Quasar-Galaxy Associations
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Quantum Detection of Wormholes Carlos Sabín
www.nature.com/scientificreports OPEN Quantum detection of wormholes Carlos Sabín We show how to use quantum metrology to detect a wormhole. A coherent state of the electromagnetic field experiences a phase shift with a slight dependence on the throat radius of a possible distant wormhole. We show that this tiny correction is, in principle, detectable by homodyne measurements Received: 16 February 2017 after long propagation lengths for a wide range of throat radii and distances to the wormhole, even if the detection takes place very far away from the throat, where the spacetime is very close to a flat Accepted: 15 March 2017 geometry. We use realistic parameters from state-of-the-art long-baseline laser interferometry, both Published: xx xx xxxx Earth-based and space-borne. The scheme is, in principle, robust to optical losses and initial mixedness. We have not observed any wormhole in our Universe, although observational-based bounds on their abundance have been established1. The motivation of the search of these objects is twofold. On one hand, the theoretical implications of the existence of topological spacetime shortcuts would entail a challenge to our understanding of deep physical principles such as causality2–5. On the other hand, typical phenomena attributed to black holes can be mimicked by wormholes. Therefore, if wormholes exist the identity of the objects in the center of the galaxies might be questioned6 as well as the origin of the already observed gravitational waves7, 8. For these reasons, there is a renewed interest in the characterization of wormholes9–11 and in their detection by classical means such as gravitational lensing12, 13, among others14. -
Active Galactic Nuclei: a Brief Introduction
Active Galactic Nuclei: a brief introduction Manel Errando Washington University in St. Louis The discovery of quasars 3C 273: The first AGN z=0.158 2 <latexit sha1_base64="4D0JDPO4VKf1BWj0/SwyHGTHSAM=">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</latexit> <latexit sha1_base64="H7Rv+ZHksM7/70841dw/vasasCQ=">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</latexit> The power source of quasars • The luminosity (L) of quasars, i.e. how bright they are, can be as high as Lquasar ~ 1012 Lsun ~ 1040 W. • The energy source of quasars is accretion power: - Nuclear fusion: 2 11 1 ∆E =0.007 mc =6 10 W s g− -
Quantum Foundations with Astronomical Photons Calvin Leung
Claremont Colleges Scholarship @ Claremont HMC Senior Theses HMC Student Scholarship 2017 Quantum Foundations with Astronomical Photons Calvin Leung Recommended Citation Leung, Calvin, "Quantum Foundations with Astronomical Photons" (2017). HMC Senior Theses. 112. https://scholarship.claremont.edu/hmc_theses/112 This Open Access Senior Thesis is brought to you for free and open access by the HMC Student Scholarship at Scholarship @ Claremont. It has been accepted for inclusion in HMC Senior Theses by an authorized administrator of Scholarship @ Claremont. For more information, please contact [email protected]. Quantum Foundations with Astronomical Photons Calvin Leung Jason Gallicchio, Advisor Department of Physics May, 2017 Copyright c 2017 Calvin Leung. The author grants Harvey Mudd College the nonexclusive right to make this work available for noncommercial, educational purposes, provided that this copyright statement appears on the reproduced materials and notice is given that the copying is by permission of the author. To disseminate otherwise or to republish requires written permission from the author. Abstract Bell's inequalities impose an upper limit on correlations between measurements of two-photon states under the assumption that the pho- tons play by a set of local rules rather than by quantum mechanics. Quantum theory and decades of experiments both violate this limit. Recent theoretical work in quantum foundations has demonstrated that a local realist model can explain the non-local correlations observed in experimental tests of Bell's inequality if the underlying probability dis- tribution of the local hidden variable depends on the choice of measure- ment basis, or \setting choice". By using setting choices determined by astrophysical events in the distant past, it is possible to asymptotically guarantee that the setting choice is independent of local hidden vari- ables which come into play around the time of the experiment, closing this \freedom-of-choice" loophole. -
A Multimessenger View of Galaxies and Quasars from Now to Mid-Century M
