V. Spatially-Resolved Stellar Angular Momentum, Velocity Dispersion, and Higher Moments of the 41 Most Massive Local Early-Type Galaxies
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The Local Radio-Galaxy Population at 20
Mon. Not. R. Astron. Soc. 000, 1–?? (2013) Printed 2 December 2013 (MN LATEX style file v2.2) The local radio-galaxy population at 20GHz Elaine M. Sadler1⋆, Ronald D. Ekers2, Elizabeth K. Mahony3, Tom Mauch4,5, Tara Murphy1,6 1Sydney Institute for Astronomy, School of Physics, The University of Sydney, NSW 2006, Australia 2Australia Telescope National Facility, CSIRO, PO Box 76, Epping, NSW 1710, Australia 3ASTRON, the Netherlands Institute for Radio Astronomy, Postbus 2, 7990 AA, Dwingeloo, The Netherlands 4Oxford Astrophysics, Department of Physics, Keble Road, Oxford OX1 3RH 5SKA Africa, 3rd Floor, The Park, Park Road, Pinelands, 7405, South Africa 6School of Information Technologies, The University of Sydney, NSW 2006, Australia Accepted 0000 December 08. Received 0000 December 08; in original form 0000 December 08 ABSTRACT We have made the first detailed study of the high-frequency radio-source population in the local universe, using a sample of 202 radio sources from the Australia Telescope 20GHz (AT20G) survey identified with galaxies from the 6dF Galaxy Survey (6dFGS). The AT20G- 6dFGS galaxies have a median redshift of z=0.058 and span a wide range in radio luminosity, allowing us to make the first measurement of the local radio luminosity function at 20GHz. Our sample includes some classical FR-1 and FR-2 radio galaxies, but most of the AT20G-6dFGS galaxies host compact (FR-0) radio AGN which appear lack extended radio emission even at lower frequencies. Most of these FR-0 sources show no evidence for rela- tivistic beaming, and the FR-0 class appears to be a mixed population which includes young Compact Steep-Spectrum (CSS) and Gigahertz-Peaked Spectrum (GPS) radio galaxies. -
Jet-Induced Star Formation in 3C 285 and Minkowski's Object⋆
A&A 574, A34 (2015) Astronomy DOI: 10.1051/0004-6361/201424932 & c ESO 2015 Astrophysics Jet-induced star formation in 3C 285 and Minkowski’s Object? Q. Salomé, P. Salomé, and F. Combes LERMA, Observatoire de Paris, CNRS UMR 8112, 61 avenue de l’Observatoire, 75014 Paris, France e-mail: [email protected] Received 5 September 2014 / Accepted 6 November 2014 ABSTRACT How efficiently star formation proceeds in galaxies is still an open question. Recent studies suggest that active galactic nucleus (AGN) can regulate the gas accretion and thus slow down star formation (negative feedback). However, evidence of AGN positive feedback has also been observed in a few radio galaxies (e.g. Centaurus A, Minkowski’s Object, 3C 285, and the higher redshift 4C 41.17). Here we present CO observations of 3C 285 and Minkowski’s Object, which are examples of jet-induced star formation. A spot (named 3C 285/09.6 in the present paper) aligned with the 3C 285 radio jet at a projected distance of ∼70 kpc from the galaxy centre shows star formation that is detected in optical emission. Minkowski’s Object is located along the jet of NGC 541 and also shows star formation. Knowing the distribution of molecular gas along the jets is a way to study the physical processes at play in the AGN interaction with the intergalactic medium. We observed CO lines in 3C 285, NGC 541, 3C 285/09.6, and Minkowski’s Object with the IRAM 30 m telescope. In the central galaxies, the spectra present a double-horn profile, typical of a rotation pattern, from which we are able to estimate the molecular gas density profile of the galaxy. -
MODEST-18: Dense Stellar Systems in the Era of Gaia, LIGO and LISA June 25 - 29, 2018 | Santorini, Greece
