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ALABAMA University Libraries THE UNIVERSITY OF ALABAMA University Libraries The Spiral Host Galaxy of the Double Radio Source 0313-192 William C. Keel – University of Alabama Raymond E. White III – University of Alabama Frazer N. Owen – National Radio Astronomy Observatory Michael J. Ledlow – Gemini Observatory, Southern Operations Center, Chile Deposited 09/17/2018 Citation of published version: Keel, W., White III, R., Owen, F., Ledlow, M. (2006): The Spiral Host Galaxy of the Double Radio Source 0313-192. The Astronomical Journal, 132(6). DOI: 10.1086/508340 © 2006. The American Astronomical Society. All rights reserved. Printed in U.S.A. The Astronomical Journal, 132:2233Y2242, 2006 December # 2006. The American Astronomical Society. All rights reserved. Printed in U.S.A. THE SPIRAL HOST GALAXY OF THE DOUBLE RADIO SOURCE 0313À1921 William C. Keel and Raymond E. White III Department of Physics and Astronomy, University of Alabama, Box 870324, Tuscaloosa, AL 35487; [email protected], [email protected] Frazer N. Owen National Radio Astronomy Observatory,2 P.O. Box O, Socorro, NM 87801 and Michael J. Ledlow3 Gemini Observatory, Southern Operations Center, AURA, Inc., Casilla 603, La Serena, Chile Received 2006 June 7; accepted 2006 August 2 ABSTRACT We present new Hubble Space Telescope (HST ), Gemini South, and Chandra observations of the radio galaxy 0313À192, which hosts a 350 kpc double source and jets, even though previous data have suggested that it is a spiral galaxy. We measure the bulge scale and the luminosity, radial, and vertical profiles of disk starlight and consider the distributions of H ii regions and absorbing dust. In each case the HST data confirm its classification as an edge-on spiral galaxy, the only such system known to produce such an extended radio source of this kind. The Gemini near-IR images and Chandra spectral fit reveal a strongly obscured central active galactic nucleus (AGN), seen through the entire interstellar medium path length of the disk and showing X-ray evidence of additional absorption from warm or dense material close to the central object. We consider several possible mechanisms for producing such a rare combination of AGN and host properties, some combination of which may be at work. These include an unusually luminous ; 8 bulge (suggesting a black hole of mass 8 10 M ), the orientation of the jets near the pole of the gas-rich disk, and some evidence of a weak gravitational interaction that has warped the disk and could have enhanced fueling of the central engine. We detect an X-ray counterpart of the kiloparsec-scale radio jet emerging to the south; jet/ counterjet limits on both radio and X-ray regimes allow them to be symmetric if seen more than 15 from the plane of the sky, still consistent with the jet axes being within 30 of the poles of the gas-rich galaxy disk. A linear or disklike emission-line structure is seen around the nucleus, inclined by 20 to the stellar disk but nearly per- pendicular to the jets; this may represent the aftermath of a galaxy encounter, in which gas is photoionized by a direct view of the nuclear continuum. Key words: galaxies: active — galaxies: individual ([OL97] 0313À192) — galaxies: spiral 1. INTRODUCTION such feedback mechanisms as heating or wind sweeping. These factors have renewed interest in the connections between prop- The relationships between active galactic nuclei (AGNs) and erties of AGNs and their host systems. their host galaxies may be important not only for the evolution of Among the most durable systematic patterns between the oc- the AGNs but for the host galaxies themselves. Since dynami- currence of AGNs and the structure of surrounding galaxies has cal evidence supports the existence of massive black holes in nu- been the finding that large double radio sources occur only around merous galactic nuclei, and very general arguments suggest that elliptical galaxies or systems that plausibly would have been the active growth of such black holes by accretion is what we see as AGNs, the current demographics of such black holes must called elliptical galaxies until a recent external disturbance (in studies ranging from Matthews et al. [1964] to Heckman et al. result from the whole history of AGN episodes. Furthermore, [1986]). This correlation has figured in theoretical explanations some aspects of galaxy formation become easier to understand if AGN episodes regulate the properties of gas in galaxies via of large-scale jets and in understanding why such jets are as- sociated with extensive synchrotron lobes. There are a handful of nearby radio galaxies showing evidence for gas-rich disks, 1 Based on observations made with the NASA/ESA Hubble Space Telescope, generally in host galaxies so disturbed that these are well ex- obtained at the Space Telescope Science Institute, which