Cosmological parameters with radio galaxies

Slides:



Advertisements
Similar presentations
An Experience of Aladin Usage for the RC Catalog Radio Source Investigation Zhelenkova Olga, SAO RAS.
Advertisements

Spitzer Observations of 3C Quasars and Radio Galaxies: Mid-Infrared Properties of Powerful Radio Sources K. Cleary 1, C.R. Lawrence 1, J.A. Marshall 2,
Copyright © 2010 Pearson Education, Inc. Chapter 16 Galaxies and Dark Matter.
“Do I have your attention…?”
Particle Astrophysics & Cosmology SS Chapter 7 Dark Matter.
PRESENTATION TOPIC  DARK MATTER &DARK ENERGY.  We know about only normal matter which is only 5% of the composition of universe and the rest is  DARK.
Star formation at high redshift (2 < z < 7) Methods for deriving star formation rates UV continuum = ionizing photons (dust obscuration?) Ly  = ionizing.
Galaxies Types Dark Matter Active Galaxies Galaxy Clusters & Gravitational Lensing.
Galaxies with Active Nuclei Chapter 17. You can imagine galaxies rotating slowly and quietly making new stars as the eons pass, but the nuclei of some.
PRE-SUSY Karlsruhe July 2007 Rocky Kolb The University of Chicago Cosmology 101 Rocky I : The Universe Observed Rocky II :Dark Matter Rocky III :Dark Energy.
Galaxies What is a galaxy? How many stars are there in an average galaxy? About how many galaxies are there in the universe? What is the name of our galaxy?
A Primer on SZ Surveys Gil Holder Institute for Advanced Study.
GALAXY FORMATION AND EVOLUTION - 2. DISCOVER Magazine’s 2007 Scientist of the Year David Charbonneau, of the Harvard-Smithsonian Canter for Astrophysics.
Dusty star formation at high redshift Chris Willott, HIA/NRC 1. Introductory cosmology 2. Obscured galaxy formation: the view with current facilities,
Program 1.The standard cosmological model 2.The observed universe 3.Inflation. Neutrinos in cosmology.
Active Galactic Nuclei Ay 16, April 8, AGN DEFINITION PROPERTIES GRAVITATIONAL LENSES BLACK HOLES MODELS.
Chapter 31 Galaxies & the Universe Review & Recap It does this by precisely measuring the speed of gas and stars around a black hole. This provides clues.
Review for Exam 3.
Quasars and Other Active Galaxies
Modelling radio galaxies in simulations: CMB contaminants and SKA / Meerkat sources by Fidy A. RAMAMONJISOA MSc Project University of the Western Cape.
Galaxy Characteristics Surface Brightness Alternative to Luminosity I(R) = Flux/area = erg/s/cm 2 /arcsec 2 I(0) – center flux I(R) = at radius R Define.
Galaxies and the Universe
Imaging Compact Supermassive Binary Black Holes with VLBI G. B. Taylor (UNM), C. Rodriguez (UNM), R. T. Zavala (USNO) A. B. Peck (CfA), L. K. Pollack (UCSC),
THE HST VIEW OF LINERS AND OTHER LOCAL AGN MARCO CHIABERGE CNR - Istituto di Radioastronomia - Bologna Alessandro Capetti (INAF-OATo) Duccio Macchetto.
Introduction to the modern observational cosmology Introduction/Overview.
Cosmology. We can simulate how a nearly smooth distribution of dark matter turns into our lumpy, grainy Universe with its hierarchy of structures -
SUNYAEV-ZELDOVICH EFFECT. OUTLINE  What is SZE  What Can we learn from SZE  SZE Cluster Surveys  Experimental Issues  SZ Surveys are coming: What.
THEORETICAL ASTROPHYSICS AND THE US-NVO INITIATIVE D. S. De Young National Optical Astronomy Observatory.
PHY306 1 Modern cosmology 3: The Growth of Structure Growth of structure in an expanding universe The Jeans length Dark matter Large scale structure simulations.