MODEST-18: Dense Stellar Systems in the Era of Gaia, LIGO and LISA June 25 - 29, 2018 | Santorini, Greece POSTER Federico Abbate (Milano-Bicocca): Ionized Gas in 47 Tuc – A Detailed Study with Millisecond Pulsars Globular clusters are known to be very poor in gas despite predictions telling us otherwise. The presence of ionized gas can be investigated through its dispersive effects on the radiation of the millisecond pulsars inside the clusters. This effect led to the first detection of any kind of gas in a globular cluster in the form of ionized gas in 47 Tucanae. With new timing results of these pulsars over longer periods of time we can improve the precision of this measurement and test different distribution models. We first use the parameters measured through timing to measure the dynamical properties of the cluster and the line of sight position of the pulsars. Then we test for gas distribution models. We detect ionized gas distributed with a constant density of n = (0.22 ± 0.05) cm−3. Models predicting a decreasing density or following the stellar distribution are highly disfavoured. Thanks to the quality of the data we are also able to test for the presence of an intermediate mass black hole in the center of the cluster and we derive an upper limit for the mass at ∼ 4000 M_sun. 1 MODEST-18: Dense Stellar Systems in the Era of Gaia, LIGO and LISA June 25 - 29, 2018 | Santorini, Greece POSTER Javier Alonso-García (Antofagasta): VVV and VVV-X Surveys – Unveiling the Innermost Galaxy We find the densest concentrations of field stars in our Galaxy when we look towards its central regions. -
Astronomy 422
Astronomy 422 Lecture 15: Expansion and Large Scale Structure of the Universe Key concepts: Hubble Flow Clusters and Large scale structure Gravitational Lensing Sunyaev-Zeldovich Effect Expansion and age of the Universe • Slipher (1914) found that most 'spiral nebulae' were redshifted. • Hubble (1929): "Spiral nebulae" are • other galaxies. – Measured distances with Cepheids – Found V=H0d (Hubble's Law) • V is called recessional velocity, but redshift due to stretching of photons as Universe expands. • V=H0D is natural result of uniform expansion of the universe, and also provides a powerful distance determination method. • However, total observed redshift is due to expansion of the universe plus a galaxy's motion through space (peculiar motion). – For example, the Milky Way and M31 approaching each other at 119 km/s. • Hubble Flow : apparent motion of galaxies due to expansion of space. v ~ cz • Cosmological redshift: stretching of photon wavelength due to expansion of space. Recall relativistic Doppler shift: Thus, as long as H0 constant For z<<1 (OK within z ~ 0.1) What is H0? Main uncertainty is distance, though also galaxy peculiar motions play a role. Measurements now indicate H0 = 70.4 ± 1.4 (km/sec)/Mpc. Sometimes you will see For example, v=15,000 km/s => D=210 Mpc = 150 h-1 Mpc. Hubble time The Hubble time, th, is the time since Big Bang assuming a constant H0. How long ago was all of space at a single point? Consider a galaxy now at distance d from us, with recessional velocity v. At time th ago it was at our location For H0 = 71 km/s/Mpc Large scale structure of the universe • Density fluctuations evolve into structures we observe (galaxies, clusters etc.) • On scales > galaxies we talk about Large Scale Structure (LSS): – groups, clusters, filaments, walls, voids, superclusters • To map and quantify the LSS (and to compare with theoretical predictions), we use redshift surveys. -
REDSHIFTS and VELOCITY DISPERSIONS of GALAXY CLUSTERS in the HOROLOGIUM-RETICULUM SUPERCLUSTER Matthew C
The Astronomical Journal, 131:1280–1287, 2006 March A # 2006. The American Astronomical Society. All rights reserved. Printed in U.S.A. REDSHIFTS AND VELOCITY DISPERSIONS OF GALAXY CLUSTERS IN THE HOROLOGIUM-RETICULUM SUPERCLUSTER Matthew C. Fleenor, James A. Rose, and Wayne A. Christiansen Department of Physics and Astronomy, University of North Carolina, Chapel Hill, NC 27599; fl[email protected], [email protected], [email protected] Melanie Johnston-Hollitt Department of Physics, University of Tasmania, Hobart, TAS 7005, Australia; [email protected] Richard W. Hunstead School of Physics, University of Sydney, Sydney, NSW 2006, Australia; [email protected] Michael J. Drinkwater Department of Physics, University of Queensland, Brisbane, QLD 4072, Australia; [email protected] and William Saunders Anglo-Australian Observatory, Epping, NSW 1710, Australia; [email protected] Received 2005 October 18; accepted 2005 November 15 ABSTRACT We present 118 new optical redshifts for galaxies in 12 clusters in the Horologium-Reticulum supercluster (HRS) of galaxies. For 76 galaxies, the data were obtained with the Dual Beam Spectrograph on the 2.3 m telescope of the Australian National University at Siding Spring Observatory. After combining 42 previously unpublished redshifts with our new sample, we determine mean redshifts and velocity dispersions for 13 clusters in which previous observa- tional data were sparse. In 6 of the 13 clusters, the newly determined mean redshifts differ by more than 750 km sÀ1 from the published values. In three clusters, A3047, A3109, and A3120, the redshift data indicate the presence of multiple components along the line of sight. -
