The Physics and Cosmology of Tev Blazars

Total Page:16

File Type:pdf, Size:1020Kb

The Physics and Cosmology of Tev Blazars Blazars Gamma-ray sky Structure formation The Physics and Cosmology of TeV Blazars Christoph Pfrommer1 in collaboration with Avery E. Broderick, Phil Chang, Ewald Puchwein, Astrid Lamberts, Mohamad Shalaby, Volker Springel 1Heidelberg Institute for Theoretical Studies, Germany Jun 11, 2015 / Nonthermal Processes in Astrophysical Phenomena, Minneapolis Christoph Pfrommer The Physics and Cosmology of TeV Blazars Blazars Gamma-ray sky Structure formation Motivation A new link between high-energy astrophysics and cosmological structure formation Introduction to Blazars active galactic nuclei (AGN) propagating gamma rays plasma physics Cosmological Consequences unifying blazars with AGN gamma-ray background thermal history of the Universe Lyman-α forest formation of dwarf galaxies Christoph Pfrommer The Physics and Cosmology of TeV Blazars AGNs are among the most luminous sources in the universe → discovery of distant objects Blazars Active galactic nuclei Gamma-ray sky Propagating γ rays Structure formation Plasma instabilities Active galactic nucleus (AGN) AGN: compact region at the center of a galaxy, which dominates the luminosity of its electromagnetic spectrum AGN emission is most likely caused by mass accretion onto a supermassive black hole and can also launch relativistic jets Centaurus A Christoph Pfrommer The Physics and Cosmology of TeV Blazars Blazars Active galactic nuclei Gamma-ray sky Propagating γ rays Structure formation Plasma instabilities Active galactic nucleus at a cosmological distance AGN: compact region at the center of a galaxy, which dominates the luminosity of its electromagnetic spectrum AGN emission is most likely caused by mass accretion onto a supermassive black hole and can also launch relativistic jets AGNs are among the most luminous sources in the universe → discovery of distant objects Quasar 3C175 at z ' 0.8: jet extends 106 light years across Christoph Pfrommer The Physics and Cosmology of TeV Blazars Blazars Active galactic nuclei Gamma-ray sky Propagating γ rays Structure formation Plasma instabilities Unified model of active galactic nuclei relativistic jet accretion disk dusty torus super−massive black hole Christoph Pfrommer The Physics and Cosmology of TeV Blazars Blazars Active galactic nuclei Gamma-ray sky Propagating γ rays Structure formation Plasma instabilities Unified model of active galactic nuclei relativistic jet accretion disk dusty torus super−massive black hole Blazar: jet aligned with line-of-sight Christoph Pfrommer The Physics and Cosmology of TeV Blazars Blazars Active galactic nuclei Gamma-ray sky Propagating γ rays Structure formation Plasma instabilities TeV gamma-ray observations MAGIC VERITAS H.E.S.S. Christoph Pfrommer The Physics and Cosmology of TeV Blazars Blazars Active galactic nuclei Gamma-ray sky Propagating γ rays Structure formation Plasma instabilities The TeV gamma-ray sky There are several classes of TeV sources: Galactic - pulsars, BH binaries, supernova remnants Extragalactic - mostly blazars, two starburst galaxies Christoph Pfrommer The Physics and Cosmology of TeV Blazars Blazars Active galactic nuclei Gamma-ray sky Propagating γ rays Structure formation Plasma instabilities Annihilation and pair production blazar e− TeV e+ extragalactic backgroud light (infrared, eV) Pfrommer Christoph Pfrommer The Physics and Cosmology of TeV Blazars Blazars Active galactic nuclei Gamma-ray sky Propagating γ rays Structure formation Plasma instabilities Annihilation and pair production blazar e− TeV e+ extragalactic backgroud light (infrared, eV) Pfrommer Christoph Pfrommer The Physics and Cosmology of TeV Blazars Blazars Active galactic nuclei Gamma-ray sky Propagating γ rays Structure formation Plasma instabilities Inverse Compton cascades cosmic microwave background, 10 −3 eV − TeV blazar GeV e e+ extragalactic backgroud light (infrared, eV) Pfrommer Christoph Pfrommer The Physics and Cosmology of