Speller Ryan.Pdf (2.871Mb)

Total Page:16

File Type:pdf, Size:1020Kb

Speller Ryan.Pdf (2.871Mb) Local Group Analogues by Ryan Speller A thesis presented to the University of Waterloo in fulfillment of the thesis requirement for the degree of Master of Science in Physics Waterloo, Ontario, Canada, 2012 c Ryan Speller 2012 I hereby declare that I am the sole author of this thesis. This is a true copy of the thesis, including any required final revisions, as accepted by my examiners. I understand that my thesis may be made electronically available to the public. ii Abstract The abundance of satellite galaxies is a critical small-scale test of the standard cosmo- logical model. From comparing the predictions of structure formation in simulations with observations of Local Group dwarf galaxies there is a clear mismatch in the abundance, leading to the so-called \missing satellites" problem. The comparison between simulation and observation have, however, suffered from a limited sample of satellite galaxies, with the only reasonably complete sample being from the most local galaxy groups. It is un- known whether the observed abundance of dwarf satellite galaxies of the nearest groups is statistically representative of the abundance of dwarf satellites in the greater universe. We construct a volume-limited sample of galaxies down to a well-defined stellar mass limit 9 (M? ≥ 6 × 10 M ) using the Atlas3D parent sample of spiral and ellipsoidal galaxies by Cappellari et al. 2011 [18]. In order to statistically identify bound satellites around galax- ies in our primary catalogue, we apply cuts on the background based on the properties of known dwarf satellites of the Local Group using both the Sloan Digital Sky Survey Data Release 8 (SDSS DR8) (http://www.sdss3.org/dr8/) spectroscopic and photomet- ric galaxy catalogues. We detect an over-density of faint objects at projected separations of < 500 kpc at S/N ∼ 8, corresponding to an average of 4:8 ± 0:65 satellite detections per primary after stacking these systems and subtracting the background. We further find that the over-density of faint objects strongly depends on primary morphology and magnitude. While the Milky Way seems to be unusual in its number of bright satellites, our faint end satellite abundances are in agreement from the ∆m luminosity function for primaries in our sample as bright as the Milky Way. Our work has extended the work of previous authors by several magnitudes further down the faint end of the luminosity function. iii Acknowledgements I owe a debt of gratitude to my supervisor, Dr. James Taylor, who took a risk in taking me on as a graduate student and whose valuable knowledge and advice have benefited me greatly in this endeavour and the experience with whom will surely leave a significant impact on me long after my graduate experience. I would like to thank the members of my committee for taking the time to read my thesis and also for the feedback from committee meetings. I am also most grateful to my fellow graduate student Jonathan Grossauer, for many illuminating discussions. Lastly, I would like to acknowledge the love and support of my parents, David and Cor- rine Speller, and my fianc´eKrista Burke, whose understanding and encouragement have made this work possible. iv Table of Contents List of Tables vii List of Figures viii 1 Introduction1 1.1 Background Theory...............................3 1.1.1 Cosmology................................3 1.1.2 Structure Formation..........................7 1.2 Galaxies.....................................8 1.2.1 Dwarf galaxies............................. 11 2 The Local Group and Neighbouring Galaxy Groups 12 2.1 The Local Group of Galaxies.......................... 13 2.1.1 Local Group Dwarf Satellites..................... 13 2.2 The Karachentsev Catalogue.......................... 21 2.2.1 The M81 Group............................. 21 2.2.2 The Centaurus A/M83 Group..................... 22 2.2.3 The IC342/Maffei Group........................ 23 2.2.4 Spatial Distribution of Satellite Galaxies............... 23 2.2.5 Velocity Offset............................. 24 2.2.6 The Curious Case of Centaurus A................... 28 2.2.7 Sample Completeness.......................... 30 v 3 Searching for Faint Satellites in SDSS 32 3.1 Foreground................................... 33 3.1.1 Atlas3D................................. 33 3.1.2 Isolation Criteria............................ 34 3.2 Background................................... 