Abstract:We report an early science discovery of the 12 CO(1-0) emission line in the collisional ring galaxy, VII Zw466, using the Redshift Search Receiver instrument on the Large Millimeter Telescope Alfonso Serrano.The apparent molecular-to-atomic gas ratio either places the ISM of VII Zw466 in the HI-dominated regime or implies a large quantity of CO-dark molecular gas, given its high star formation rate. The molecular gas densities and star formation rate densities of VII Zw466 are consistent with the standard Kenn… Show more
“…• Ring galaxies live in massive groups (Mhalo ∼ 10 13 M ) that are preferentially more concentrated than groups without ring galaxies at fixed halo mass. This is in agreement with the observations, in which ring galaxies are located within galaxy groups and have at least one companion galaxy (Higdon & Wallin 1997;Higdon 1995;Romano et al 2008;Conn et al 2016;Wong et al 2017;Elagali et al 2018).…”
Section: Discussionsupporting
confidence: 93%
“…This is different than the result presented in Figure 12, where the star formation rate surface density in ring galaxies is higher in the outer radii (r > 20 kpc) in comparison with the star-forming galaxy sample implying that the abundance of cold gas in the ring should be relatively normal. To examine the photodissociation hypothesis suggested in Higdon et al (2015); Wong et al (2017), we need to follow the formation and the evolution of the molecular hydrogen. This requires a detailed description of the ISM and the photoionisation effects of local sources on the H2 gas, which is not currently feasible in simulations with a boxsize as large as EAGLE and only prescribed in zoom-in simulations, see for example Hopkins et al (2014Hopkins et al ( , 2017.…”
Section: The Ism Of Eagle Ring Galaxiesmentioning
confidence: 99%
“…Mihos & Hernquist (1994) and Mapelli et al (2008a) showed in their simulations that it takes around 100 Myr after the collision to develop the ring in the disk of these galaxies and that the ring morphology remains visible for ∼ 0.5 Gyr, which is very short compared to the Hubble timescale. Since the formation mechanisms of collisional ring galaxies are very well constrained via simulations, they can be considered as galaxy-scale perturbation experiments that facilitate the study of extreme modes of interaction-triggered star formation and feedback processes (Higdon et al 2012(Higdon et al , 2015Wong et al 2017;Renaud et al 2018).…”
Section: Introductionmentioning
confidence: 99%
“…Further, observations of collisional ring galaxies suggests that these systems contain on average high amounts of HI gas in comparison with galaxies that have the same stellar mass (Elagali et al 2018), yet are H2 deficient (Higdon et al 2015;Wong et al 2017) especially at the outer rings where the atomic hydrogen surface density is the highest (e.g., in the Cartwheel galaxy ΣHI = 19 − 65 M pc −2 ; Higdon et al 2015). The reason behind this deficiency is not yet well understood, however Wong et al (2017) and Higdon et al (2015) hypothesise that the ISM in ring galaxies behaves differently as a result of the extreme conditions in, e.g., pressure, temperature and metallicity, induced by the drop-through collision.…”
We study the formation and evolution of ring galaxies in the Evolution and Assembly of GaLaxies and their Environments (EAGLE) simulations. We use the largest reference model Ref-L100N1504, a cubic cosmological volume of 100 comoving megaparsecs on a side, to identify and characterise these systems through cosmic time. The number density of ring galaxies in EAGLE is in broad agreement with the observations. The vast majority of ring galaxies identified in EAGLE (83 per cent) have an interaction origin, i.e., form when one or more companion galaxies drop-through a disk galaxy. The remainder (17 per cent) have very long-lived ring morphologies (> 2 Gyr) and host strong bars. Ring galaxies are HI rich galaxies, yet display inefficient star formation activity and tend to reside in the green valley particularly at z 0.5. This inefficiency is mainly due to the low pressure and metallicity of their interstellar medium (ISM) compared with the ISM of similar star-forming galaxies. We find that the interaction(s) is responsible for decreasing the ISM pressure by causing the ISM gas to flow from the inner regions to the outer disk, where the ring feature forms. At a fixed radius, the star formation efficiency of ring galaxies is indistinguishable from their star-forming counterparts, and thus the main reason for their integrated lower efficiency is the different gas surface density profiles. Since galaxy morphologies are not used to tune the parameters in hydrodynamical simulations, the experiment performed here demonstrates the success of the current numerical models in EAGLE.
