\alpha$, Pa $\\beta$, and He\\,I $\\lambda$10833\\,\\AA), and constrain\ntheir stellar masses ($M_{*}$) from AGN-galaxy image decomposition or SED\ndecomposition. Taking account of the observational biases, the intrinsic\nscatter of the $M_{\\bullet}-M_{*}$ relation, and the errors in mass\nmeasurements, we find no significant difference in the $M_{\\bullet}/M_{*}$\nratio for 2.5 $< $ z $ <$ 3.6 compared to that at lower redshifts ($1 < z <\n2.5$), suggesting no evolution of the $M_{\\bullet} - M_{*}$ relation up to\nz$\\sim$4.","PeriodicalId":501187,"journal":{"name":"arXiv - PHYS - Astrophysics of Galaxies","volume":"109 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Astrophysics of Galaxies","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.06796","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Over the past two decades, tight correlations between black hole masses
($M_\bullet$) and their host galaxy properties have been firmly established at
low-$z$ ($z<1$), indicating coevolution of supermassive black holes and
galaxies. However, the situation at high-$z$, especially beyond cosmic noon
($z\gtrsim2.5$), is controversial. With a combination of \emph{JWST}
NIRCam/wide field slitless spectroscopy (WFSS) from FRESCO, CONGRESS and deep
multi-band NIRCam/image data from JADES in the GOODS fields, we study the black
hole to galaxy mass relation at z$\sim$1--4. After identifying 18 broad-line
active galactic nuclei (BL AGNs) at $0.92.5$) from the
WFSS data, we measure their black hole masses based on broad near-infrared
lines (Pa $\alpha$, Pa $\beta$, and He\,I $\lambda$10833\,\AA), and constrain
their stellar masses ($M_{*}$) from AGN-galaxy image decomposition or SED
decomposition. Taking account of the observational biases, the intrinsic
scatter of the $M_{\bullet}-M_{*}$ relation, and the errors in mass
measurements, we find no significant difference in the $M_{\bullet}/M_{*}$
ratio for 2.5 $< $ z $ <$ 3.6 compared to that at lower redshifts ($1 < z <
2.5$), suggesting no evolution of the $M_{\bullet} - M_{*}$ relation up to
z$\sim$4.