Properties of Simulated Milky Way-Mass Galaxies in Loose Group and field Environments
A&A 547, A63 (2012) Astronomy DOI: 10.1051/0004-6361/201219649 & c ESO 2012 Astrophysics Properties of simulated Milky Way-mass galaxies in loose group and field environments C. G. Few1,B.K.Gibson1,2,3,S.Courty4, L. Michel-Dansac4,C.B.Brook5, and G. S. Stinson6 1 Jeremiah Horrocks Institute, University of Central Lancashire, Preston, PR1 2HE, UK e-mail: [email protected] 2 Department of Astronomy & Physics, Saint Mary’s University, Halifax, Nova Scotia, B3H 3C3, Canada 3 Monash Centre for Astrophysics, Monash University, 3800 Victoria, Australia 4 Université de Lyon, Université Lyon 1, Observatoire de Lyon, CNRS, UMR 5574, Centre de Recherche Astrophysique de Lyon, École Normale Supérieure de Lyon, 9 avenue Charles André, 69230 Saint-Genis Laval, France 5 Grupo de Astrofísica, Departamento de Fisica Teorica, Modulo C-15, Universidad Autónoma de Madrid, 28049 Cantoblanco, Spain 6 Max-Planck-Institut für Astronomie, Königstuhl 17, 69117 Heidelberg, Germany Received 22 May 2012 / Accepted 27 September 2012 ABSTRACT Aims. We test the validity of comparing simulated field disk galaxies with the empirical properties of systems situated within envi- ronments more comparable to loose groups, including the Milky Way’s Local Group. Methods. Cosmological simulations of Milky Way-mass galaxies have been realised in two different environment samples: in the field and in loose groups environments with similar properties to the Local Group. Apart from the differing environments of the galaxies, the samples are kept as homogeneous as possible with equivalent ranges in last major merger time, halo mass and halo spin. Comparison of these two samples allow for systematic differences in the simulations to be identified. -
A 10000-Solar-Mass Black Hole in the Nucleus of a Bulgeless Dwarf Galaxy
A 10,000-solar-mass black hole in the nucleus of a bulge- less dwarf galaxy Jong-Hak Woo1, Hojin Cho1, Elena Gallo2, Edmund Hodges-Kluck2;3;4, Huynh Anh Le1, Jaejin Shin1, Donghoon Son1, & John C. Horst5 1Department of Physics & Astronomy, Seoul National University, Seoul, 08826, Republic of Korea 2Department of Astronomy, University of Michigan, Ann Arbor, MI 48109, USA 3Department of Astronomy, University of Maryland, College Park, MD 20742, USA 4NASA/GSFC, Code 662, Greenbelt, MD 20771, USA 5San Diego State University, San Diego, CA 92182, USA The motions of gas and stars in the nuclei of nearby large galaxies have demonstrated that massive black holes are common1 and that their masses strongly correlate with the stellar 2;3;4 velocity dispersion σ? of the bulge . This correlation suggests that massive black holes and galaxies influence each other’s growth5;6;7. Dynamical measurements are less reliable when the sphere of influence is unresolved, thus it remains unknown whether this correlation exists in galaxies much smaller than the Milky Way, as well as what fraction of these galaxies have central black holes. Light echoes from photoionized clouds around accreting black 8;9 arXiv:1905.00145v2 [astro-ph.GA] 13 Jun 2019 holes , in combination with the velocity of these clouds, yield a direct mass measurement that circumvents this difficulty. Here we report an exceptionally low reverberation delay of 83 14 minutes between variability in the accretion disk and high velocity Hα emission from ± the nucleus of the bulgeless dwarf galaxy NGC 4395. Combined with the Hα line-of-sight 1 −1 velocity dispersion σ = 426 1 km s , this lag determines a mass of about 10,000 M for line ± the black hole. -
Dark Matter in Elliptical Galaxies?