“…• Ring galaxies live in massive groups (Mhalo ∼ 10 13 M ) that are preferentially more concentrated than groups without ring galaxies at fixed halo mass. This is in agreement with the observations, in which ring galaxies are located within galaxy groups and have at least one companion galaxy (Higdon & Wallin 1997;Higdon 1995;Romano et al 2008;Conn et al 2016;Wong et al 2017;Elagali et al 2018).…”
Section: Discussionsupporting
confidence: 93%
“…This is different than the result presented in Figure 12, where the star formation rate surface density in ring galaxies is higher in the outer radii (r > 20 kpc) in comparison with the star-forming galaxy sample implying that the abundance of cold gas in the ring should be relatively normal. To examine the photodissociation hypothesis suggested in Higdon et al (2015); Wong et al (2017), we need to follow the formation and the evolution of the molecular hydrogen. This requires a detailed description of the ISM and the photoionisation effects of local sources on the H2 gas, which is not currently feasible in simulations with a boxsize as large as EAGLE and only prescribed in zoom-in simulations, see for example Hopkins et al (2014Hopkins et al ( , 2017.…”
Section: The Ism Of Eagle Ring Galaxiesmentioning
confidence: 99%
“…Mihos & Hernquist (1994) and Mapelli et al (2008a) showed in their simulations that it takes around 100 Myr after the collision to develop the ring in the disk of these galaxies and that the ring morphology remains visible for ∼ 0.5 Gyr, which is very short compared to the Hubble timescale. Since the formation mechanisms of collisional ring galaxies are very well constrained via simulations, they can be considered as galaxy-scale perturbation experiments that facilitate the study of extreme modes of interaction-triggered star formation and feedback processes (Higdon et al 2012(Higdon et al , 2015Wong et al 2017;Renaud et al 2018).…”
Section: Introductionmentioning
confidence: 99%
“…Further, observations of collisional ring galaxies suggests that these systems contain on average high amounts of HI gas in comparison with galaxies that have the same stellar mass (Elagali et al 2018), yet are H2 deficient (Higdon et al 2015;Wong et al 2017) especially at the outer rings where the atomic hydrogen surface density is the highest (e.g., in the Cartwheel galaxy ΣHI = 19 − 65 M pc −2 ; Higdon et al 2015). The reason behind this deficiency is not yet well understood, however Wong et al (2017) and Higdon et al (2015) hypothesise that the ISM in ring galaxies behaves differently as a result of the extreme conditions in, e.g., pressure, temperature and metallicity, induced by the drop-through collision.…”
We study the formation and evolution of ring galaxies in the Evolution and Assembly of GaLaxies and their Environments (EAGLE) simulations. We use the largest reference model Ref-L100N1504, a cubic cosmological volume of 100 comoving megaparsecs on a side, to identify and characterise these systems through cosmic time. The number density of ring galaxies in EAGLE is in broad agreement with the observations. The vast majority of ring galaxies identified in EAGLE (83 per cent) have an interaction origin, i.e., form when one or more companion galaxies drop-through a disk galaxy. The remainder (17 per cent) have very long-lived ring morphologies (> 2 Gyr) and host strong bars. Ring galaxies are HI rich galaxies, yet display inefficient star formation activity and tend to reside in the green valley particularly at z 0.5. This inefficiency is mainly due to the low pressure and metallicity of their interstellar medium (ISM) compared with the ISM of similar star-forming galaxies. We find that the interaction(s) is responsible for decreasing the ISM pressure by causing the ISM gas to flow from the inner regions to the outer disk, where the ring feature forms. At a fixed radius, the star formation efficiency of ring galaxies is indistinguishable from their star-forming counterparts, and thus the main reason for their integrated lower efficiency is the different gas surface density profiles. Since galaxy morphologies are not used to tune the parameters in hydrodynamical simulations, the experiment performed here demonstrates the success of the current numerical models in EAGLE.
