Gravitational Interactions in Poor Galaxy Groups
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View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CERN Document Server Gravitational Interactions in Poor Galaxy Groups David S. Davis1 and William C. Keel2 Department of Physics and Astronomy, The University of Alabama, 206 Gallalee Hall, Tuscaloosa AL 35487 John S. Mulchaey The Observatories of the Carnegie Institution of Washington, 813 Santa Barbara St., Pasadena CA 91101-1292 and Patricia A. Henning Department of Physics and Astronomy, The University of New Mexico, 800 Yale Blvd., NE, Albuquerque, NM 87131 ABSTRACT We report the results of the spatial analysis of deep ROSAT HRI ob- servations, optical imaging and spectroscopy, and high–resolution VLA H I and continuum imaging of NGC 1961 and NGC 2276. These spirals were selected as showing some previous evidence for interaction with a surrounding (hot) diffuse medium. Our results favor most aspects of these galaxies as being shaped by gravitational interactions with companions, rather than the asymmetric pressure from motion through an external medium. The old stars follow the asymmetric structures of young stars and ionized gas, which suggests a tidal origin for the lopsided appearance of these galaxies. In NGC 2276, the H I and star-forming regions are strongly concentrated along 1Present address: MIT Center for Space Research, Building 37-662B, Cambridge, MA 02139-4307 2Visiting astronomer, Kitt Peak National Observatory, National Optical Astronomy Observatories, operated by AURA, Inc., under cooperative agreement with the National Science Foundation. 1 the western edge of the disk. In this case, the ROSAT HRI detects the brightest star-forming regions as well as the diffuse disk emission, the most distant galaxy with such a detection. An asymmetric ionization gradient in the H II regions suggests radial movement of gas, which might have occurred in either tidal or wind scenarios. The X-ray emission from NGC 1961 is dominated by a point source near the nucleus of the galaxy but extended emission is seen out to a radius of ∼ 0.08. Previous studies of the enrichment of the intragroup medium in the NGC 2300 group indicates that stripping may be important in this sys- tem, but the density of the IGM is much too tenuous to effectively strip the gas from the galaxy. However, we propose that gravitational in- teractions in the group environment may enhance stripping. During a gravitational encounter the disk of the spiral galaxy may be warped, making ram pressure stripping more efficient than in a quiescent disk. Subject headings: interstellar medium - X-rays: galaxies - galaxies: in- dividual NGC 1961 - galaxies: individual NGC 2276 2 1. Introduction fuse medium. Confirmation of this process would be important in suggesting a new arena The discovery of hot gas in clusters of for environmental influences outside of rich galaxies presented the possibility that inter- clusters. actions between a galaxy and its environment We report here new multi-wavelength ob- could influence its evolution. A galaxy’s mo- servations of two of the strongest candidates tion through the cluster gas may play a role for such interactions, NGC 1961 (Arp 184) in the segregation of elliptical and S0 galax- and NGC 2276 (Arp 25 and 114), analyzed ies from gas rich spirals by stripping of the with the aim of distinguishing the gravita- interstellar medium. Evidence that stripping tional effects of surrounding galaxies from hy- does occur in clusters is strongest in the case drodynamic effects of surrounding gas. We of Virgo, where the spiral galaxies near the trace the young and old stellar components as cluster center show a pronounced HI deficit well as ionized, neutral, and X-ray gas, to dis- associated with truncation and asymmetry of tinguish the response to tidal perturbations, the H I disks (Cayatte et al. 1990) which is at- which is to first order similar for stars and tributed to the hot cluster medium stripping gas, from the effects of a gaseous disturbance, HI gas from the galaxies. An extreme case inconsequential for old stars but manifest in may be found in NGC 5291 on the outskirts low-density gas tracers. of the IC 4329 cluster, where a large H I mass is found outside the optical galaxy and sys- These galaxies were selected as showing the tematically offset outwards from the cluster most likely signatures of sweeping by a hot ex- core, with intense star formation seen along ternal medium based on radio and optical ev- the “upstream” sides of H I clumps (Long- idence. Radio studies of bright spiral galaxies more et al. 1979, Malphrus et al. 1995). (Condon 1983; Condon et al. 1990) identi- There is evidence that this process also oc- fied a population of spiral galaxies