A multimessenger view of galaxies and quasars from now to mid-century M. D’Onofrio 1;∗, P. Marziani 2;∗ 1 Department of Physics & Astronomy, University of Padova, Padova, Italia 2 National Institute for Astrophysics (INAF), Padua Astronomical Observatory, Italy Correspondence*: Mauro D’Onofrio [email protected] ABSTRACT In the next 30 years, a new generation of space and ground-based telescopes will permit to obtain multi-frequency observations of faint sources and, for the first time in human history, to achieve a deep, almost synoptical monitoring of the whole sky. Gravitational wave observatories will detect a Universe of unseen black holes in the merging process over a broad spectrum of mass. Computing facilities will permit new high-resolution simulations with a deeper physical analysis of the main phenomena occurring at different scales. Given these development lines, we first sketch a panorama of the main instrumental developments expected in the next thirty years, dealing not only with electromagnetic radiation, but also from a multi-messenger perspective that includes gravitational waves, neutrinos, and cosmic rays. We then present how the new instrumentation will make it possible to foster advances in our present understanding of galaxies and quasars. We focus on selected scientific themes that are hotly debated today, in some cases advancing conjectures on the solution of major problems that may become solved in the next 30 years. Keywords: galaxy evolution – quasars – cosmology – supermassive black holes – black hole physics 1 INTRODUCTION: TOWARD MULTIMESSENGER ASTRONOMY The development of astronomy in the second half of the XXth century followed two major lines of improvement: the increase in light gathering power (i.e., the ability to detect fainter objects), and the extension of the frequency domain in the electromagnetic spectrum beyond the traditional optical domain. -
A Supernova Origin for Dust in a High-Redshift Quasar
A SUPERNOVA ORIGIN FOR DUST IN A HIGH-REDSHIFT QUASAR R. Maiolino ∗, R. Schneider †∗, E. Oliva ‡∗, S. Bianchi §, A. Ferrara ¶, F. Mannucci§, M. Pedani‡, M. Roca Sogorb k ∗ INAF - Osservatorio Astrofisico di Arcetri, Largo Enrico Fermi 5, 50125 Firenze, Italy † “Enrico Fermi” Center, Via Panisperna 89/A, 00184 Roma, Italy ‡ Telescopio Nazionale Galileo, C. Alvarez de Abreu, 70, 38700 S.ta Cruz de La Palma, Spain § CNR-IRA, Sezione di Firenze, Largo Enrico Fermi 5, 50125 Firenze, Italy ¶ SISSA/International School for Advanced Studies, Via Beirut 4, 34100 Trieste, Italy k Astrofisico Fco. S`anchez, Universidad de La Laguna, 38206 La Laguna, Tenerife, Spain Interstellar dust plays a crucial role in the evolution of the Universe by assisting the formation of molecules1, by triggering the formation of the first low-mass stars2, and by absorbing stellar ultraviolet-optical light and subsequently re-emitting it at infrared/millimetre wavelengths. Dust is thought to be produced predominantly in the envelopes of evolved (age >1 Gyr), low-mass stars3. This picture has, however, recently been brought into question by the discovery of large masses of dust in the host galaxies of quasars4,5 at redshift z > 6, when the age of the Universe was less than 1 Gyr. Theoretical studies6,7,8, corroborated by observations of nearby supernova remnants9,10,11, have suggested that supernovae provide a fast and efficient dust formation environment in the early Universe. Here we report infrared observations of a quasar at redshift 6.2, which are used to obtain directly its dust extinction curve. We then show that such a curve is in excellent agreement with supernova dust models. -
Fy10 Budget by Program
AURA/NOAO FISCAL YEAR ANNUAL REPORT FY 2010 Revised Submitted to the National Science Foundation March 16, 2011 This image, aimed toward the southern celestial pole atop the CTIO Blanco 4-m telescope, shows the Large and Small Magellanic Clouds, the Milky Way (Carinae Region) and the Coal Sack (dark area, close to the Southern Crux). The 33 “written” on the Schmidt Telescope dome using a green laser pointer during the two-minute exposure commemorates the rescue effort of 33 miners trapped for 69 days almost 700 m underground in the San Jose mine in northern Chile. The image was taken while the rescue was in progress on 13 October 2010, at 3:30 am Chilean Daylight Saving time. Image Credit: Arturo Gomez/CTIO/NOAO/AURA/NSF National Optical Astronomy Observatory Fiscal Year Annual Report for FY 2010 Revised (October 1, 2009 – September 30, 2010) Submitted to the National Science Foundation Pursuant to Cooperative Support Agreement No. AST-0950945 March 16, 2011 Table of Contents MISSION SYNOPSIS ............................................................................................................ IV 1 EXECUTIVE SUMMARY ................................................................................................ 1 2 NOAO ACCOMPLISHMENTS ....................................................................................... 2 2.1 Achievements ..................................................................................................... 2 2.2 Status of Vision and Goals ................................................................................ -
Quasar Pairs with Arcminute Angular Separations