TeV Blazars Blazars Active galactic nuclei Gamma-ray sky Propagating γ rays Structure formation Plasma instabilities Inverse Compton cascades cosmic microwave background, 10 −3 eV − TeV blazar GeV e e+ extragalactic backgroud light (infrared, eV) each TeV point source should also be a GeV point source! Pfrommer Christoph Pfrommer The Physics and Cosmology of TeV Blazars – not seen! Blazars Active galactic nuclei Gamma-ray sky Propagating γ rays Structure formation Plasma instabilities What about the cascade emission? Every TeV source should be associated with a 1-100 GeV gamma-ray halo expected cascade TeV detections emission intrinsic spectra Neronov & Vovk (2010) Christoph Pfrommer The Physics and Cosmology of TeV Blazars Blazars Active galactic nuclei Gamma-ray sky Propagating γ rays Structure formation Plasma instabilities What about the cascade emission? Every TeV source should be associated with a 1-100 GeV gamma-ray halo – not seen! expected cascade TeV detections emission intrinsic spectra Fermi exclusion region Neronov & Vovk (2010) Christoph Pfrommer The Physics and Cosmology of TeV Blazars Blazars Active galactic nuclei Gamma-ray sky Propagating γ rays Structure formation Plasma instabilities Inverse Compton cascades cosmic microwave background, 10 −3 eV − TeV blazar GeV e e+ extragalactic backgroud light (infrared, eV) Pfrommer Christoph Pfrommer The Physics and Cosmology of TeV Blazars Blazars Active galactic nuclei Gamma-ray sky Propagating γ rays Structure formation Plasma instabilities Extragalactic magnetic fields? pair deflection in intergalactic magnetic field blazar e− TeV GeV e+ extragalactic backgroud light (infrared, eV) Pfrommer Christoph Pfrommer The Physics and Cosmology of TeV Blazars Blazars Active galactic nuclei Gamma-ray sky Propagating γ rays Structure formation Plasma instabilities Extragalactic magnetic fields? pair deflection in intergalactic magnetic field blazar e− TeV GeV e+ extragalactic backgroud light (infrared, eV) GeV point source diluted weak "pair halo" stronger B−field implies more deflection and dilution, gamma−ray non−detection −Pfrommer primordial fields? Christoph Pfrommer The Physics and Cosmology of TeV Blazars Blazars Active galactic nuclei Gamma-ray sky Propagating γ rays Structure formation Plasma instabilities Extragalactic magnetic fields? pair deflection in intergalactic magnetic field blazar e− TeV GeV e+ extragalactic backgroud light (infrared, eV) problem for unified AGN model: no increase in comoving blazar density with redshift allowed (as seen in other AGNs) since other− wise, extragalactic GeV background would be overproduced!Pfrommer Christoph Pfrommer The Physics and Cosmology of TeV Blazars Blazars Active galactic nuclei Gamma-ray sky Propagating γ rays Structure formation Plasma instabilities What else could happen? blazar e− TeV e+ extragalactic backgroud light (infrared, eV) Pfrommer Christoph Pfrommer The Physics and Cosmology of TeV Blazars Blazars Active galactic nuclei Gamma-ray sky Propagating γ rays Structure formation Plasma instabilities Plasma instabilities intergalactic medium blazar e− TeV e+ pair plasma beam propagating through the intergalactic medium Pfrommer Christoph Pfrommer The Physics and Cosmology of TeV Blazars Blazars Active galactic nuclei Gamma-ray sky Propagating γ rays Structure formation Plasma instabilities Plasma instabilities pair beam intergalactic medium (IGM) this configuration is unstable to plasma instabilities characteristic frequency and length scale of the problem: s 2 4πe ne c 8 ωp = , λp = ∼ 10 cm me ωp ρ¯(z=0) Christoph Pfrommer The Physics and Cosmology of TeV Blazars Blazars Active galactic nuclei Gamma-ray sky Propagating γ rays Structure formation Plasma instabilities Two-stream instability consider wave-like perturbation in background plasma along the beam direction (Langmuir wave): initially homogeneous beam-e−: attractive (repulsive) force by potential maxima (minima) e− attain lowest velocity in potential minima → bunching up e+ attain lowest velocity in potential maxima → bunching up Φ + p p e− e − Christoph Pfrommer The Physics and Cosmology of TeV Blazars Blazars Active galactic nuclei Gamma-ray sky Propagating γ rays Structure formation Plasma instabilities Two-stream instability consider wave-like perturbation in background plasma along the beam direction (Langmuir wave): beam-e+/e− couple in phase with the background perturbation: enhances background potential stronger forces on beam-e+/e− → positive feedback exponential wave-growth → instability e+ e+ Φ + p p e− e− e− e − Christoph Pfrommer The Physics and Cosmology of TeV Blazars Blazars Active galactic nuclei Gamma-ray sky Propagating γ rays Structure formation Plasma instabilities Two-stream instability: momentum transfer particles with v & vphase: pair momentum → plasma waves → growing modes: instability particles with v . vphase: plasma wave momentum → pairs → Landau damping Christoph Pfrommer The Physics and Cosmology of TeV Blazars Blazars Active galactic nuclei Gamma-ray sky Propagating γ rays Structure formation Plasma instabilities Oblique instability k oblique to v beam: real word perturbations don’t choose “easy” alignment = P all orientations oblique grows faster than two-stream: E-fields can easier deflect ultra-relativistic particles than change their parallel velocities (Nakar, Bret & Milosavljevic 2011) Bret (2009), Bret+ (2010) Christoph Pfrommer The Physics and Cosmology of TeV Blazars Blazars Active galactic nuclei Gamma-ray sky Propagating γ rays Structure formation Plasma instabilities Beam physics – growth rates excluded for collective consider a light beam plasma phenomena
Recommended publications
  • 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=">AAACOXicbVDLSgMxFM34tr6qLt0Ei+BC64wK6kIoPtCNUMU+oNOWTJq2wWRmSO4IZZjfcuNfuBPcuFDErT9g+hC09UC4h3PvJeceLxRcg20/W2PjE5NT0zOzqbn5hcWl9PJKUQeRoqxAAxGoskc0E9xnBeAgWDlUjEhPsJJ3d9rtl+6Z0jzwb6ETsqokLZ83OSVgpHo6754xAQSf111JoK1kTChN8DG+uJI7N6buYRe4ZBo7di129hJ362ew5NJGAFjjfm3V4m0nSerpjJ21e8CjxBmQDBogX08/uY2ARpL5QAXRuuLYIVRjooBTwZKUG2kWEnpHWqxiqE+MmWrcuzzBG0Zp4GagzPMB99TfGzGRWnekZya7rvVwryv+16tE0DysxtwPI2A+7X/UjASGAHdjxA2uGAXRMYRQxY1XTNtEEQom7JQJwRk+eZQUd7POfvboej+TOxnEMYPW0DraRA46QDl0ifKogCh6QC/oDb1bj9ar9WF99kfHrMHOKvoD6+sbuhSrIw==</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−
    [Show full text]
  • Messier Objects
    Messier Objects From the Stocker Astroscience Center at Florida International University Miami Florida The Messier Project Main contributors: • Daniel Puentes • Steven Revesz • Bobby Martinez Charles Messier • Gabriel Salazar • Riya Gandhi • Dr. James Webb – Director, Stocker Astroscience center • All images reduced and combined using MIRA image processing software. (Mirametrics) What are Messier Objects? • Messier objects are a list of astronomical sources compiled by Charles Messier, an 18th and early 19th century astronomer. He created a list of distracting objects to avoid while comet hunting. This list now contains over 110 objects, many of which are the most famous astronomical bodies known. The list contains planetary nebula, star clusters, and other galaxies. - Bobby Martinez The Telescope The telescope used to take these images is an Astronomical Consultants and Equipment (ACE) 24- inch (0.61-meter) Ritchey-Chretien reflecting telescope. It has a focal ratio of F6.2 and is supported on a structure independent of the building that houses it. It is equipped with a Finger Lakes 1kx1k CCD camera cooled to -30o C at the Cassegrain focus. It is equipped with dual filter wheels, the first containing UBVRI scientific filters and the second RGBL color filters. Messier 1 Found 6,500 light years away in the constellation of Taurus, the Crab Nebula (known as M1) is a supernova remnant. The original supernova that formed the crab nebula was observed by Chinese, Japanese and Arab astronomers in 1054 AD as an incredibly bright “Guest star” which was visible for over twenty-two months. The supernova that produced the Crab Nebula is thought to have been an evolved star roughly ten times more massive than the Sun.
