2022AJ....163..146S


Query : 2022AJ....163..146S

2022AJ....163..146S - Astron. J., 163, 146-146 (2022/April-0)

The Evolution of AGN Activity in Brightest Cluster Galaxies.

SOMBOONPANYAKUL T., McDONALD M., NOBLE A., AGUENA M., ALLAM S., AMON A., ANDRADE-OLIVEIRA F., BACON D., BAYLISS M.B., BERTIN E., BHARGAVA S., BROOKS D., BUCKLEY-GEER E., BURKE D.L., CALZADILLA M., CANNING R., CARNERO ROSELL A., CARRASCO KIND M., CARRETERO J., COSTANZI M., DA COSTA L.N., PEREIRA M.E.S., DE VICENTE J., DOEL P., EISENHARDT P., EVERETT S., EVRARD A.E., FERRERO I., FLAUGHER B., FLOYD B., GARCIA-BELLIDO J., GAZTANAGA E., GERDES D.W., GONZALEZ A., GRUEN D., GRUENDL R.A., GSCHWEND J., GUPTA N., GUTIERREZ G., HINTON S.R., HOLLOWOOD D.L., HONSCHEID K., HOYLE B., JAMES D.J., JELTEMA T., KHULLAR G., KIM K.J., KLEIN M., KUEHN K., LIMA M., MAIA M.A.G., MARSHALL J.L., MARTINI P., MELCHIOR P., MENANTEAU F., MIQUEL R., MOHR J.J., MORGAN R., OGANDO R.L.C., PALMESE A., PAZ-CHINCHON F., PIERES A., PLAZAS MALAGON A.A., REIL K., ROMER A.K., RUPPIN F., SANCHEZ E., SARO A., SCARPINE V., SCHUBNELL M., SERRANO S., SEVILLA-NOARBE I., SINGH P., SMITH M., SOARES-SANTOS M., STRAZZULLO V., SUCHYTA E., SWANSON M.E.C., TARLE G., TO C., TUCKER D.L. and WILKINSON R.D.

Abstract (from CDS):

We present the results of an analysis of Wide-field Infrared Survey Explorer (WISE) observations of the full 2500 deg2 South Pole Telescope (SPT)-Sunyaev-Zel'dovich cluster sample. We describe a process for identifying active galactic nuclei (AGN) in brightest cluster galaxies (BCGs) based on WISE mid-IR color and redshift. Applying this technique to the BCGs of the SPT-SZ sample, we calculate the AGN-hosting BCG fraction, which is defined as the fraction of BCGs hosting bright central AGNs over all possible BCGs. Assuming an evolving single-burst stellar population model, we find statistically significant evidence (>99.9%) for a mid-IR excess at high redshift compared to low redshift, suggesting that the fraction of AGN-hosting BCGs increases with redshift over the range of 0 < z < 1.3. The best-fit redshift trend of the AGN-hosting BCG fraction has the form (1 + z)4.1±1.0. These results are consistent with previous studies in galaxy clusters as well as as in field galaxies. One way to explain this result is that member galaxies at high redshift tend to have more cold gas. While BCGs in nearby galaxy clusters grow mostly by dry mergers with cluster members, leading to no increase in AGN activity, BCGs at high redshift could primarily merge with gas-rich satellites, providing fuel for feeding AGNs. If this observed increase in AGN activity is linked to gas-rich mergers rather than ICM cooling, we would expect to see an increase in scatter in the Pcav versus Lcool relation at z > 1. Last, this work confirms that the runaway cooling phase, as predicted by the classical cooling-flow model, in the Phoenix cluster is extremely rare and most BCGs have low (relative to Eddington) black hole accretion rates.

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

Journal keyword(s): Galaxy clusters - Galaxy evolution

Simbad objects: 12

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Number of rows : 12
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 ACT-CL J0106.2-5355 ClG 01 06 17.379 -53 55 37.95           ~ 6 0
2 ACT-CL J0106.4-5942 ClG 01 06 28.737 -59 43 12.54           ~ 25 0
3 ClG 0657-56 ClG 06 58 26.9 -55 58 21           ~ 1077 1
4 IRAS 09104+4109 Sy2 09 13 45.4951283928 +40 56 28.215343572   19.69 19.21     ~ 260 1
5 ACO 1656 ClG 12 59 44.40 +27 54 44.9           ~ 5141 2
6 ACO 1835 ClG 14 01 02.07 +02 52 43.2           ~ 727 1
7 LEDA 1900245 Bla 15 32 53.780 +30 20 59.41   19.1   15.7 17.819 ~ 155 1
8 7C 1821+6419 Sy1 18 21 57.2130271440 +64 20 36.221312076   14.23 14.24     ~ 632 1
9 [SMG2021] CHIPS J1911+4455 C?G 19 11 01.00 +44 55 20.0           ~ 7 0
10 ACT-CL J2146.5-4633 ClG 21 46 34.8 -46 32 56           ~ 36 0
11 ACT-CL J2341.2-5119 ClG 23 41 12.3 -51 19 43           ~ 52 0
12 ACT-CL J2344.7-4243 ClG 23 44 43.9 -42 43 11           ~ 229 0

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