A&A 372, 1–7 (2001) Astronomy DOI: 10.1051/0004-6361:20010283 & c ESO 2001 Astrophysics Quasar pairs with arcminute angular separations V. I. Zhdanov1,2 and J. Surdej1,? 1 Institut d’Astrophysique, Universit´edeLi`ege, Avenue de Cointe 5, 4000 Li`ege, Belgium 2 Astronomical Observatory of Kyiv University, Observatorna St. 3, UA- 04053 Kyiv, Ukraine Received 19 October 2000 / Accepted 16 February 2001 Abstract. We use the V´eron-Cetty & V´eron (2000) catalog (VV) of 13 213 quasars to investigate their possible physical grouping over angular scales 1000 ≤ ∆θ ≤ 100000. We first estimate the number of quasar pairs that would be expected in VV assuming a random distribution for the quasar positions and taking into account observational selection effects affecting heterogeneous catalogs. We find in VV a statistically significant (>3σ)excessofpairs of quasars with similar redshifts (∆z ≤ 0.01) and angular separations in the 5000−10000 range, corresponding to projected linear separations (0.2−0.5) Mpc/h75(ΩM =1, ΩΛ =0)or(0.4−0.7) Mpc/h75(ΩM =0.3, ΩΛ =0.7). There is also some excess in the 10000−60000 range corresponding to (1−5) Mpc in projected linear separations. If most of these quasar pairs do indeed belong to large physical entities, these separations must represent the inner scales of huge mass concentrations (cf. galaxy clusters or superclusters) at high redshifts; but it is not excluded that some of the pairs may actually consist of multiple quasar images produced by gravitational lensing. Of course, a fraction of these pairs could also arise due to random projections of quasars on the sky. -
Stellar Death: White Dwarfs, Neutron Stars, and Black Holes
Stellar death: White dwarfs, Neutron stars & Black Holes Content Expectaions What happens when fusion stops? Stars are in balance (hydrostatic equilibrium) by radiation pushing outwards and gravity pulling in What will happen once fusion stops? The core of the star collapses spectacularly, leaving behind a dead star (compact object) What is left depends on the mass of the original star: <8 M⦿: white dwarf 8 M⦿ < M < 20 M⦿: neutron star > 20 M⦿: black hole Forming a white dwarf Powerful wind pushes ejects outer layers of star forming a planetary nebula, and exposing the small, dense core (white dwarf) The core is about the radius of Earth Very hot when formed, but no source of energy – will slowly fade away Prevented from collapsing by degenerate electron gas (stiff as a solid) Planetary nebulae (nothing to do with planets!) THE RING NEBULA Planetary nebulae (nothing to do with planets!) THE CAT’S EYE NEBULA Death of massive stars When the core of a massive star collapses, it can overcome electron degeneracy Huge amount of energy BAADE ZWICKY released - big supernova explosion Neutron star: collapse halted by neutron degeneracy (1934: Baade & Zwicky) Black Hole: star so massive, collapse cannot be halted SN1006 1967: Pulsars discovered! Jocelyn Bell and her supervisor Antony Hewish studying radio signals from quasars Discovered recurrent signal every 1.337 seconds! Nicknamed LGM-1 now called PSR B1919+21 BRIGHTNESS TIME NATURE, FEBRUARY 1968 1967: Pulsars discovered! Beams of radiation from spinning neutron star Like a lighthouse Neutron -
Observational Searches for Star-Forming Galaxies at Z > 6
Publications of the Astronomical Society of Australia (PASA), Vol. 33, e037, 35 pages (2016). C Astronomical Society of Australia 2016; published by Cambridge University Press. doi:10.1017/pasa.2016.26 Observational Searches for Star-Forming Galaxies at z > 6 Steven L. Finkelstein1,2 1Department of Astronomy, The University of Texas at Austin, Austin, TX 78712, USA 2Email: [email protected] (Received November 19, 2015; Accepted June 23, 2016) Abstract Although the universe at redshifts greater than six represents only the first one billion years (<10%) of cosmic time, the dense nature of the early universe led to vigorous galaxy formation and evolution activity which we are only now starting to piece together. Technological improvements have, over only the past decade, allowed large samples of galaxies at such high redshifts to be collected, providing a glimpse into the epoch of formation of the first stars and galaxies. A wide variety of observational techniques have led to the discovery of thousands of galaxy candidates at z > 6, with spectroscopically confirmed galaxies out to nearly z = 9. Using these large samples, we have begun to gain a physical insight into the processes inherent in galaxy evolution at early times. In this review, I will discuss (i) the selection techniques for finding distant galaxies, including a summary of previous and ongoing ground and space-based searches, and spectroscopic follow-up efforts, (ii) insights into galaxy evolution gleaned from measures such as the rest-frame ultraviolet luminosity function, the stellar mass function, and galaxy star-formation rates, and (iii) the effect of galaxies on their surrounding environment, including the chemical enrichment of the universe, and the reionisation of the intergalactic medium. -
HST Images of Nearby Luminous Quasars II: Results for Eight Quasars and Tests of the Detection Sensitivity