    [Show full text]
  • Gamma-Ray and Neutrino Signals from Accretion Disk Coronae of Active Galactic Nuclei
    galaxies Review Gamma-ray and Neutrino Signals from Accretion Disk Coronae of Active Galactic Nuclei Yoshiyuki Inoue 1,2,3,* , Dmitry Khangulyan 4 and Akihiro Doi 5,6 1 Department of Earth and Space Science, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan 2 Interdisciplinary Theoretical & Mathematical Science Program (iTHEMS), RIKEN, 2-1 Hirosawa, Saitama 351-0198, Japan 3 Kavli Institute for the Physics and Mathematics of the Universe (WPI), The University of Tokyo, Kashiwa 277-8583, Japan 4 Department of Physics, Rikkyo University, Nishi-Ikebukuro 3-34-1, Toshima-ku, Tokyo 171-8501, Japan; [email protected] 5 Institute of Space and Astronautical Science JAXA, 3-1-1 Yoshinodai, Chuo-ku, Sagamihara, Kanagawa 252-5210, Japan; [email protected] 6 Department of Space and Astronautical Science, The Graduate University for Advanced Studies (SOKENDAI), 3-1-1 Yoshinodai, Chuou-ku, Sagamihara, Kanagawa 252-5210, Japan * Correspondence: [email protected] Abstract: To explain the X-ray spectra of active galactic nuclei (AGN), non-thermal activity in AGN coronae such as pair cascade models has been extensively discussed in the past literature. Although X-ray and Gamma-ray observations in the 1990s disfavored such pair cascade models, recent millimeter-wave observations of nearby Seyferts have established the existence of weak non-thermal coronal activity. In addition, the IceCube collaboration reported NGC 1068, a nearby Seyfert, as the hottest spot in their 10 year survey. These pieces of evidence are enough to investigate the non-thermal perspective of AGN coronae in depth again. This article summarizes our current Citation: Inoue, Y.; Khangulyan, D.; observational understanding of AGN coronae and describes how AGN coronae generate high-energy Doi, A.
