2025ApJ...992...82H


Query : 2025ApJ...992...82H

2025ApJ...992...82H - Astrophys. J., 992, 82 (2025/October-2)

Magnetic Reconnection as a Potential Driver of X-Ray Variability in Active Galactic Nuclei.

HU C.-R., HUANG Y.-F., CUI L., ZHANG H., LI J.-T., JI L., GENG J.-J., AMAT O., XU F., DU C., ZHANG W.-L., ZOU Z.-C., DONG X.-F., DENG C., JIANG P. and LIAO J.

Abstract (from CDS):

We present a systematic analysis on the X-ray variability in 13 bright quasars at z > 4.5, combining recent Swift observations from 2021 to 2023 and archival multiepoch observations. Upper limits of the luminosity measurements were included in the analysis by using the Kaplan-Meier estimator method. It is found that the high-redshift quasars exhibit X-ray variability on both short-term (hours to days) and intermediate-term (weeks to months) timescales, with short-term variability dominating the overall variation. A linear correlation exists between the global mean (${\mu }_{{L}_{2-{\rm{10keV}}}}$) and standard deviation (${\sigma }_{{L}_{2-{\rm{10keV}}}}$) of X-ray luminosities, which is independent of the X-ray photon index and optical-to-X-ray spectral slope. The localized stochastic magnetic reconnection mechanism is strongly favored, which can naturally lead to a scale-invariant power-law energy distribution and satisfactorily explain the correlation. The σ-μ correlation parallels the well-documented rms-flux relation of low-redshift active galactic nuclei (AGNs), implying that the magnetic reconnection mechanism could drive short-timescale X-ray variability in both high- and low-redshift AGNs. The highest-redshift quasar in our sample, J142952+544717 (z = 6.18), shows a luminosity distribution extending to 1047 erg s–1 with a not conspicuous median luminosity. On the other hand, J143023+420436 (z = 4.7), which hosts the most relativistic jet among known high-redshift blazars, is dominated in the high-luminosity regime (1047 erg s–1), making it an ideal target for multiwavelength follow-up observations. J090630+693030 is found to have a rest-frame period of 182.46 days, and J143023+420436 has a period of 16.89 days; both could be explained by the global evolution of plasmoid chains, in which magnetic islands formed during reconnection may merge successively.

Abstract Copyright: © 2025. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): X-ray active galactic nuclei - X-ray quasars - Blazars - Astrostatistics - Supermassive black holes - Galaxy magnetic fields

Simbad objects: 13

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Number of rows : 13
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 [VV2006] J001115.2+144601 QSO 00 11 15.2339604624 +14 46 01.809704964   22.68 20.95     ~ 66 0
2 QSO J0131-0321 QSO 01 31 27.3474070344 -03 21 00.075737592           ~ 47 0
3 QSO J0324-2918 Bla 03 24 44.2954658256 -29 18 21.220152624     18.66 19.41   ~ 54 1
4 QSO J0355-3811 QSO 03 55 04.8756518568 -38 11 42.543056760     17.95     ~ 26 0
5 QSO J0747+1153 QSO 07 47 49.1748470112 +11 53 52.459993320           ~ 14 0
6 QSO J0906+6930 Bla 09 06 30.74874670 +69 30 30.8287169       21.65   ~ 96 1
7 QSO J0940+0526 QSO 09 40 04.801 +05 26 30.99           ~ 18 0
8 7C 102336.6+255813 QSO 10 26 23.62115 +25 42 59.4292   24.98 23.18     ~ 86 1
9 CFHQS J142952+544717 QSO 14 29 52.16880 +54 47 17.6964           ~ 68 0
10 7C 1428+4218 Bla 14 30 23.74163471 +42 04 36.4910561   24.43 22.04 20.2   ~ 157 1
11 [VV2006] J145147.1-151220 QSO 14 51 47.0510334120 -15 12 20.230974720     19.14     ~ 28 0
12 QSO J1548+3335 QSO 15 48 24.013 +33 35 00.11           ~ 19 1
13 QSO J2102+6015 Bla 21 02 40.21905211 +60 15 09.8365719           ~ 31 1

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