34 3.2.1 SDSS................................... 34 3.2.2 Masking................................. 37 3.2.3 Cuts................................... 41 3.3 Preliminary Estimate.............................. 43 3.4 Comparison With Other Groups........................ 43 3.4.1 Guo et al. 2011............................. 44 3.4.2 Lares et al. 2011............................ 45 3.4.3 Liu et al. 2011............................. 45 3.4.4 Strigari et al. 2012........................... 46 3.4.5 Nierenberg et al. 2011/2012...................... 47 4 Results 48 4.1 Density Profile................................. 49 4.2 Number Profile................................. 52 4.3 Number vs. ∆M................................ 59 4.4 Velocity Offset................................. 60 4.5 Comparison With Previous Results..................... 63 4.5.1 Guo et al. 2011............................. 66 4.5.2 Lares et al. 2011............................ 66 4.5.3 Liu et al. 2011............................. 67 4.5.4 Strigari et al. 2012........................... 67 4.5.5 Nierenberg et al. 2011/2012...................... 67 5 Discussion and Conclusion 68 References 72 vi List of Tables 1.1 Hubble T morphological scale......................... 10 2.1 Properties of the known dwarf spheroidal satellites and the Magellanic Clouds of the Milky Way................................ 18 2.2 Properties of the known dwarf spheroidal satellites of Andromeda..... 20 vii List of Figures 1.1 The Hubble Sequence morphological classification of galaxies........9 2.1 Cumulative Milky Way satellite count vs. galactic declination....... 14 2.2 Local Group luminosity function........................ 16 2.3 Absolute magnitude vs. half-light radius of the Local Group dwarf galaxies 17 2.4 Local Group dwarf colour vs. absolute (B-band) magnitude......... 19 2.5 Cumulative satellite number counts of the Local Group and neighbouring galaxy groups.................................. 25 2.6 Projected satellite positions of the Local Group and neighbouring galaxy groups...................................... 26 2.7 Projected positions of satellite galaxies of the Centaurus A subgroup... 27 2.8 Velocity offset vs. projected separation of the satellites of the Local Group and neighbouring galaxy groups........................ 28 2.9 Absolute magnitudes of known galaxies vs. distance............. 31 3.1 Selection Criteria Schematic Diagram..................... 36 3.2 Masking detection in simulated galaxy distributions............. 38 3.3 Masking correction model........................... 39 3.4 Total masked area vs projected separation.................. 40 3.5 Size-magnitude diagram of SDSS data with the Local Group dwarf galaxies seen from a distance of 25 Mpc........................ 42 4.1 Projected radial density profile........................ 50 viii 4.2 Logarithmic projected radial density profile.................. 51 4.3 Cumulative number over-density profile.................... 53 4.4 Cumulative number over-density profile by magnitude............ 55 4.5 Cumulative number over-density profile by morphology........... 56 4.6 Signal to noise on cumulative number over-density profile by magnitude.. 57 4.7 Signal to noise on cumulative number over-density profile by morphology. 58 4.8 Cumulative excess clustering signal binned by difference in apparent mag- nitude from central galaxy unweighted and weighted versions........ 61 4.9 Cumulative excess clustering signal binned by difference in apparent mag- nitude from central galaxy........................... 62 4.10 Binned and cumulative number over-density profile for the spectroscopic sample...................................... 64 4.11 Velocity offset from central host vs projected separation for spectroscopic detections.................................... 65 ix Chapter 1 Introduction In the early 20th century there was Great Debate regarding the scale of the universe. The \Great Debate" between astronomers Harlow Shapley and Heber Curtis began in 1920 and concerned observations of spiral nebulae. Curtis thought of the universe as composed of many galaxies like the Milky Way, as suggested by observations of the spiral nebulae. Shapley opposed this view, taking the stance that the observed spiral nebulae were gas clouds within the Milky Way and that the universe consisted solely of the Milky Way galaxy. The debate was settled when Edwin Hubble first identified Cepheid variable stars in the neighbouring Andromeda galaxy in the mid 1920s. Using the Cepheid variable stars, Hubble was able to calculate the distance to Andromeda, finding that it was large enough to be considered a distinct galaxy. Since this time, the number of known galaxies has increased to the hundreds of billions, populating an intricate web of structure that is presently the focus of much research in astrophysics and cosmology. The structure that we see in the universe today is the result of early fluctuations in the primordial plasma of baryons, photons, and dark matter that filled the early universe which have been amplified over time. Galaxy clusters are the largest virialized structures in the universe, and the satellite abundances of galaxy