    [Show full text]
  • Positron Annihilation Spectroscopy of Active Galactic Nuclei
    Research Paper J. Astron. Space Sci. 36(1), 21-33 (2019) https://doi.org/10.5140/JASS.2019.36.1.21 Positron Annihilation Spectroscopy of Active Galactic Nuclei Dmytry N. Doikov1, Alexander V. Yushchenko2, Yeuncheol Jeong3† 1Odessa National Maritime University, Department of Mathematics, Physics and Astronomy, Odessa, 65029, Ukraine 2Astrocamp Contents Research Institute, Goyang, 10329, Korea 3Daeyang Humanity College, Sejong University, Seoul, 05006, Korea This paper focuses on the interpretation of radiation fluxes from active galactic nuclei. The advantage of positron annihilation spectroscopy over other methods of spectral diagnostics of active galactic nuclei (therefore AGN) is demonstrated. A relationship between regular and random components in both bolometric and spectral composition of fluxes of quanta and particles generated in AGN is found. We consider their diffuse component separately and also detect radiative feedback after the passage of high-velocity cosmic rays and hard quanta through gas-and-dust aggregates surrounding massive black holes in AGN. The motion of relativistic positrons and electrons in such complex systems produces secondary radiation throughout the whole investigated region of active galactic nuclei in form of cylinder with radius R= 400-1000 pc and height H=200-400 pc, thus causing their visible luminescence across all spectral bands. We obtain radiation and electron energy distribution functions depending on the spatial distribution of the investigated bulk of matter in AGN. Radiation luminescence of the non- central part of AGN is a response to the effects of particles and quanta falling from its center created by atoms, molecules and dust of its diffuse component. The cross-sections for the single-photon annihilation of positrons of different energies with atoms in these active galactic nuclei are determined.
    [Show full text]
  • Active Galactic Nuclei - Suzy Collin, Bożena Czerny
    ASTRONOMY AND ASTROPHYSICS - Active Galactic Nuclei - Suzy Collin, Bożena Czerny ACTIVE GALACTIC NUCLEI Suzy Collin LUTH, Observatoire de Paris, CNRS, Université Paris Diderot; 5 Place Jules Janssen, 92190 Meudon, France Bożena Czerny N. Copernicus Astronomical Centre, Bartycka 18, 00-716 Warsaw, Poland Keywords: quasars, Active Galactic Nuclei, Black holes, galaxies, evolution Content 1. Historical aspects 1.1. Prehistory 1.2. After the Discovery of Quasars 1.3. Accretion Onto Supermassive Black Holes: Why It Works So Well? 2. The emission properties of radio-quiet quasars and AGN 2.1. The Broad Band Spectrum: The “Accretion Emission" 2.2. Optical, Ultraviolet, and X-Ray Emission Lines 2.3. Ultraviolet and X-Ray Absorption Lines: The Wind 2.4. Variability 3. Related objects and Unification Scheme 3.1. The “zoo" of AGN 3.2. The “Line of View" Unification: Radio Galaxies and Radio-Loud Quasars, Blazars, Seyfert 1 and 2 3.2.1. Radio Loud Quasars and AGN: The Jet and the Gamma Ray Emission 3.3. Towards Unification of Radio-Loud and Radio-Quiet Objects? 3.4. The “Accretion Rate" Unification: Low and High Luminosity AGN 4. Evolution of black holes 4.1. Supermassive Black Holes in Quasars and AGN 4.2. Supermassive Black Holes in Quiescent Galaxies 5. Linking the growth of black holes to galaxy evolution 6. Conclusions Acknowledgements GlossaryUNESCO – EOLSS Bibliography Biographical Sketches SAMPLE CHAPTERS Summary We recall the discovery of quasars and the long time it took (about 15 years) to build a theoretical framework for these objects, as well as for their local less luminous counterparts, Active Galactic Nuclei (AGN).
    [Show full text]
  • On the Time Scales of Optical Variability of AGN and the Shape of Their Optical Emission Line Profiles
    atoms Article On the Time Scales of Optical Variability of AGN and the Shape of Their Optical Emission Line Profiles Edi Bon 1,* , Paola Marziani 2, Predrag Jovanovi´c 1 and Nataša Bon 1,2 1 Astronomical Observatory, Volgina 7, 11060 Belgrade, Serbia; [email protected] (P.J.); [email protected] (N.B.) 2 National Institute for Astrophysics (INAF), Astronomical Observatory of Padova, IT 35122 Padova, Italy; [email protected] * Correspondence: [email protected] Received: 8 December 2018; Accepted: 6 February 2019; Published: 14 February 2019 Abstract: The mechanism of the optical variability of active galactic nuclei (AGN) is still very puzzling. It is now widely accepted that the optical variability of AGN is stochastic, producing red noise-like light curves. In case they were to be periodic or quasi-periodic, one should expect that the time scales of optical AGN variability should relate to orbiting time scales of regions inside the accretion disks with temperatures mainly emitting the light in this wavelength range. Knowing the reverberation scales and masses of AGN, expected orbiting time scales are in the order of decades. Unfortunately, most of monitored AGN light curves are not long enough to investigate such time scales of periodicity. Here we investigate the AGN optical variability time scales and their possible connections with the broad emission line shapes. Keywords: AGN; black holes; gravitational waves; binary black holes; quasars 1. Introduction Active galactic nuclei (AGN) are very strong and variable emitters [1]. It is widely believed that the AGN patterns correspond to red noise-like curves [2,3], as a result of unpredicted processes of fluctuations of their accretion disks (AD).