FRI RADIO GALAXIES AT z > 1 STUDYING THE BUILDING BLOCKS OF TODAY'S MOST MASSIVE GALAXIES AND CLUSTERS Marco Chiaberge Space Telescope Science Institute.
Racah Institute of physics, Hebrew University (Jerusalem, Israel)
Announcements The final exam will be at Noon on Monday, December 13 in Van Allen Hall LR1. Practice questions for unit #5 are available on the class web.
Galaxies with Active Nuclei Chapter 14:. Active Galaxies Galaxies with extremely violent energy release in their nuclei (pl. of nucleus).  “active galactic.
Quasars and Other Active Galaxies
ALMA and the Formation of Galaxies Pierre Cox IAS, Orsay, France.
USING LOW POWER RADIO GALAXIES AS BEACONS FOR CLUSTERS AT 1
Copyright © 2010 Pearson Education, Inc. Chapter 16 Galaxies and Dark Matter Lecture Outline.
Radio Galaxies part 4. Apart from the radio the thin accretion disk around the AGN produces optical, UV, X-ray radiation The optical spectrum emitted.
The Dark Age and Cosmology Xuelei Chen ( 陈学雷 ) National Astronomical Observarories of China The 2nd Sino-French Workshop on the Dark Universe, Aug 31st.
KASI Galaxy Evolution Journal Club A Massive Protocluster of Galaxies at a Redshift of z ~ P. L. Capak et al. 2011, Nature, in press (arXive: )
Probing Dark Energy with Cosmological Observations Fan, Zuhui ( 范祖辉 ) Dept. of Astronomy Peking University.
Chapter 25 Galaxies and Dark Matter. 25.1Dark Matter in the Universe 25.2Galaxy Collisions 25.3Galaxy Formation and Evolution 25.4Black Holes in Galaxies.
Active Galaxies Galaxies with extremely violent energy release in their nuclei (pl. of nucleus). → “Active Galactic Nuclei” (= AGN) Up to many thousand.
“Globular” Clusters: M15: A globular cluster containing about 1 million (old) stars. distance = 10,000 pc radius  25 pc “turn-off age”  12 billion years.
Chapter 20 Cosmology. Hubble Ultra Deep Field Galaxies and Cosmology A galaxy’s age, its distance, and the age of the universe are all closely related.
A single galaxy with its millions or billions of stars is only a very small spot in the observable universe. Galaxies & AGN’s (Chapter 13) Hercules Cluster.
Galaxies with Active Nuclei
Thomas Collett Institute of Astronomy, Cambridge
Note that the following lectures include animations and PowerPoint effects such as fly ins and transitions that require you to be in PowerPoint's Slide.
Announcements Grades for third exam are now available on WebCT
EVOLUTION OF LUMINOSITY-LINEAR SIZE RELATION
Thomas Collett Institute of Astronomy, Cambridge
Chapter 25 Active Galaxies and Quasars
Molecular gas in cooling flows Interplay with AGN and starbursts
Multi range study of the radio sources of the RATAN-600 surveys
Cosmology with Supernovae
Paul Alexander Dave Green, Malcolm Longair, Julia Riley, Martin Krause
Chapter 16 Active Galaxy.
1.4 GHz Source Counts (Hopkins 2000)
© 2017 Pearson Education, Inc.
The origin nuclear X-ray emission in the nuclei of radio galaxy-FR Is
A Search for water masers in High-redshift un-beamed AGNs: T. Ghosh, S
Galaxies With Active Nuclei
ACTIVE GALAXIES and GALAXY EVOLUTION
Quasars and Active Galactic Nuclei
Note that the following lectures include animations and PowerPoint effects such as fly ins and transitions that require you to be in PowerPoint's Slide.
Galaxies With Active Nuclei
Yuan Liu and Shuang Nan Zhang
Dark matter and anomalous gas in the spiral galaxy NGC 4559
Galaxies With Active Nuclei
Presentation transcript:

Cosmological parameters with radio galaxies Oleg Verkhodanov Special astrophysical observator Nizhnij Arkhyz

Radio cosmology Dark ages

Radio galaxies - galaxies with radio power mostly due to nucleus activity Power of emission is up to 10^48 erg/s

What are the radio galaxies ?

Cygnus A E-galaxy m=16 z = 0.057, theta~2' (80 kpc), v = 0.02c, P= 3x10^44 erg/s

Centaurus A (NGC 5128) P = 10^42 erg/s, d = 12 kpc

Virgo A (NGC 4486, M87) cD-galaxy 20'' (1.5 kpc) optical jet

Radio galaxies identified with gE or cD galaxies and should be visible in optics and radio waves from very beginning (z<~6)

2 basic morphological types of RG Fanaroff – Riley I Fanaroff – Riley II

Unified model

Continuum radio galaxy spectra alpha S~nu Steep spectrum: alpha<-0.5

Radio galaxies as Universe reference point The most distant radio galaxy: z=5.19 (van Breugel et al., 1999)

Distribution of radio galaxies for Cambridge catalogs (Cruz et al., 2007)

Cosmology with radio galaxies a) “size – redshift” (standard rod) b) “luminosity – redshift” (standard candle) c) ''Log N – Log S'' (“source number – flux density”) d) Gravitational lensing e) Clustering and large stellar structure forming f) Age of stellar systems g) Black hole formation at high redshift h) Dark matter search in halos What is good ? (probably, we know) 1) Universe expands, accelerating; 2) There are CMB radiation and its angular fluctuations; 3) elements in Universe.

Radio galaxies and large scale structure

''Size – redshift'' diagram for radio sources and CMB (Jackson, Janneta, 2006)

Gravitational lenses Einstein ring (RC 1131+0456) B 1938+666

Source counts: Log N – Log S FR II: 1) FRII & QSR, alp<-0.5 2) QSR with flat Sp 3) RG, BL Lac, FR I: 6) BL Lac,  7) Starburst galaxies (Jackson, Wall, 1999)

“Big Trio” Program RATAN-600 VLA BTA

“Big Trio” program 1) Radio sources of the “Cold” survey ( >10 mJy at 7.6 cm) 2) Steep radio spectrum (synchrotron) selection 3) VLA (radio): morphology selection (FR II) 4) 6m telescope (optics): identification, BVRI-photometry, spectrosopy (redshift) 5) Age estimation

“Big Trio” program

Age of radio galaxies

Giant elliptical galaxies with old stellar population ==> photometrical study and existance at very high z ~4 (Pipino & Mantteucci, 2004). selection of distant gE (z>0.5) with radio galaxies ==> by radio astronomical methods (Pedani, 2003).

Estimation of stellar and galaxy age by thermal nuclear reactions - independent test for Universe expansion

Sample of 220 objects with 3 subsamples: (1) Famous radio galaxies FR II (1<z<4): initially 300 RGs (NED) ---> resulting 30 FRII (2) RGs of FR II from the “Cold” survey (“Big Trio”: Parijskij et al., 1990-2003), (3) Elliptical galaxies from clusters (Stanford, 2002) (0.1<z<1.3)

(Verkhodanov, Parijskij, Starobinsky, 2005) Approximation of t(z) with integral curve and detection of H_o и Omega_Lambda (Verkhodanov, Parijskij, Starobinsky, 2005) Sample binning dz=0.2 и dz=0.3 Take maximum in each bin

Two models of synthetic spectra

Age [Myr] Redshift z Age [Myr] Redshift z

Possible errors metalicity: error ~100 Myr (Jimenez, Loeb, 2002) initial mass function has low influence (Bolzonella et al., 2001), error in galaxy type detection, incomplete sample: robust detection Bootstrap method: mutiplication coefficient 100, variation of H_o ~ 10%

Model dz Om_mOm_L H_o epsilon SED [Myr] GISSEL 0.2 0.2 0.8 78 1695 GISSEL 0.3 0.2 0.8 72 1367 PEGASE 0.2 0.2 0.8 65 4101 PEGASE 0.3 0.2 0.8 53 2748 H_o = 72 +/- 10 Om_L = 0.8 +/- 0.1, not exelent, but satisfys the model

What is further ? 2) Combining different methods 1) Select ALL the distant RGs and typical close gEs 2) Combining different methods

z = 4.514 (Kopylov et al., 2006) The 2nd RG by z, the 1st RG by power among RGs, z>4

Thank you for hospitality !