Recommended publications
  • Large Scale Structure in the Local Universe — the 2MASS Galaxy Catalog
    Structure and Dynamics in the Local Universe CSIRO PUBLISHING Publications of the Astronomical Society of Australia, 2004, 21, 396–403 www.publish.csiro.au/journals/pasa Large Scale Structure in the Local Universe — The 2MASS Galaxy Catalog Thomas JarrettA A Infrared Processing and Analysis Center, MS 100-22, California Institute of Technology, Pasadena, CA 91125, USA. Email: [email protected] Received 2004 May 3, accepted 2004 October 12 Abstract: Using twin ground-based telescopes, the Two-Micron All Sky Survey (2MASS) scanned both equatorial hemispheres, detecting more than 500 million stars and resolving more than 1.5 million galaxies in the near-infrared (1–2.2 µm) bands. The Extended Source Catalog (XSC) embodies both photometric and astrometric whole sky uniformity, revealing large scale structures in the local Universe and extending our view into the Milky Way’s dust-obscured ‘Zone of Avoidance’. The XSC represents a uniquely unbiased sample of nearby galaxies, particularly sensitive to the underlying, dominant, stellar mass component of galaxies. The basic properties of the XSC, including photometric sensitivity, source counts, and spatial distribution, are presented here. Finally, we employ a photometric redshift technique to add depth to the spatial maps, reconstructing the cosmic web of superclusters spanning the sky. Keywords: general: galaxies — fundamental parameters: infrared — galaxies: clusters — surveys: astronomical 1 Introduction 2003), distance indicators (e.g. Karachentsev et al. 2002), Our understanding of the origin and evolution of the Uni- angular correlation functions (e.g. Maller et al. 2003a), and verse has been fundamentally transformed with seminal the dipole of the local Universe (e.g.
    [Show full text]
  • Stellar Tidal Streams As Cosmological Diagnostics: Comparing Data and Simulations at Low Galactic Scales
    RUPRECHT-KARLS-UNIVERSITÄT HEIDELBERG DOCTORAL THESIS Stellar Tidal Streams as Cosmological Diagnostics: Comparing data and simulations at low galactic scales Author: Referees: Gustavo MORALES Prof. Dr. Eva K. GREBEL Prof. Dr. Volker SPRINGEL Astronomisches Rechen-Institut Heidelberg Graduate School of Fundamental Physics Department of Physics and Astronomy 14th May, 2018 ii DISSERTATION submitted to the Combined Faculties of the Natural Sciences and Mathematics of the Ruperto-Carola-University of Heidelberg, Germany for the degree of DOCTOR OF NATURAL SCIENCES Put forward by GUSTAVO MORALES born in Copiapo ORAL EXAMINATION ON JULY 26, 2018 iii Stellar Tidal Streams as Cosmological Diagnostics: Comparing data and simulations at low galactic scales Referees: Prof. Dr. Eva K. GREBEL Prof. Dr. Volker SPRINGEL iv NOTE: Some parts of the written contents of this thesis have been adapted from a paper submitted as a co-authored scientific publication to the Astronomy & Astrophysics Journal: Morales et al. (2018). v NOTE: Some parts of this thesis have been adapted from a paper accepted for publi- cation in the Astronomy & Astrophysics Journal: Morales, G. et al. (2018). “Systematic search for tidal features around nearby galaxies: I. Enhanced SDSS imaging of the Local Volume". arXiv:1804.03330. DOI: 10.1051/0004-6361/201732271 vii Abstract In hierarchical models of galaxy formation, stellar tidal streams are expected around most galaxies. Although these features may provide useful diagnostics of the LCDM model, their observational properties remain poorly constrained. Statistical analysis of the counts and properties of such features is of interest for a direct comparison against results from numeri- cal simulations. In this work, we aim to study systematically the frequency of occurrence and other observational properties of tidal features around nearby galaxies.
