A hard X-ray view of luminous and ultra-luminous infrared galaxies in GOALS – I. AGN obscuration along the merger sequence

Author:

Ricci C12ORCID,Privon G C3ORCID,Pfeifle R W4,Armus L5,Iwasawa K67,Torres-Albà N8,Satyapal S4,Bauer F E91011,Treister E9,Ho L C212,Aalto S13,Arévalo P14,Barcos-Muñoz L3,Charmandaris V1516,Diaz-Santos T1516,Evans A S173,Gao T18,Inami H19,Koss M J20ORCID,Lansbury G21ORCID,Linden S T22,Medling A2324ORCID,Sanders D B25,Song Y17,Stern D26,U V27,Ueda Y28,Yamada S28

Affiliation:

1. Núcleo de Astronomía de la Facultad de Ingeniería, Universidad Diego Portales, Av. Ejército Libertador 441, Santiago 22, Chile

2. Kavli Institute for Astronomy and Astrophysics, Peking University, Beijing 100871, China

3. National Radio Astronomy Observatory, 520 Edgemont Road, Charlottesville, VA 22903, USA

4. Department of Physics & Astronomy, George Mason University, MS 3F3, 4400 University Drive, Fairfax, VA 22030, USA

5. IPAC, California Institute of Technology, 1200 E. California Boulevard, Pasadena, CA 91125, USA

6. Institut de Ciències del Cosmos, Universitat de Barcelona, IEEC-UB, Martí i Franquès, 1, E-08028 Barcelona, Spain

7. ICREA, Pg. Lluís Companys, 23, E-08010 Barcelona, Spain

8. Kinard Laboratory of Physics, Clemson University, Clemson, SC 29634, USA

9. Instituto de Astrofísica and Centro de Astroingeniería, Facultad de Física, Pontificia Universidad Católica de Chile, Casilla 306, Santiago 22, 8970117, Chile

10. Millennium Institute of Astrophysics, Nuncio Monseor Stero Sanz 100, Providencia, Santiago 8010000, Chile

11. Space Science Institute, 4750 Walnut Street, Suite 205, Boulder, CO 80301, USA

12. Department of Astronomy, School of Physics, Peking University, Beijing 100871, China

13. Department of Space, Earth and Environment, Chalmers University of Technology, Onsala Space Observatory, SE-439 92 Onsala, Sweden

14. Instituto de Física y Astronomía, Facultad de Ciencias, Universidad de Valparaíso, Gran Bretana N1111, Playa Ancha, Valparaíso, 2340000, Chile

15. Department of Physics, University of Crete, Heraklion GR-71003, Greece

16. Institute of Astrophysics, Foundation for Research and Technology – Hellas, Heraklion GR-70013, Greece

17. Department of Astronomy, University of Virginia, Charlottesville, VA 22904, USA

18. Department of Astronomy, Beijing Normal University, Beijing 100875, China

19. Hiroshima Astrophysical Science Center, Hiroshima University, 1-3-1 Kagamiyama, Higashi-Hiroshima, Hiroshima 739-8526, Japan

20. Eureka Scientific, 2452 Delmer Street Suite 100, Oakland, CA 94602-3017, USA

21. European Southern Observatory, Karl-Schwarzschild-Strasse 2, D-85748 Garching, Germany

22. Department of Astronomy, University of Massachusetts at Amherst, Amherst, MA 01003, USA

23. Ritter Astrophysical Research Center, University of Toledo, Toledo, OH 43606, USA

24. ARC Centre of Excellence for All Sky Astrophysics in 3 Dimensions (ASTRO 3D)

25. Institute for Astronomy, University of Hawaii, 2680 Woodlawn Drive, Honolulu, HI 96822, USA

26. Jet Propulsion Laboratory, California Institute of Technology, 4800 Oak Grove Drive, MS 169-224, Pasadena, CA 91109, USA

27. Department of Physics and Astronomy, University of California, 4129 Frederick Reines Hall, Irvine, CA 92697, USA

28. Department of Astronomy, Kyoto University, Kitashirakawa-Oiwake-cho, Sakyo-ku, Kyoto 606-8502, Japan

Abstract

ABSTRACT The merger of two or more galaxies can enhance the inflow of material from galactic scales into the close environments of active galactic nuclei (AGNs), obscuring and feeding the supermassive black hole (SMBH). Both recent simulations and observations of AGN in mergers have confirmed that mergers are related to strong nuclear obscuration. However, it is still unclear how AGN obscuration evolves in the last phases of the merger process. We study a sample of 60 luminous and ultra-luminous IR galaxies (U/LIRGs) from the GOALS sample observed by NuSTAR. We find that the fraction of AGNs that are Compton thick (CT; $N_{\rm H}\ge 10^{24}\rm \, cm^{-2}$) peaks at $74_{-19}^{+14}{{\ \rm per\ cent}}$ at a late merger stage, prior to coalescence, when the nuclei have projected separations (dsep) of 0.4–6 kpc. A similar peak is also observed in the median NH [$(1.6\pm 0.5)\times 10^{24}\rm \, cm^{-2}$]. The vast majority ($85^{+7}_{-9}{{\ \rm per\ cent}}$) of the AGNs in the final merger stages (dsep ≲ 10 kpc) are heavily obscured ($N_{\rm H}\ge 10^{23}\rm \, cm^{-2}$), and the median NH of the accreting SMBHs in our sample is systematically higher than that of local hard X-ray-selected AGN, regardless of the merger stage. This implies that these objects have very obscured nuclear environments, with the $N_{\rm H}\ge 10^{23}\rm \, cm^{-2}$ gas almost completely covering the AGN in late mergers. CT AGNs tend to have systematically higher absorption-corrected X-ray luminosities than less obscured sources. This could either be due to an evolutionary effect, with more obscured sources accreting more rapidly because they have more gas available in their surroundings, or to a selection bias. The latter scenario would imply that we are still missing a large fraction of heavily obscured, lower luminosity ($L_{2-10}\lesssim 10^{43}\rm \, erg\, s^{-1}$) AGNs in U/LIRGs.

Funder

National Key Research and Development Program of China

National Science Foundation of China

CATA

FONDECYT

NASA

MICINN

ICCUB

JSPS

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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