    [Show full text]
  • AGN Radiative Feedback in the Early Growth of Massive Black Holes
    Mon. Not. R. Astron. Soc. 000, 1{6 (2012) Printed 25 September 2019 (MN LATEX style file v2.2) AGN radiative feedback in the early growth of massive black holes W. Ishibashi1? 1Physik-Institut, Universitat Zurich, Winterthurerstrasse 190, 8057 Zurich, Switzerland Accepted ? Received ?; in original form ? ABSTRACT Growing observational evidence confirms the existence of massive black holes (MBH ∼ 9 10 M ), accreting at rates close to the Eddington limit, at very high redshifts (z & 6 − 7) in the early Universe. Recent observations indicate that the host galax- ies of the first quasars are chemically evolved systems, containing unexpectedly large amounts of dust. Such a combination of high luminosities and large dust content should form favourable physical conditions for radiative dusty feedback. We explore the impact of the active galactic nucleus (AGN) feedback, driven by radiation pressure on dust, on the early growth of massive black holes. Assuming Eddington-limited ex- ponential black hole growth, we find that the dynamics and energetics of the radiation pressure-driven outflows also follow exponential trends at late times. We obtain mod- _ −3 est outflow energetics (with momentum fluxp _ . L=c and kinetic power Ek . 10 L), comparable with available observations of quasar-driven outflows at very high red- shifts, but significantly lower than typically observed in local quasars and predicted by wind energy-driven models. AGN radiative dusty feedback may thus play an im- portant role in powering galactic outflows in the first quasars in the early Universe. Key words: black hole physics - galaxies: active - galaxies: evolution 1 INTRODUCTION and/or several super-Eddington accretion episodes are re- quired, while the constraints may be slightly relaxed in the Observations over the past years have revealed the existence case of heavy seeds.
    [Show full text]
  • The Unique Potential of Extreme Mass-Ratio Inspirals for Gravitational-Wave Astronomy 1, 2 3, 4 Christopher P
    Main Thematic Area: Formation and Evolution of Compact Objects Secondary Thematic Areas: Cosmology and Fundamental Physics, Galaxy Evolution Astro2020 Science White Paper: The unique potential of extreme mass-ratio inspirals for gravitational-wave astronomy 1, 2 3, 4 Christopher P. L. Berry, ∗ Scott A. Hughes, Carlos F. Sopuerta, Alvin J. K. Chua,5 Anna Heffernan,6 Kelly Holley-Bockelmann,7 Deyan P. Mihaylov,8 M. Coleman Miller,9 and Alberto Sesana10, 11 1CIERA, Northwestern University, 2145 Sheridan Road, Evanston, IL 60208, USA 2Department of Physics and MIT Kavli Institute, Massachusetts Institute of Technology, Cambridge, MA 02139, USA 3Institut de Ciencies` de l’Espai (ICE, CSIC), Campus UAB, Carrer de Can Magrans s/n, 08193 Cerdanyola del Valles,` Spain 4Institut d’Estudis Espacials de Catalunya (IEEC), Edifici Nexus I, Carrer del Gran Capita` 2-4, despatx 201, 08034 Barcelona, Spain 5Jet Propulsion Laboratory, California Institute of Technology, 4800 Oak Grove Drive, Pasadena, CA 91109, USA 6School of Mathematics and Statistics, University College Dublin, Belfield, Dublin 4, Ireland 7Department of Physics and Astronomy, Vanderbilt University and Fisk University, Nashville, TN 37235, USA 8Institute of Astronomy, University of Cambridge, Madingley Road, Cambridge, CB3 0HA, UK 9Department of Astronomy and Joint Space-Science Institute, University of Maryland, College Park, MD 20742-2421, USA 10School of Physics & Astronomy and Institute for Gravitational Wave Astronomy, University of Birmingham, Edgbaston, Birmingham B15 2TT, UK 11Universita` di Milano Bicocca, Dipartimento di Fisica G. Occhialini, Piazza della Scienza 3, I-20126, Milano, Italy (Dated: March 7, 2019) The inspiral of a stellar-mass compact object into a massive ( 104–107M ) black hole ∼ produces an intricate gravitational-wave signal.
