293 research outputs found

    A robust method for investigating galactic evolution in the submillimetre waveband: II the submillimetre background and source counts

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    This is the second of two papers describing a model of galactic evolution in the submillimetre waveband. The model incorporates a self-consistent treatment of the evolution of dust and stars, is normalized to the submillimetre properties of galaxies in the local universe, and can be used to make predictions for both disk and elliptical galaxies and for `closed-box', `inflow', and `outflow' models of galactic evolution. In Paper I we investigated whether it is possible to explain the extreme dust masses of high-redshift quasars and radio galaxies by galactic evolution. In this paper we use the model to make predictions of the submillimetre background and source counts. All our disk-galaxy models exceed at short wavelengths the submillimetre background recently measured by Puget et al. (1996). We also find that it is possible to fit the background over the entire wavelength range with a elliptical model but not with a disk model. We make source count predictions at 190 μ\mum for the ISOPHOT instrument on ISO and at 850 μ\mum for SCUBA. We show that the shape of the 850 μ\mu m source counts depends almost entirely on the mass spectrum of the radiating objects. Finally, we consider the limitations of the models. We find that one of the biggest uncertainties in the model is our lack of information about the submillimetre properties of nearby galaxies, in particular the lack of a direct measurement of the submillimetre luminosity function.Comment: 17 pages, 9 postscript figures, TEX, accepted by MNRA

    Non-steller light from high-redshift radiogalaxies

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    With the aid of a new IRCAM image of 3C356, researchers question the common assumption that radiosource-stimulated starbursts are responsible for the extended optical emission aligned with radio structures in high-redshift radiogalaxies. They propose an alternative model in which the radiation from a hidden luminous quasar is beamed along the radio axis and illuminates dense clumps of cool gas to produce both extended narrow emission line regions and, by Thomson scattering, extended optical continua. Simple observational tests of this model are possible and necessary if we are to continue to accept that the color, magnitude and shape evolution of radiogalaxies are controlled by the active evolution of stellar populations

    Morphology and Surface Brightness Evolution of z\sim1.1 Radio Galaxies

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    We use Kbandimagingtoinvestigatetheangularsizeandmorphologyof106Cradiogalaxies,atredshiftsK-band imaging to investigate the angular size and morphology of 10 6C radio galaxies, at redshifts 1\leq z\leq 1.4.Twoappeartobeundergoingmergers,anothercontainstwointensitypeaksalignedwiththeradiojets,whiletheothersevenappearconsistentwithbeingnormalellipticalsintheKband.Intrinsichalflightradiiareestimatedfromtheareasofeachradiogalaxyimageaboveaseriesofthresholds.The6Cgalaxyradiiarefoundtobesignificantlysmallerthanthoseofthemoreradioluminous3CRgalaxiesatsimilarredshifts.ThiswouldindicatethatthehighermeanKbandluminosityofthe3CRgalaxiesresultsfromadifferenceinthesizeofthehostgalaxies,andnotsolelyfromadifferenceinthepoweroftheactivenuclei.Thesizeluminosityrelationofthe. Two appear to be undergoing mergers, another contains two intensity peaks aligned with the radio jets, while the other seven appear consistent with being normal ellipticals in the K-band. Intrinsic half-light radii are estimated from the areas of each radio galaxy image above a series of thresholds. The 6C galaxy radii are found to be significantly smaller than those of the more radioluminous 3CR galaxies at similar redshifts. This would indicate that the higher mean K-band luminosity of the 3CR galaxies results from a difference in the size of the host galaxies, and not solely from a difference in the power of the active nuclei. The size-luminosity relation of the z\sim 1.16Cgalaxiesindicatesa1.01.8magenhancementoftherestframeRbandsurfacebrightnessrelativetoeitherlocalellipticalsofthesamesizeorFRIIradiogalaxiesat 6C galaxies indicates a 1.0--1.8 mag enhancement of the rest-frame R-band surface brightness relative to either local ellipticals of the same size or FRII radio galaxies at z<0.2.The3CRgalaxiesat. The 3CR galaxies at z\sim 1.1showacomparableenhancementinsurfacebrightness.Themeanradiusofthe6Cgalaxiessuggeststhattheyevolveintoellipticalsof show a comparable enhancement in surface brightness. The mean radius of the 6C galaxies suggests that they evolve into ellipticals of L\sim L^*luminosity,andisconsistentwiththeirlowredshiftcounterpartsbeingrelativelysmallFRIIgalaxies,afactor luminosity, and is consistent with their low redshift counterparts being relatively small FRII galaxies, a factor \sim 25lowerinradioluminosity,orsmallFRIgalaxiesafactorof lower in radio luminosity, or small FRI galaxies a factor of \sim 1000$ lower in radio luminosity. Hence the 6C radio galaxies may undergo at least as much optical and radio evolution as the 3CR galaxies.Comment: 17 pages, 7 postscript figures, TEX, submitted to MNRA