with ex- curs for the hot gas seen in elliptical galaxies. traordinarily strong disk emission at centime- The X-ray plume from M86 is thought to be ter wavelengths. Optical work shows that this due to stripping as the elliptical plunges into is invariably linked to strong disk star for- the hot cluster gas (Forman Jones & Tucker mation, and often to interactions. The link 1985; Irwin & Sarizan 1996). The discovery to galaxy interactions is hardly unusual given of diffuse gas in poor groups (e.g. Mulchaey the abundant evidence that tidal forces can et al. 1993; Ponman & Bertram 1993) raised induce star formation, but some of the most the possibility that gas stripping could also striking examples have no plausible nearby occur in environments much less dense than companion. In two of the best studied spi- that of clusters. Since the group environment rals of this kind (NGC 1961 and NGC 2276), is less dense that the cluster environment and there is no obviously interacting nearby com- the velocity dispersions of groups are also less, panion and yet a strong asymmetry appears the effects of stripping should be more subtle in the optical and radio maps, suggesting than those seen in clusters. Nonetheless, op- that these galaxies may be interacting with tical and radio work has suggested that some the intragroup medium rather than another spirals in rather sparse environments show ev- galaxy. However, the galaxy environments of idence of interaction with a surrounding dif- such groups have made the interpretation am- 3 biguous in each case; there is usually a bright last 40 years, three of which were in the ap- galaxy close enough in projection to poten- parent “leading edge” and close to but not tially act as a tidal perturber, perhaps several necessarily directly associated with bright H crossing times ago so that the interaction is II regions (Iskudarian & Shakhbazian 1967, not immediately apparent. Shakhbazian 1968, Iskudarian 1968, Treffers NGC 1961 is also notable for its exception- 1993). While the elliptical NGC 2300 and ally large linear size among spirals (Rubin, the spiral NGC 2276 form a relatively iso- Roberts & Ford 1979 ; Romanishin 1983). lated pair according to position-driven algo- Rubin et al. find that the optical rotation rithms, they are rather far apart (≈ 150 kpc −1 −1 curve implies an encircled mass above 1012 for H0 =50kms Mpc ), which at first glance makes a tidal origin for the asymmet- M , and mention a significant role for non- circular motions. This large mass is confirmed ric disk unlikely. The galaxy gained height- by Shostak et al. (1982) who map the galaxy ened interest with the discovery of a diffuse using 21 cm spectral imaging. The rotation X-ray medium in its surroundings, the NGC curve derived from the channel maps is well 2300 group (Mulchaey et al. 1993). organized and implies a mass of ∼ 1.5 × 1012 The theme of our analysis is to ask whether M . The integrated H I map shows that the we can distinguish the effects of gravitational bulk of the neutral hydrogen emission is coin- interactions involving neighboring galaxies from cident with the optical galaxy, but the H I is those of ram pressure driven by a surround- also extended to the NW. This extension con- ing diffuse medium, and if so whether there tains ≈10% of the total H I mass. Faint spiral is any strong evidence that ram pressure is arms are seen in the optical image coincident responsible for the peculiar features of these with the H I extension. Opposite the H I ex- galaxies. Both galaxies are members of poor tension, on the SW side of the galaxy, the H groups (Maia, da Costa & Latham 1986) so I distribution is sharply truncated. This H I that their distorted morphologies might be in- morphology leads Shostak et al. (1982) to in- terpreted as evidence for a recent interaction terpret this as stripping of the H I by the hot with another galaxy in each group. intergalactic medium. They noted rough co- incidence of diffuse X-ray structure in an Ein- 2. Observations stein IPC image with an extended H I feature, and interpreted this as evidence of the hot 2.1. ROSAT X-ray Observations stripping medium. However, ROSAT PSPC NGC 1961 and NGC 2276 were observed observations do not confirm the presence of by the ROSAT PSPC and the HRI. The such a hot cloud (Mulchaey et al. 1996). combination of these two instruments allows NGC 2276 is a very luminous Sc I spiral, the spectral and spatial properties of the X- in the NGC 2300 poor group. This is the ray emission for the galaxies in this group most Hα-luminous galaxy in the Kennicutt to be determined. The useful HRI exposure and Kent (1983) survey, and is remarkable for NGC 1961 is almost 83 ksec and that for not only for its disturbed morphology but for NGC 2276 is about 74 ksec.