    [Show full text]
  • Alessandro Marconi Department of Physics and Astronomy University of Florence
    Active Galactic Nuclei Alessandro Marconi Department of Physics and Astronomy University of Florence Challenges in UV Astronomy, ESO Garching, 7-11 October 2013 Outline A brief introduction to Active Galactic Nuclei (or ... accreting supermassive black holes) Coevolution of black holes and host galaxies Open questions: seeking answers in near-UV spectroscopy A. Marconi Challenges in UV Astronomy, ESO Garching 2 Outline A brief introduction to Active Galactic Nuclei (or ... accreting supermassive black holes) Coevolution of black holes and host galaxies Open questions: seeking answers in near-UV spectroscopy A. Marconi Challenges in UV Astronomy, ESO Garching 3 AGN in a nutshell An Active Galactic Nucleus (AGN) is a galaxy nucleus with indications non-stellar activity (L~1011-1015 L☉ , non-stellar continuum, prominent emission lines, jets of relativistic material, strong and fast variability) Many observational classes: Quasars, Seyfert galaxies, radio gal., etc. Radio MicrowavesMicroonde Infrarosso Infrared Visibile Visible UV raggiX-rays X [Å] 47 6000 4000 2000 46.0 46 45.5 Nucleo AGN Attivo 45 14.8 15.0 ) [erg/s] SpiralSpirale [Å] L 44 6000 4000 2000 45.0 log( 44.5 43 44.0 43.5 42 EllipticalEllittica 43.0 14.8 15.0 41 10 12 14 16 18 log() [Hz] 472 ZHENG ET AL. Vol. 475 corresponding wavelength range. The sum of the normal- lar, yield signi–cant *s2 because of the very high S/N level. ized spectra was smoother than the template at shorter Therefore, the selected windows at long wavelengths are wavelengths where the S/N level was lower, and it serves as narrow.
    [Show full text]
  • Arp 299-A (D=45 Mpc), Showing ∼ † ∗ [email protected] Speaker
    Arp 299: The show must go on! PoS(11th EVN Symposium)002 Miguel Pérez-Torres∗ † IAA-CSIC, Glorieta de la Astronomía s/n, 18008 Granada, Spain E-mail: [email protected] Luminous and Ultra-Luminous Infrared Galaxies (U/LIRGs) are also strong emitters of both ther- mal (free-free) and non-thermal (mainly synchrotron) radio emission. This is very handy since, unlike optical and infra-red observations, radio is not obscured by the ubiquitous dust present in U/LIRGs, which allows a direct view of the ongoing activity inside those prolific star-forming galaxies. In this talk, I present some selected results on what is probably the most spectacular supernova factory in a nearby LIRG, Arp 299. Namely, I show (i) the impressive discovery of an extremely prolific supernova factory in the central ∼150 pc of the galaxy Arp 299-A (D=45 Mpc), showing that essentially all core-collapse supernovae explode in the central 150 pc of the galaxy, (ii) the detection and precise location of the long-sought AGN in Arp 299-A, and (iii) the monitoring of the compact sources in Arp 299-A. A movie summarizing those findings can be found in the fol- lowing URL: http://www.iaa.es/ torres/research/arp299a.html. All those results demonstrate that very-high angular resolution studies of nearby U/LIRGs are of high relevance for the comprehen- sion of both local and high-z starbursting galaxies, and that Arp 299 stands itself as a fundamental piece of such studies. 11th European VLBI Network Symposium & Users Meeting, October 9-12, 2012 Bordeaux, France ∗Speaker.
