Issue |
A&A
Volume 683, March 2024
|
|
---|---|---|
Article Number | A120 | |
Number of page(s) | 7 | |
Section | Extragalactic astronomy | |
DOI | https://doi.org/10.1051/0004-6361/202348146 | |
Published online | 13 March 2024 |
Active galactic nuclei and gravitational redshifts
1
Instituto de Astronomía Teórica y Experimental (IATE), CONICET – U. Nacional de Córdoba, X5000BGR Córdoba, Argentina
e-mail: nelson.padilla@unc.edu.ar
2
Instituto de Física, Universidade Federal da Bahia, 40210-340 Salvador, BA, Brazil
3
Observatório Nacional, 20921-400 Rio de Janeiro, RJ, Brazil
4
Institut de Física d’Altes Energies, The Barcelona Institute of Science and Technology, Campus UAB, 08193 Bellaterra, Barcelona, Spain
5
Observatorio Astronómico de Córdoba, Universidad Nacional de Córdoba, X5000BGR Córdoba, Argentina
Received:
3
October
2023
Accepted:
20
December
2023
Context. Gravitational redshift is a classical effect of General Relativity. It has been measured in stars, quasars, and clusters of galaxies.
Aims. We identify the signature of gravitational redshift in the emission lines of active galaxies that is caused by supermassive black holes and compare this signature to what is found for inactive galaxies.
Methods. Using the virial theorem, we estimated gravitational redshifts for quasars from the 14th data release (DR14) of the Sloan Digital Sky Survey (SDSS) and compared them with measured gravitational redshifts from the difference between the redshifts of emission lines of Sydney Australian Astronomical Observatory Multi-object Integral Field (SAMI) galaxies in the central and outer annuli of their integral field spectra.
Results. Firstly, from the full width at half maximum of Hβ lines of 57 Seyfert type I galaxies of the active galactic nucleus (AGN) Black Hole Mass Database, we derive a median gravitational redshift zg = 1.18 × 10−4. Expanding this analysis to 86 755 quasars from DR14 of SDSS, we have a median value zg = 1.52 × 10−4. Then, by comparing the redshifts of 34 lines measured in the central and outer regions of low-ionization nuclear emission-line region galaxies in the SAMI survey, we obtain zg = (0.68 ± 0.09)×10−4, which increases to zg = (1.0 ± 0.1)×10−4 for the Hα and Hβ lines. These numbers are compatible with central black holes of ∼109 solar masses and broad line regions of ∼1 pc. For non-AGN galaxies, the gravitational redshift is compatible with zero.
Key words: relativistic processes / galaxies: active / galaxies: Seyfert
Publisher note: The inappropriate sentences in the first paragraph of Section 2 (accidentally left inserted) were deleted on 27 September 2024.
© The Authors 2024
Open Access article, published by EDP Sciences, under the terms of the Creative Commons Attribution License (https://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
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