    [Show full text]
  • Chemo-Kinematics of the Milky Way from the SDSS-III MARVELS Survey
    MNRAS 000,1–22 (2018) Preprint 6 October 2020 Compiled using MNRAS LATEX style file v3.0 Chemo-kinematics of the Milky Way from the SDSS-III MARVELS Survey Nolan Grieves,1¢ Jian Ge,1 Neil Thomas,2 Kevin Willis,1 Bo Ma,1 Diego Lorenzo-Oliveira,3,4 A. B. A. Queiroz,5,4 Luan Ghezzi,6 Cristina Chiappini,7,4 Friedrich Anders,7,4 Letícia Dutra-Ferreira,5,4 Gustavo F. Porto de Mello,8,4 Basílio X. Santiago,5,4 Luiz N. da Costa,6,4 Ricardo L. C. Ogando,6,4 E. F. del Peloso,4 Jonathan C. Tan,9,1 Donald P. Schneider,10,11 Joshua Pepper,12 Keivan G. Stassun,13 Bo Zhao,1 Dmitry Bizyaev,14,15 and Kaike Pan14 1Department of Astronomy, University of Florida, Gainesville, FL 32611, USA 2Department of Astronautical Engineering, United States Air Force Academy, CO 80840, USA 3Universidade de São Paulo, Departamento de Astronomia IAG/USP, Rua do Matão 1226, Cidade Universitária, São Paulo, SP 05508-900, Brazil 4Laboratório Interinstitucional de e-Astronomia-LIneA, Rua Gereral José Cristino 77, São Cristóvão, Rio de Janeiro, RJ 20921-400, Brazil 5Instituto de Física, Universidade Federal do Rio Grande do Sul, Caixa Postal 15051,Porto Alegre, RS - 91501-970, Brazil 6Observatório Nacional, Rua General José Cristino 77, São Cristóvão, Rio de Janeiro, RJ 20921-400, Brazil 7Leibniz-Institut für Astrophysik Potsdam, An der Sternwarte 16, 14482 Potsdam, Germany 8Observatório do Valongo, Universidade Federal do Rio de Janeiro, Ladeira do Pedro Antônio 43, Rio de Janeiro, RJ 20080-090, Brazil 9Department of Astronomy, University of Virginia, Charlottesville, VA 22904 10Department of Astronomy and Astrophysics, The Pennsylvania State University, University Park, PA 16802 11Center for Exoplanets and Habitable Worlds, The Pennsylvania State University, University Park, PA 16802 12Department of Physics, Lehigh University, 16 Memorial Drive East, Bethlehem, PA, 18015, USA 13Vanderbilt University, Physics & Astronomy Department, 6301 Stevenson Center Ln., Nashville, TN 37235 14Apache Point Observatory and New Mexico State University, P.O.
    [Show full text]
  • Wyn Evans Institute of Astronomy, Cambridge
    DARK MATTER SUBSTRUCTURES IN THE NEARBY UNIVERSE Wyn Evans Institute of Astronomy, Cambridge Monday, 16 July 2012 DARK MATTER 1. The dwarf spheroidals 2. The ultra-faints 3. The clouds & streams 4. The unknown Monday, 16 July 2012 DWARF SPHEROIDALS Image (35’ by 35’) of the Sculptor dwarf spheroidal taken with the NOAO CTIO 4 m telescope. Monday, 16 July 2012 DWARF SPHEROIDALS Surrounding the Milky Way are 9 classical dwarf spheroidal galaxies (Scu, For, Leo I, Leo II, UMi, Dra, Car, Sex, Sgr). These contain intermediate age to old stellar populations and no gas. They have velocity dispersions ∼ 8-10 km/s, half-light radius ∼ 200-300 pc, and absolute magnitudes MV brighter than -8. They are all highly dark matter dominated, and are natural targets for indirect detection experiments. What are their dark matter profiles? Are they cusped or cored? Monday, 16 July 2012 DWARF SPHEROIDALS Radial velocity surveys with multi-object spectrographs have now provided datasets of thousands of velocities for the giants stars. Early hopes that the photometry and line of sight velocity dispersion profile could be used to constrain the dark halo give way to pessimism. Most early modelers used the spherical Jeans equations to deduce dark matter properties at the center. Monday, 16 July 2012 JEANS EQUATIONS • The spherical Jeans equation is dangerous! If the light profile is cored (Plummer), then assuming isotropy gives a cored dark matter density. If the light profile is cusped (exponential), then so is the dark halo (An & Evans 2009). • The degeneracies in the Jeans equations are also illustrated by Walker et al.