    [Show full text]
  • Elisa/NGO, Revealing a Hidden Universe Notes & News for GW
    GW Notes Special Issue: eLISA/NGO, revealing a hidden universe Notes & News for GW science Guest editors: David Spergel and Zhang Shuangnan Editors: Pau Amaro-Seoane and Bernard F. Schutz ISSN: 1868-1921 GW Notes was born from the need for a journal where the distinct communities in- volved in gravitational wave research might gather. While these three communities - Astrophysics, General Relativity and Data Analysis - have made significant collabora- tive progress over recent years, we believe that it is indispensable to future advancement that they draw closer, and that they speak a common idiom. Notes & News for GW science 1 Publisher: Max-Planck-Institut für Gravitationsphysik (Albert-Einstein-Institut) Am Mühlenberg 1 14476 Potsdam Germany Editors: P. Amaro Seoane and B.F. Schutz ISSN: 1868-1921 URL: http://brownbag.lisascience.org/lisa-gw-notes/ Notes & News for GW science #6 May 28, 2013 GW Notes 1 Notes & News for GW science eLISA/NGO: Revealing a hidden universe Editorial Prof. A. Lobo As you proably know, Prof. José Alberto Lobo Gutiérrez passed away last September 30 2012. He left behind a wife (Rosa Maria), a son (Albert), and a daughter (Montser- rat). Prof. Lobo has been a pioneer of the field of Gravitational Wave Astronomy in Spain, devoting his life to resonant ground-based detectors and to space-based ones. His contributions range from theoretical studies to the development of instrumen- tation, including data analysis methods. Even in the final stages of his cancer, he was mainly concerned and actively planning towards maintaining and promoting Notes & News for GW science the Spanish team activities and involvement into LISA PathFinder and its successor mission LISA.
    [Show full text]
  • Mining the VLA Archives for Radio Transients
    AMERICAN JOURNAL OF UNDERGRADUATE RESEARCH VOL. 5, NO. 2 (2006) Looking for the Elusive: Mining the VLA Archives for Radio Transients Destry R. Saul and Geoffrey C. Bower Astronomy Department and Radio Astronomy Laboratory University of California - Berkeley 601 Campbell Hall Berkeley, California 94720 USA Received: June 7, 2006 Accepted: July 24, 2006 ABSTRACT Detecting extragalactic radio transients will provide valuable information on several astronomical phenomena. Orphan gamma-ray burst afterglows (OGRBAs) and radio supernovae detection will be important for the theories of stellar collapse while the detection of tidal flares and variable active galactic nuclei (AGN) will provide details on massive black holes and galactic centers. In this paper we present the results of a survey we conducted using archived observations from the Very Large Array (VLA). We did not detect any transients in this set of data and from this we computed an upper limit on the rate of radio transients above 400 μJansky at 0.23 transients per square degree per year. This rules out one of several theories on the rates of OGRBAs. I. INTRODUCTION transients of 0.23 per square degree per year above 400 μJy.* This value agrees Transient radio sources are objects that did with some models and disagrees with not previously radiate detectably in the radio others. We will discuss our results in Section spectrum, but then begin to emit for a period III. of time, and then fade away. Of the several classes of predicted extragalactic radio a. A Brief Introduction to Extragalactic transients, only radio supernova explosions Radio Transient Theories and gamma-ray burst afterglows have been confirmed.
    [Show full text]