Chapter 13 Dark Matter in Elliptical Galaxies? Dark matter in elliptical galaxies includes both central black holes and extended dark halos. On dimensional grounds, one might expect that the velocity dispersion profile !(r) of an elliptical galaxy to be related to the cumulative mass profile M(r) by r ! 2(r) M(r) . (13.1) ! G In fact, dispersion alone does not provide enough information; without additional constraints on the velocity anisotropy, a very wide range of mass profiles are consistent with a given dispersion profile. Luckily, there is one component commonly found in elliptical galaxies which can be used to detect extended dark halos – X-ray emitting gas. 13.1 Jeans Models of Spherical Systems Perhaps the simplest application of the Jeans equations is to equilibrium spherical systems. Assum- ing that all properties are constant in time and invariant with respect to rotation about the center, the radial Jeans equation is d 2" d# ("v2) + (v2 v2) = " , (13.2) dr r r r − t − dr where " is the stellar density, and vr and vt are velocities in the radial and tangential directions, respectively. Define the radial and tangential dispersions, ! 2 v2 , ! 2 v2 , (13.3) r ≡ r t ≡ t and the anisotropy, $ 1 ! 2/! 2 , (13.4) ≡ − t r which is % for a purely tangential velocity distribution, 0 for an isotropic distribution, and +1 for − a purely radial velocity distribution. Then (13.2) becomes 1 d 2 d# ("! 2) + $! 2 = . (13.5) " dr r r r − dr If "(r), $(r), and #(r) are known functions, (13.5) may treated as a differential equation for the radial dispersion profile. -
Arxiv:1801.08245V2 [Astro-Ph.GA] 14 Feb 2018
Draft version June 21, 2021 Preprint typeset using LATEX style emulateapj v. 12/16/11 THE MASSIVE SURVEY IX: PHOTOMETRIC ANALYSIS OF 35 HIGH MASS EARLY-TYPE GALAXIES WITH HST WFC3/IR1 Charles F. Goullaud Department of Physics, University of California, Berkeley, CA, USA; [email protected] Joseph B. Jensen Utah Valley University, Orem, UT, USA John P. Blakeslee Herzberg Astrophysics, Victoria, BC, Canada Chung-Pei Ma Department of Astronomy, University of California, Berkeley, CA, USA Jenny E. Greene Princeton University, Princeton, NJ, USA Jens Thomas Max Planck-Institute for Extraterrestrial Physics, Garching, Germany. Draft version June 21, 2021 ABSTRACT We present near-infrared observations of 35 of the most massive early-type galaxies in the local universe. The observations were made using the infrared channel of the Hubble Space Telescope (HST ) Wide Field Camera 3 (WFC3) in the F110W (1.1 µm) filter. We measured surface brightness profiles and elliptical isophotal fit parameters from the nuclear regions out to a radius of ∼10 kpc in most cases. We find that 37% (13) of the galaxies in our sample have isophotal position angle rotations greater than 20◦ over the radial range imaged by WFC3/IR, which is often due to the presence of neighbors or multiple nuclei. Most galaxies in our sample are significantly rounder near the center than in the outer regions. This sample contains six fast rotators and 28 slow rotators. We find that all fast rotators are either disky or show no measurable deviation from purely elliptical isophotes. Among slow rotators, significantly disky and boxy galaxies occur with nearly equal frequency. -
The Cosmic Distance Scale • Distance Information Is Often Crucial to Understand the Physics of Astrophysical Objects
The cosmic distance scale • Distance information is often crucial to understand the physics of astrophysical objects. This requires knowing the basic properties of such an object, like its size, its environment, its location in space... • There are essentially two ways to derive distances to astronomical objects, through absolute distance estimators or through relative distance estimators • Absolute distance estimators Objects for whose distance can be measured directly. They have physical properties which allow such a measurement. Examples are pulsating stars, supernovae atmospheres, gravitational lensing time delays from multiple quasar images, etc. • Relative distance estimators These (ultimately) depend on directly measured distances, and are based on the existence of types of objects that share the same intrinsic luminosity (and whose distance has been