is operated by the As- plained as captured material from major mergers; 3C 120 (Arp sociation of Universities for Research in Astronomy (AURA), Inc., under NASA 1975; Heckman & Balick 1979; Garcı´a-Lorenzo et al. 2005), contract NAS5-26555; made with the Chandra X-Ray Observatory; and obtained at 3C 293 (van Bruegel et al. 1984; Floyd et al. 2006), 3C 305 the Gemini Observatory, which is operated by AURA, Inc., under a cooperative (Heckman et al. 1982; Jackson et al. 2003), and 3C 285 (Roche agreement with the National Science Foundation (NSF) on behalf of the Gemini partnership: the NSF (United States), the Particle Physics and Astronomy Research & Eales 2000) are well-studied examples. In each of these the Council (United Kingdom), the National Research Council (Canada), CONICYT system is disturbed enough to leave its original galaxy type am- (Chile), the Australian Research Council (Australia), CNPq (Brazil), and CONICET biguous. While normal spiral galaxies with AGNs often have (Argentina). kiloparsec-scale radio jets, no previously reported case of a large- 2 The National Radio Astronomy Observatory is a facility of the National Science Foundation, operated under cooperative agreement by Associated Uni- scale double radio source associated with a spiral has withstood versities, Inc. detailed examination as regards both the host Hubble type and 3 Deceased 2004 June 5. its identification with the radio source. In contrast, the edge-on 2233 2234 KEEL ET AL. Vol. 132 galaxy associated with the radio source 0313À192 in the cluster us confidence that the radio source and galaxy are indeed the same Abell 428 obviously has a significant stellar disk (Ledlow et al. object. For visual reference Figure 1 shows a composite VLA 1998) and a prominent dust lane of the kind usually associated A-configuration image, in which the outer regions are as seen at with spiral galaxies. Here we report Hubble Space Telescope (HST ) 1.4 GHz and the inner jet is from an 8.5 GHz observation, super- Advanced Camera for Surveys (ACS), Gemini South (Gemini-S), posed on the color rendition of the ACS imagery. The prominent and Chandra ACIS images of this galaxy, resulting in quanti- grand-design spiral to the northwest is not a good candidate for a tative photometric evidence that the galaxy is in fact a spiral and physical companion, lying at cz ¼ 15;225 Æ 87 km sÀ1 (Ledlow pointing to peculiar features of its gas distribution that may shed et al. 2001), as opposed to a redshift of cz ¼ 20;143 Æ 66 for light on how this rare combination of galaxy and nuclear activity 0313À192 itself. A combination of sparse galaxy population happened. and large redshift spread led Ledlow et al. to suggest that Abell As shown by Ledlow et al. (2001), the radio structure of 428 is more like a filament seen end-on, rich in small groups, than 0313À192 includes a nuclear source, a nuclear jet toward the a cluster environment. southern lobe of about the same extent as that in M87 but sev- Figure 2 shows the smaller field view in the continuum as eral times less powerful, larger twin jets directed at projected a composite color display. This view emphasizes the intricate angles of about 70 to the galaxy disk plane, and edge-darkened structure in the disk dust lane and the blue star-forming regions lobes spanning roughly 28000 (about 360 kpc at z ¼ 0:067 for seen around the disk warp. À1 À1 H0 ¼ 70 km s Mpc ). This structure would typically fall Continuum-subtracted emission-line images were constructed into Fanaroff-Riley type I (FR I), a classification in which it would using the broadband images as continuum, with the correction for lie near the middle of the power distribution (1024 WHzÀ1 at line radiation in these bands being small. The relative shifts be- 1400 MHz). Strong 21 cm H i absorption is detected against the tween broadband and narrowband images could be checked from 22 À2 central source at a column density NH > 10 cm , with the thedatathemselvesonlytotheÆ2 pixel level, since there are no limit set by its large optical depth and the resolution of the data bright unresolved sources in the region of useful LRF trans- (Ledlow et al. 2001). The H i absorption is also narrow in ve- mission; however, this should cause no particular problem in locity span (34 km sÀ1 FWHM), more characteristic of a line of the analysis, since we see no features with the positive/negative sight cutting radially through a large disk than one dominated pattern that would result from subtraction of an inappropriately by gas closer to the central mass. This large column density is com- shifted continuum. The scaling factors to account for the contin- parable to what we see toward Sgr A, supporting the idea that we uum included in the narrow bands were empirically determined are seeing a galaxy similar to our own viewed exactly edge-on.
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