    [Show full text]
  • Spatial Distribution of Galactic Globular Clusters: Distance Uncertainties and Dynamical Effects
    Juliana Crestani Ribeiro de Souza Spatial Distribution of Galactic Globular Clusters: Distance Uncertainties and Dynamical Effects Porto Alegre 2017 Juliana Crestani Ribeiro de Souza Spatial Distribution of Galactic Globular Clusters: Distance Uncertainties and Dynamical Effects Dissertação elaborada sob orientação do Prof. Dr. Eduardo Luis Damiani Bica, co- orientação do Prof. Dr. Charles José Bon- ato e apresentada ao Instituto de Física da Universidade Federal do Rio Grande do Sul em preenchimento do requisito par- cial para obtenção do título de Mestre em Física. Porto Alegre 2017 Acknowledgements To my parents, who supported me and made this possible, in a time and place where being in a university was just a distant dream. To my dearest friends Elisabeth, Robert, Augusto, and Natália - who so many times helped me go from "I give up" to "I’ll try once more". To my cats Kira, Fen, and Demi - who lazily join me in bed at the end of the day, and make everything worthwhile. "But, first of all, it will be necessary to explain what is our idea of a cluster of stars, and by what means we have obtained it. For an instance, I shall take the phenomenon which presents itself in many clusters: It is that of a number of lucid spots, of equal lustre, scattered over a circular space, in such a manner as to appear gradually more compressed towards the middle; and which compression, in the clusters to which I allude, is generally carried so far, as, by imperceptible degrees, to end in a luminous center, of a resolvable blaze of light." William Herschel, 1789 Abstract We provide a sample of 170 Galactic Globular Clusters (GCs) and analyse its spatial distribution properties.
    [Show full text]
  • Observations of New Galaxies in the Zone of Avoidance Using the Arecibo Radio Telescope R
    Observations of new galaxies in the Zone of Avoidance using the Arecibo Radio Telescope R. Birdsall, N. Ballering, A. Beardsley, L. Hunt, S. Stanimirovic (Mentor) University of Wisconsin Astronomy Department Abstract: As part of an undergraduate research techniques course, we detected the neutral hydrogen (HI) spectrum of the galaxy SPITZER192404+145632. This galaxy is located in the Zone of Avoidance (ZoA), a region of the large-scale distribution of galaxies that is obscured by our own galactic disk. Using the Arecibo Observatory*, we were able to confirm the infrared detection made by 9 11 Marleau et al. (2008). We find a redshift of z = 0.019, an HI mass of MHI = 1.02 x 10 Mo, and dynamical mass of MT ≈ 3.9 x 10 Mo. Motivation: The Zone of avoidance (ZoA) is located in the night sky in Observations: Analysis: Using the observed spectrum, we calculate the systemic the direction of our galactic disk. Observations of galaxies at optical We observed remotely velocity, distance, rotational velocity, HI mass, and dynamical mass of wavelengths are extremely difficult in this region because of absorption of on October 16, 2008, SPITZER192404+145632. The systemic velocity is found by simply light by the dust in the disk of the Milky Way. Therefore, fewer objects using position switch- evaluating the midpoint velocity of the spectrum. We found vsys = 5800 have been found in the ZoA than in other regions of space (see Figure 1). ing (ON/OFF) observa- km/s. This corresponds to a redshift of z = 0.019. The distance to the Observations in the ZoA with very sensitive infrared and radio telescopes, tions with the L-wide galaxy is determined using Hubble’s Law: present an opportunity for astronomers to discover new galaxies, as receiver of the Arecibo waves at these wavelengths are not absorbed by dust.