determined somehow). For example, there are types of stars that have all the same intrinsic luminosity. If the distance to a sample of these objects has been measured directly (e.g. through trigonometric parallax), then we can use these to determine the distance to a nearby galaxy by comparing their apparent brightness to those in the Milky Way. Essentially we use that log(D1/D2) = 1/5 * [(m1 –m2) - (A1 –A2)] where D1 is the distance to system 1, D2 is the distance to system 2, m1 is the apparent magnitudes of stars in S1 and S2 respectively, and A1 and A2 corrects for the absorption towards the sources in S1 and S2. Stars or objects which have the same intrinsic luminosity are known as standard candles. If the distance to such a standard candle has been measured directly, then the relative distances will have been anchored to an absolute distance scale. -
7.5 X 11.5.Threelines.P65
Cambridge University Press 978-0-521-19267-5 - Observing and Cataloguing Nebulae and Star Clusters: From Herschel to Dreyer’s New General Catalogue Wolfgang Steinicke Index More information Name index The dates of birth and death, if available, for all 545 people (astronomers, telescope makers etc.) listed here are given. The data are mainly taken from the standard work Biographischer Index der Astronomie (Dick, Brüggenthies 2005). Some information has been added by the author (this especially concerns living twentieth-century astronomers). Members of the families of Dreyer, Lord Rosse and other astronomers (as mentioned in the text) are not listed. For obituaries see the references; compare also the compilations presented by Newcomb–Engelmann (Kempf 1911), Mädler (1873), Bode (1813) and Rudolf Wolf (1890). Markings: bold = portrait; underline = short biography. Abbe, Cleveland (1838–1916), 222–23, As-Sufi, Abd-al-Rahman (903–986), 164, 183, 229, 256, 271, 295, 338–42, 466 15–16, 167, 441–42, 446, 449–50, 455, 344, 346, 348, 360, 364, 367, 369, 393, Abell, George Ogden (1927–1983), 47, 475, 516 395, 395, 396–404, 406, 410, 415, 248 Austin, Edward P. (1843–1906), 6, 82, 423–24, 436, 441, 446, 448, 450, 455, Abbott, Francis Preserved (1799–1883), 335, 337, 446, 450 458–59, 461–63, 470, 477, 481, 483, 517–19 Auwers, Georg Friedrich Julius Arthur v. 505–11, 513–14, 517, 520, 526, 533, Abney, William (1843–1920), 360 (1838–1915), 7, 10, 12, 14–15, 26–27, 540–42, 548–61 Adams, John Couch (1819–1892), 122, 47, 50–51, 61, 65, 68–69, 88, 92–93, -
Shapley Supercluster Survey: Mapping the filamentary Network Connecting the Clusters
MNRAS 481, 1055–1074 (2018) doi:10.1093/mnras/sty2338 Advance Access publication 2018 August 25 Shapley Supercluster Survey: mapping the filamentary network connecting the clusters C. P. Haines,1,2‹ G. Busarello,3 P. Merluzzi,3‹ K. A. Pimbblet,4 F. P. A. Vogt,5† 6 3 3 3‡ M. A. Dopita, A. Mercurio, A. Grado, and L. Limatola Downloaded from https://academic.oup.com/mnras/article-abstract/481/1/1055/5079654 by University of Hull user on 05 February 2019 1INAF - Osservatorio Astronomico di Brera, via Brera 28, I-20121 Milano, Italy 2Departamento de Astronom´ıa, Universidad de Chile, Casilla 36-D, Correo Central, Santiago, Chile 3INAF - Osservatorio Astronomico di Capodimonte, via Moiariello 16, I-80131 Napoli, Italy 4E.A. Milne Centre for Astophysics, University of Hull, Cottingham Road, Kingston-upon-Hull, HU6 7RX, UK 5European Southern Observatory, Av. Alonso de Cordova´ 3107, Vitacura, Casilla 19001, Santiago, Chile 6Research School of Australia and Astrophysics, Australian National University, Canberra, ACT 2611, Australia Accepted 2018 August 21. Received 2018 August 21; in original form 2018 July 2 ABSTRACT We have mapped the structure and connectivity of the Shapley supercluster core and its sur- roundings as traced by its member galaxies. To achieve this, we have carried out a new redshift survey of galaxies across a 21 square degree region (17×17 Mpc2) of the Shapley supercluster containing 11 rich clusters, all lying at z ∼ 0.048. This survey aims to provide full spectro- scopic coverage of galaxies for the Shapley Supercluster Survey (ShaSS), a multiwavelength survey based on high-quality optical ugri and near-infrared K-band imaging acquired with the 2.6-m VST and 4.1-m VISTA telescopes.