    The Clustering of K\sim 20 Galaxies on 17 Radio Galaxy Fields

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    We investigate the angular correlation function, ω(θ)\omega(\theta), of the galaxi es detected in the K-band on 17 fields (101.5 square arcmin in total), each containing a z1.1z\sim 1.1 radio galaxy. There is a significant detection of galaxy clustering at K20K\sim 20 limits, with an amplitude higher than expected from simple models which fit the faint galaxy clustering in the blue and red passbands, but consistent with a pure luminosity evolution model i f clustering is stable and early-type galaxies have a steeper correlation function than spirals. We do not detect a significant cross-correlation between the radio galaxies and the other galaxies on these fields, obtaining upper limits consistent with a mean clustering environment of Abell class 0 for z1.1z\sim 1.1 radio galaxies, similar to that observed for radio galaxies at z0.5z\sim 0.5. At K20K\leq 20, the number of galaxy-galaxy pairs of 2--3 arcsec separations exceeds the random expectation by a factor of 2.15±0.262.15\pm 0.26. This excess suggests at least a tripling of the local merger rate at z1z\sim 1.Comment: 13 pages, 3 tables, 7 postscript figures, TEX, submitted to MNRA

    The SCUBA Local Universe Galaxy Survey Optically-Selected Sample

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    We discuss the progress of the SCUBA Local Universe Galaxy Survey (SLUGS), the first large, statistical sub-mm survey of the local universe. Since our original survey of a sample of 104 IRAS-selected galaxies we have recently completed a sample of 78 Optically-Selected galaxies. Since SCUBA is sensitive to the large proportion of dust too cold to be detected by IRAS the addition of this optically-selected sample allows us for the first time to determine the amount of cold dust in galaxies of different Hubble types. We detect 6 ellipticals in the sample and find them to have dust masses in excess of 10^7 solar masses. We derive local sub-mm luminosity functions, both directly for the two samples, and by extrapolation from the IRAS PSCz, and find excellent agreement.Comment: 2 pages, 2 figures. In the proceedings of the conference: "Penetrating Bars through Masks of Cosmic Dust: The Hubble Tuning Fork Strikes a New Note", South Africa, June 2004 (Kluwer

    Evidence against a simple two-component model for the far-infrared emission from galaxies

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    Two of the first Infrared Astronomy Satellite (IRAS) results were that galaxies have a wide range of values for the ratio of 60 micron to 100 micron flux density (0.2 less than or equal to S sub 60/S sub 100 less than or equal to 1.0) and that this ratio is correlated with L sub fir, L sub b, L sub fir being the total far-infrared luminosity and L sub b being the luminosity at visible wavelengths (de Jong et al. 1984; Soifer et al. 1984). From these results arose the following simple model for the far-infrared emission from galaxies (de Jong et al. 1984), which has remained the standard model ever since. In this model, the far-infrared emission comes from two dust components: warm dust (T approx. equals 50 K) intermingled with, and heated by, young massive OB stars in molecular clouds and HII regions, and colder dust (T approx. equals 20 K) associated with the diffuse atomic hydrogen in the interstellar medium and heated by the general interstellar radiation field. As the number of young stars in a galaxy increases, S sub 60/S sub 100 increases, because there is a greater proportion of warm dust, and so does L sub fir/L sub b, because most of the radiation from the young stars is absorbed by the dust, leading to a swifter increase in far-infrared emission than in visible light. Although this model explains the basic IRAS results, it is inelegant. It uses two free parameters to fit two data (the 60 and 100 micron flux densities)-and there are now several observations that contradict it. Despite these major problems with the two-component model, it is not clear what should be put in its place. When considering possible models for the far-infrared emission from galaxies, the observational evidence for our own galaxy must be considered. Researchers suspect that the study by Boulanger and Perault (1988) of the far-infrared properties of the local interstellar medium may be particularly relevant. They showed that molecular clouds are leaky - that most of the light from OB stars in molecular clouds does not heat the dust in the clouds, but instead leaks out. The consequence of this is that that while most of the far-infrared emission from the solar neighborhood is from dust associated with diffuse HI, this dust is mostly heated by young stars