    [Show full text]
  • OBSERVATIONS in the ZONE of AVOIDANCE USING ARECIBO OBSERVATORY R.Birdsall, N.Ballering, A.Beardsley, L.Hunt, R.Wilson, S.Stanim
    OBSERVATIONS IN THE ZONE OF AVOIDANCE USING ARECIBO OBSERVATORY R.Birdsall, N.Ballering, A.Beardsley, L.Hunt, R.Wilson, S.Stanimi 1. Abstract The Zone of Avoidance is a relatively unknown region of space that lies on the other side of our galactic disk. Previous observations made by other collaborators such as Galactic Legacy Infrared Mid-Plane Survey Extraordinaire (GLIMPSE) and MIPS Galactic Plane Survey (MIPSGAL) which surveyed the Zone of Avoidance in the infrared spectrum with the Spitzer Space Telescope.[1] Our team decided to focus on target objects observed by the (GLIMPSE) and(MIPSGAL). These two collaborations identified twenty five new objects in the Infrared Spectrum that had the properties of galaxy like objects. For that reason, we used the Arecibo Radio Observatory in the hopes of detecting the radio signal of neutral hydrogen and identifying these objects. This piece focuses on SP192404+1456 2. Zone of Avoidance The Zone of Avoidance is a interesting region of the night sky because very little is known about what occupies that space. The ZOA is the region of the sky that lies beyond in the direction of the Milky Way galactic center. Thus EM radiation sources from the ZOA must make its way through the galactic disk. This makes detection of these galaxies difficult to near impossible. Both GLIMPSE and MIPSGAL where able to detect twenty-five obscure objects in the IR part of the spectrum, but where unable to verify exact source parameters. 1 2 OBSERVATIONS IN THE ZONE OF AVOIDANCE USING ARECIBO OBSERVATORY [2] In Figure 1. we see a spacial map of previous galactic survey's.
    [Show full text]
  • Galactic Archaeology. the Dwarfs That Survived and Perished
    Galactic Archaeology. The dwarfs that survived and perished Vasily Belokurova,∗ aInstitute of Astronomy, Cambridge Abstract From the archaeological point of view, the local dwarf galaxies are unique objects in which the imprint of the conditions that shaped the early structure formation can be studied today at high resolution. Over the last decade, this new window into the high redshift Universe has started to be exploited using deep wide-field imaging, high resolution spectroscopy and cutting edge N- body and hydro-dynamical simulations. We review the recent advances in the observational studies of the Milky Way dwarf galaxies, with the aim to understand the properties of the population as a whole and to assist an objective comparison between the models and the data. Keywords: Galaxies: kinematics and dynamics, Galaxies: dwarf, dark matter, Local Group, Galaxies: stellar content. 1. Introduction The prehistoric stars whose formation epochs lie beyond the redshift ac- cessible by the Hubble Ultra Deep Field, have been found en masse in little satellites around the Milky Way. Other less fortunate dwarf galaxies have been pulled apart by gravity to furnish the diffuse Galactic halo. These re- cently uncovered relics of the ancient dwarf galaxy population may play a arXiv:1307.0041v2 [astro-ph.GA] 15 Jul 2013 vital role in the pursuit of reconstructing the formation of the Galaxy. Its path from the distant pre-reionisation era, through the most active growth ∗Corresponding author Email address: [email protected] (Vasily Belokurov) Preprint submitted to New Astronomy Reviews July 16, 2013 periods to the present day, can be gleaned by studying the chemical compo- sition and the phase-space density distribution of these halo denizens.
