2022ApJ...926...76U


Query : 2022ApJ...926...76U

2022ApJ...926...76U - Astrophys. J., 926, 76-76 (2022/February-2)

A Wide and Deep Exploration of Radio Galaxies with Subaru HSC (WERGS). VI. Distant Filamentary Structures Pointed Out by High-z Radio Galaxies at z ∼ 4.

UCHIYAMA H., YAMASHITA T., TOSHIKAWA J., KASHIKAWA N., ICHIKAWA K., KUBO M., ITO K., KAWAKATU N., NAGAO T., TOBA Y., ONO Y., HARIKANE Y., IMANISHI M., KAJISAWA M., LEE C.-H. and LIANG Y.

Abstract (from CDS):

We present the environmental properties around high-z radio galaxies (HzRGs) at z ∼ 4, which have been poorly investigated because of their rarity. We use the largest samples of HzRGs and g-dropout galaxy overdense regions at z ∼ 4, which were constructed from the Hyper Suprime-Cam Subaru Strategic Program, to characterize the HzRG environments statistically. We measure the g-dropout galaxy overdensities around 21 HzRGs whose rest-frame 1.4 GHz radio luminosities (L _1.4 GHz_) are 1026–27 W Hz–1. We find that the overdensities around the faint HzRGs with L _1.4 GHz_ ∼ 1026.0–26.5 W Hz–1 tend to be higher than those of the g-dropout galaxies. On the other hand, no significant difference of density environments is found between the luminous HzRGs with L _1.4 GHz_ ∼ 1026.5–27.0 W Hz–1 and the g-dropout galaxies. The HzRGs are found to occupy more massive halos than g-dropout galaxies through a cross-correlation between the HzRGs and g-dropout galaxies. This trend is more pronounced in the faint HzRGs. These results are consistent with a scenario where HzRGs get older and more massive as the radio luminosity decreases. The HzRGs are expected to trace the progenitors of Local Cluster halos from their calculated halo mass. In addition, we find that surrounding galaxies tend to distribute along the radio jet major axis of the HzRGs at angular distances of <=500 physical kpc. Our findings imply the onset of the filamentary structures around the HzRGs at z ∼ 4.

Abstract Copyright: © 2022. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Radio galaxies - Active galaxies - High-redshift galaxies - Lyman-break galaxies - Protoclusters

Simbad objects: 25

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Number of rows : 25
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 FIRST J020343.8-055556 QSO 02 03 43.792 -05 55 56.26           ~ 1 0
2 HSCS J020612.23-031615.2 rG 02 06 12.23 -03 16 15.2           ~ 1 0
3 SDSS J020630.49-032847.0 QSO 02 06 30.490 -03 28 47.07           ~ 9 0
4 NVSS J021353-045817 rG 02 13 53.669 -04 58 17.66           ~ 1 0
5 NVSS J021803-053824 rG 02 18 03.4 -05 38 25   26.1566 24.5809 24.5523   ~ 8 1
6 FIRST J021952.7-053249 rG 02 19 52.722 -05 32 49.47           ~ 2 1
7 SDSS J022320.70-031824.2 QSO 02 23 20.7031926864 -03 18 24.276207312   21.51   18.82   ~ 17 1
8 FIRST J022454.9-032905 QSO 02 24 54.926 -03 29 05.30           ~ 2 1
9 HSCS J023030.67-055440.8 rG 02 30 30.67 -05 54 40.8           ~ 1 0
10 HSCS J023032.41-040302.3 rG 02 30 32.41 -04 03 02.3           ~ 1 0
11 HSCS J023303.17-051100.9 rG 02 33 03.17 -05 11 00.9           ~ 1 0
12 HSCS J115038.16-015028.6 rG 11 50 38.16 -01 50 28.6           ~ 1 0
13 NVSS J115208-005742 rG 11 52 08.925 -00 57 36.36           ~ 1 0
14 HSCS J120258.99-001543.8 rG 12 02 58.99 -00 15 43.8           ~ 1 0
15 HSCS J120343.34+000313.1 rG 12 03 43.34 +00 03 13.1           ~ 1 0
16 NVSS J142815-002139 rG 14 28 15.6096 -00 21 31.060           ~ 2 0
17 NVSS J142949-003617 rG 14 29 49.663 -00 36 16.68           ~ 2 1
18 HSCS J143618.45+004309.1 rG 14 36 18.45 +00 43 09.1           ~ 1 0
19 SDSS J143634.49+005111.9 QSO 14 36 34.499 +00 51 11.97           ~ 11 0
20 NVSS J144422+000704 rG 14 44 22.801 +00 07 00.11           ~ 2 1
21 HSCS J162404.42+435624.2 rG 16 24 04.42 +43 56 24.2           ~ 1 0
22 HSCS J162713.96+433258.0 rG 16 27 13.96 +43 32 58.0           ~ 1 0
23 HSCS J221828.11+004301.6 rG 22 18 28.11 +00 43 01.6           ~ 1 0
24 HSCS J221959.44+013124.2 rG 22 19 59.44 +01 31 24.2           ~ 1 0
25 HSCS J222252.11+003806.1 rG 22 22 52.11 +00 38 06.1           ~ 1 0

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