“…The RSR data was reduced using the D package (Data REduction and Analysis Methods in PYthon, written by G. Narayanan) and following the standard procedure (e.g. Yun et al 2015;Cybulski et al 2016;Wong et al 2017). A careful visual inspection of individual scans was performed to identify and remove those with the noisiest spectral features.…”
We present LMT/AzTEC 1.1mm observations of ∼100 luminous high-redshift dusty star-forming galaxy candidates from the ∼600 sq.deg Herschel-ATLAS survey, selected on the basis of their SPIRE red far-infrared colours and with $S_{500\, \mu \rm m}=35-80$ mJy. With an effective θFWHM ≈ 9.5 arcsec angular resolution, our observations reveal that at least 9 per cent of the targets break into multiple systems with SNR ≥4 members. The fraction of multiple systems increases to ∼23 per cent (or more) if some non-detected targets are considered multiples, as suggested by the data. Combining the new AzTEC and deblended Herschel photometry we derive photometric redshifts, IR luminosities, and star formation rates. While the median redshifts of the multiple and single systems are similar (zmed ≈ 3.6), the redshift distribution of the latter is skewed towards higher redshifts. Of the AzTEC sources ∼85 per cent lie at zphot > 3 while ∼33 per cent are at zphot > 4. This corresponds to a lower limit on the space density of ultra-red sources at 4 < z < 6 of ∼3 × 10−7 Mpc−3 with a contribution to the obscured star-formation of ≳ 8 × 10−4 M⊙ yr−1 Mpc−3. Some of the multiple systems have members with photometric redshifts consistent among them suggesting possible physical associations. Given their angular separations, these systems are most likely galaxy over-densities and/or early-stage pre-coalescence mergers. Finally, we present 3mm LMT/RSR spectroscopic redshifts of six red-Herschel galaxies at zspec = 3.85 − 6.03, two of them (at z ∼ 4.7) representing new redshift confirmations. Here we release the AzTEC and deblended Herschel photometry as well as catalogues of the most promising interacting systems and z > 4 galaxies.
The Widefield ASKAP L-band Legacy All-sky Blind surveY (WALLABY) is a next-generation survey of neutral hydrogen (H I) in the Local Universe. It uses the widefield, high-resolution capability of the Australian Square Kilometer Array Pathfinder (ASKAP), a radio interferometer consisting of 36 × 12-m dishes equipped with Phased-Array Feeds (PAFs), located in an extremely radioquiet zone in Western Australia. WALLABY aims to survey three-quarters of the sky (−90 • < δ < +30 • ) to a redshift of z 0.26, and generate spectral line image cubes at ∼30 arcsec resolution and ∼1.6 mJy beam −1 per 4 km s −1 channel sensitivity. ASKAP's instantaneous field of view at 1.4 GHz, delivered by the PAF's 36 beams, is about 30 sq deg. At an integrated signal-to-noise ratio of five, WALLABY is expected to detect around half a million galaxies with a mean redshift of z ∼ 0.05 (∼200 Mpc). The scientific goals of WALLABY include: (a) a census of gas-rich galaxies in the vicinity of the Local Group; (b) a study of the H I properties of galaxies, groups and clusters, in particular the influence of the environment on galaxy evolution; and (c) the refinement of cosmological parameters using the spatial and redshift distribution of low-bias gas-rich galaxies. For context we provide an overview of recent and planned large-scale H I surveys. Combined with existing and new multi-wavelength sky surveys, WALLABY will enable an exciting new generation of panchromatic studies of the Local Universe. -First results from the WALLABY pilot survey are revealed, with initial data products publicly available in the CSIRO ASKAP Science Data Archive (CASDA).
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