    [Show full text]
  • Science in the Urantia Papers
    Science ¾ Scientific Validation of the UB z By Denver Pearson z By Phil Calabrese ¾ Seraphic Velocities ¾ Astronomy The Scientific Integrity of the Urantia Book by Denver Pearson As scientifically minded readers first peruse the Urantia Book, it soon occurs to them that many of its statements on the natural sciences conflict with currently held data and theories. In the minds of many this gives rise to doubts about the truthfulness of those statements. Wisdom would lead us to realize that nothing short of perfection is perfect, and anything touched by human hands has fingerprints. This should be our guiding thoughts as we contemplate the accuracy of the scientific content of the Urantia Papers. Several years ago, at the first scientific symposium, it was implied by one of the speakers that the revelation contains errors. This implication is alarming. More recently, at the second symposium held in Oklahoma, an interesting publication named "The Science Content of The Urantia Book" was made available (this document is obtainable from the Brotherhood of Man Library). In this publication is an article entitled "Time Bombs" in which the author suggests that the revelators planted certain inaccurate scientific statements in the book in order to prevent it from becoming a fetish. He states "...the revelators incorporated safeguards in the papers that would form The Urantia Book to diminish the tendency to regard it as an object of worship. What safeguards did they use? Suppose they decided to make sure that mortals reading it understood that some cosmological statements in the book would be found to be inaccurate".
    [Show full text]
  • Formation of Disc Galaxies from Cosmological Simulations: Galactic Outflows and Chemical Evolution
    Scuola Internazionale Superiore di Studi Avanzati - Trieste Formation of disc galaxies from cosmological simulations: galactic outflows and chemical evolution Author: Milena Valentini Supervisors: Prof. Stefano Borgani, Prof. Alessandro Bressan, Dr. Giuseppe Murante International School for Advanced Studies SISSA/ISAS A thesis submitted in fulfilment of the requirements for the degree of Doctor Philosophiae in ASTROPHYSICS and COSMOLOGY October 2018 SISSA - Via Bonomea 265 - 34136 TRIESTE - ITALY To Nicola Abstract In this Thesis, I study the formation of late-type galaxies and the role that feedback from stars and supermassive black holes (SMBHs) plays in galaxy evolution across cosmic time. By carrying out cosmological hydrodynamical simulations, I investigate how different processes, such as the cosmological gas accretion from the large scale environment, star formation and chemical enrichment, stellar and AGN (Active Galactic Nucleus) feedback, affect the early stages of forming galaxies and contribute to determine their present-day properties. Driven by the challenging task of simulating late-type galaxies with a limited bulge and a dominant disc in a cosmological context, I study the impact of galactic outflow modelling on the formation and evolution of a disc galaxy. I find that galactic outflows regulate the timing of gas accretion and determine the star formation history of the forming galaxy. Also, I quantify the strong interplay between the adopted hydrodynamical scheme and the sub-resolution model describing star formation and stellar feedback. Throughout this Thesis, I devote particular emphasis to connect chemical evolution and gas dynamics, in order to interpret observations of metal abundance in the interstellar medium (ISM) and circumgalactic medium (CGM).
    [Show full text]
  • What Is an Ultra-Faint Galaxy?