HST IMAGES OF NEARBY LUMINOUS QUASARS I I RESULTS FOR EIGHT QUASARS AND TESTS OF THE 1 DETECTION SENSITIVITY John N Bahcall Soa Kirhakos Institute for Advanced Study School of Natural Sciences Princeton NJ and Donald P Schneider Department of Astronomy and Astrophysics The Pennsylvania State University University Park PA and Institute for Advanced Study School of Natural Sciences Princeton NJ Received accepted astro-ph/9501018 6 Jan 95 Based on observations with the NASAESA Hubble Space Telescope obtained at the Space Telescope Science Institute which is op erated by the Asso ciation of Universities for Research in Astronomy Inc under NASA contract NAS ABSTRACT HST observations of eight intrinsically luminous quasars with redshifts b etween and are presented Seven companion galaxies brighter than M H kms Mp c lie within a pro jected V distance of kp c of the quasars three of the companions are lo cated closer 00 than kp c pro jected distance from the quasars well within the volume that would b e enclosed by a typical L host galaxy The observed asso ciation of quasars and companion galaxies is statistically signicant and may b e an imp ortant element in the luminousquasar phenomenon Evidence for candidate host galaxies is presented for the three most promising cases PG C and PG but additional observations are required b efore the characteristics of the candidate hosts can b e regarded as established Upp er limits are placed on the visualband brightnesses of representative galactic hosts for all of the quasars -
Safeye Quasar 900 the New Safeye Quasar 900 Is an Open Path Detection System Which Provides Continuous Monitoring for Combustible Hydrocarbon Gases
SafEye Quasar 900 The New SafEye Quasar 900 is an open path detection system which provides continuous monitoring for combustible hydrocarbon gases. It employs "spectral fingerprint" analysis of the atmosphere using the Differential Optical Absorption Spectroscopy (DOAS) technique. FEATURES & BENEFITS • Detects Hydrocarbon gases including methane, ethylene, propylene • Detection range: 4-200m in three different models (same detector different sources) • Built in event recorder – real time record of the last 100 events • Fast connection to Hand-Held for prognostic and diagnostic maintenance • Heated optics • Design to meet SIL2, per IEC61508 • Outputs: - 0-20mA - HART protocol for maintenance and asset managements - RS-485, Modbus Compatible The Quasar 900 consists of a Xenon Flash infrared transmitter and infrared receiver, separated over a • High reliability – MTBF minimum 100,000 hours line of sight from 13 ft (4m) up to 650 ft (200m) • User programmable via HART or RS-485 in extremely harsh environments where dust, fog, • 3 years warranty (10 years for the flash source) rain, snow or vibration can cause a high reduction of signal. • Ex approval: - Design to ATEX, IECEx per The Quasar 900 transmitter and receiver are both Ex II 2 (1) GD housed in a rugged, stainless steel, ATEX and IECEx approved enclosure. The main enclosure is EExd EEx de ia II C T5 flameproof with an integral, segregated, EExe - Design to FM, CSA per increased safety terminal section. Class I Div 1 Group B, C and D Class I, II Div 1 Group E, F and D The hand-held communication unit can be connected - Performance test: design to FM6325 and in-situ via the intrinsically safe approved data port EN50241-1 and 2 for prognostic and diagnostic maintenance. -
8. Active Galactic Nuclei. Radio Galaxies and Quasars
8. ACTIVE GALACTIC NUCLEI. RADIO GALAXIES AND QUASARS This Section starts analyzing the phenomenon of extragalactic Active Galactic Nuclei. Here we will essentially discuss their low-photon-energy emissions, while in Sect. 9 we will expand on the high-photon-energy ones. 8.1 Active Galactic Nuclei: Generalities We know that normal galaxies constitute the majority population of cosmic sources in 12 the local universe. Although they may be quite massive (up to 10 M), they are not 11 44 typically very luminous (never more luminous than 10 Lʘ10 erg/sec). For this reason normal galaxies have remained hardly detectable at very large cosmic distances for long time, with recent advances mostly thanks to technological observational improvements. For several decades, since the ’60, the only detectable objects at large cosmic distances belonged to a completely different class of sources, which did not derive their energy from thermonuclear burning in stars. These are the Active Galactic Nuclei, for which we use the acronym AGN. The galaxies hosting them are called active galaxies. For their luminosity, Active Galactic Nuclei and Active Galaxies have plaid a key role in the development of cosmology, further to the fact that they make one of the most important themes of extragalactic astrophysics and High Energy Astrophysics. Apparently, the interest for the Active Galaxies as a population might seem modest, as in the local universe they make a small fraction of normal galaxies, as summarized in the following. There are four main categories of Active Galaxies and AGN: 1. galaxies with an excess of infrared emission and violent activity of star formation (starburst), selected in particular in the far-IR, the luminous (LIRG), ultra-luminous (ULIRG) and hyper-luminous (HYLIRG) galaxies: the 3 classes 11 12 13 have bolometric luminosities >10 L (LIRG), >10 L (ULIRG), >10 L (HYLIRG); 2.