    The SCUBA Local Universe Galaxy Survey: Results from the Optically-Selected Sample

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    We present new results from the SCUBA Local Universe Galaxy Survey, the first large statistical submillimetre survey of the local Universe. Following our initial survey of a sample of 104 IRAS-selected galaxies we now present the results of a sample of 80 Optically-selected galaxies. Since SCUBA is sensitive to the large proportion of dust too cold to be detected by IRAS the addition of this Optically-selected sample allows us for the first time to determine the amount of cold dust in galaxies of different Hubble types. We detect 6 ellipticals in the sample and find them to have dust masses in excess of 10^7 solar masses. We derive local submillimetre Luminosity Functions and Dust Mass functions, both directly for the Optically-Selected SLUGS sample and by extrapolation from the IRAS PSCz survey, and find them to be well-fitted by Schechter functions. We find excellent agreement between the two LFs and DMFs and show that, whereas the slope of the IRAS-selected LF at lower luminosities was steeper than -2 (a submm "Olbers' Paradox"), as expected the PSCz-extrapolated LF flattens out at the low luminosity end.Comment: 2 pages, 4 figures. To be published in proceedings of the conference: "The Dusty and Molecular Universe - A Prelude to HERSCHEL and ALMA", Paris, October 2004 (ESA Publications

    Faint radio samples: the key to understanding radio galaxies

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    The large number of differences between high- and low-redshift radio galaxies have almost all been discovered by looking at the bright 3C sample of radio sources. This has the disadvantage that the strong correlation between radio luminosity and redshift within a single sample makes it impossible to be determine whether these differences are the result of cosmic evolution or whether they are simply the result of source properties depending on radio luminosity. The solution to this problem is to compare the properties of sources in faint samples with those of the 3C sources. I and collaborators have recently removed the degeneracy between redshift and radio luminosity by comparing the 3C sample to the recently completed 6C and 7C samples. In this paper I concentrate on what our study has revealed about the host galaxies of radio sources. At low redshift, radio galaxies are giant ellipticals with absolute magnitude being independent of radio luminosity over a range of 104\rm 10^4 in radio luminosity. At z1z \sim 1, the radio-luminous 3C radio galaxies are still giant ellipticals, but the 6C galaxies, only a factor of six lower in radio luminosity, are fainter by about 1 mag in the near-IR and have much more compact near-IR structures. At z1z \sim 1, radio galaxies follow a line in a diagram of optical luminosity verses de Vaucouleurs scale length parallel to the projection of the fundamental plane for nearby ellipticals in this diagram. I discuss the significance of these results for our understanding of radio galaxies.Comment: to be published in `The most distant radio galaxies' KNAW Colloquium, Amsterdam, October 1997, eds Best et al., Kluwer. 15 pages of LaTex, 4 postscript figures, uses knawproc.cl

    Upper limits on K-band polarization in three high-redshift radio galaxies: LBDS 53W091, 3C 441 and MRC 0156-252

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    We present the results of K-band imaging polarimetry of three radio galaxies, including the very red and apparently old z=1.55 galaxy 53W091. We find weak evidence for polarization in components of 3C 441 and in the south-east companion of 53W091, but no evidence of significant polarization in 53W091 itself. We also find strong evidence that MRC 0156-252 is unpolarised. We present upper limits for the K-band polarization of all three sources. For 53W091, the lack of significant K-band polarization provides further confidence that its red R-K colour can be attributed to a mature stellar population, consistent with the detailed analyses of its ultraviolet spectral-energy distribution which indicate a minimum age of 2-3.5 Gyr.Comment: 7 pages, 3 postscript figures. In press at MNRA
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