    What is an ultra-faint Galaxy? UCSB KITP Feb 16 2012 Beth Willman (Haverford College) ~ 1/10 Milky Way luminosity Large Magellanic Cloud, MV = -18 image credit: Yuri Beletsky (ESO) and APOD NGC 205, MV = -16.4 ~ 1/40 Milky Way luminosity image credit: www.noao.edu Image credit: David W. Hogg, Michael R. Blanton, and the Sloan Digital Sky Survey Collaboration ~ 1/300 Milky Way luminosity MV = -14.2 Image credit: David W. Hogg, Michael R. Blanton, and the Sloan Digital Sky Survey Collaboration ~ 1/2700 Milky Way luminosity MV = -11.9 Image credit: David W. Hogg, Michael R. Blanton, and the Sloan Digital Sky Survey Collaboration ~ 1/14,000 Milky Way luminosity MV = -10.1 ~ 1/40,000 Milky Way luminosity ~ 1/1,000,000 Milky Way luminosity Ursa Major 1 Finding Invisible Galaxies bright faint blue red Willman et al 2002, Walsh, Willman & Jerjen 2009; see also e.g. Koposov et al 2008, Belokurov et al. Finding Invisible Galaxies Red, bright, cool bright Blue, hot, bright V-band apparent brightness V-band faint Red, faint, cool blue red From ARAA, V26, 1988 Willman et al 2002, Walsh, Willman & Jerjen 2009; see also e.g. Koposov et al 2008, Belokurov et al. Finding Invisible Galaxies Ursa Major I dwarf 1/1,000,000 MW luminosity Willman et al 2005 ~ 1/1,000,000 Milky Way luminosity Ursa Major 1 CMD of Ursa Major I Okamoto et al 2008 Distribution of the Milky Wayʼs dwarfs -14 Milky Way dwarfs 107 -12 -10 classical dwarfs V -8 5 10 Sun M L -6 ultra-faint dwarfs Canes Venatici II -4 Leo V Pisces II Willman I 1000 -2 Segue I 0 50 100 150 200 250 300
    [Show full text]
  • And Ecclesiastical Cosmology
    GSJ: VOLUME 6, ISSUE 3, MARCH 2018 101 GSJ: Volume 6, Issue 3, March 2018, Online: ISSN 2320-9186 www.globalscientificjournal.com DEMOLITION HUBBLE'S LAW, BIG BANG THE BASIS OF "MODERN" AND ECCLESIASTICAL COSMOLOGY Author: Weitter Duckss (Slavko Sedic) Zadar Croatia Pусскй Croatian „If two objects are represented by ball bearings and space-time by the stretching of a rubber sheet, the Doppler effect is caused by the rolling of ball bearings over the rubber sheet in order to achieve a particular motion. A cosmological red shift occurs when ball bearings get stuck on the sheet, which is stretched.“ Wikipedia OK, let's check that on our local group of galaxies (the table from my article „Where did the blue spectral shift inside the universe come from?“) galaxies, local groups Redshift km/s Blueshift km/s Sextans B (4.44 ± 0.23 Mly) 300 ± 0 Sextans A 324 ± 2 NGC 3109 403 ± 1 Tucana Dwarf 130 ± ? Leo I 285 ± 2 NGC 6822 -57 ± 2 Andromeda Galaxy -301 ± 1 Leo II (about 690,000 ly) 79 ± 1 Phoenix Dwarf 60 ± 30 SagDIG -79 ± 1 Aquarius Dwarf -141 ± 2 Wolf–Lundmark–Melotte -122 ± 2 Pisces Dwarf -287 ± 0 Antlia Dwarf 362 ± 0 Leo A 0.000067 (z) Pegasus Dwarf Spheroidal -354 ± 3 IC 10 -348 ± 1 NGC 185 -202 ± 3 Canes Venatici I ~ 31 GSJ© 2018 www.globalscientificjournal.com GSJ: VOLUME 6, ISSUE 3, MARCH 2018 102 Andromeda III -351 ± 9 Andromeda II -188 ± 3 Triangulum Galaxy -179 ± 3 Messier 110 -241 ± 3 NGC 147 (2.53 ± 0.11 Mly) -193 ± 3 Small Magellanic Cloud 0.000527 Large Magellanic Cloud - - M32 -200 ± 6 NGC 205 -241 ± 3 IC 1613 -234 ± 1 Carina Dwarf 230 ± 60 Sextans Dwarf 224 ± 2 Ursa Minor Dwarf (200 ± 30 kly) -247 ± 1 Draco Dwarf -292 ± 21 Cassiopeia Dwarf -307 ± 2 Ursa Major II Dwarf - 116 Leo IV 130 Leo V ( 585 kly) 173 Leo T -60 Bootes II -120 Pegasus Dwarf -183 ± 0 Sculptor Dwarf 110 ± 1 Etc.
    [Show full text]