Yuan Liu and Shuang Nan Zhang

Slides:



Advertisements
Similar presentations
AGN Eddington Ratio Distributions
Advertisements

Method To determine the multiplicity parameter and the magnetization parameter  one can use the dependence on the visible position of the core of the.
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,
1/26 Introduction 1/28 Radio Loud AGN Unification: Connecting Jets and Accretion Eileen Meyer Space Telescope Science Institute Giovanni Fossati, Rice.
The Accretion Mode - Morphology Link in Radio-Loud AGN jets: Towards a More Complete Unification Scheme Eileen Meyer Rice University University of Maryland,
Weighing black holes in radio-loud AGNs
Active Galactic Nuclei Chapter 28 Revised Active Galactic Nuclei Come in several varieties; Starburst Nuclei – Nearby normal galaxies with unusually.
Jets from Active Galactic Nuclei: Observations and Models
Kinematics of Jets of Gamma-Ray Blazars from VLBA Monitoring at 43 GHz Svetlana Jorstad Boston University, USA St.Petersburg State University, Russia VLBA.
Constraining Astronomical Populations with Truncated Data Sets Brandon C. Kelly (CfA, Hubble Fellow, 6/11/2015Brandon C. Kelly,
The fraction of obscured quasars Junxian Wang Center for Astrophysics University of Science and Technology of China Xi’an, China Collaborated with.
The MOJAVE Program: Investigating Evolution in AGN Jets Collaborators : M. Cara, N. Cooper, S. Kuchibhotla, S. Nichols, A. Lankey, N. Mellott, K. O'Brien.
CSE 221: Probabilistic Analysis of Computer Systems Topics covered: Statistical inference (Sec. )
Two years of blazar monitoring with the OVRO 40m telescope at 15GHz in support of the Fermi GST Vasiliki Pavlidou (Caltech) on behalf of the OVRO 40m team.
Numerical Modeling of Electromagnetic Radiation from AGN Jets Based on  -ray emission and spectral evolution of pair plasmas in AGN jets Bottcher et al.
Advanced Methods for Studying Astronomical Populations: Inferring Distributions and Evolution of Derived (not Measured!) Quantities Brandon C. Kelly (CfA,
Direct imaging of AGN jets and black hole vicinity Tiziana Venturi Active Galactic Nuclei 9 Ferrara,
1 The Fundamental Plane Relationship of Astrophysical Black Holes Ran Wang Supervisor: Xuebing Wu Peking University Ran Wang Supervisor: Xuebing Wu Peking.
Statistical analysis of model-fitted inner-jets of the MOJAVE blazars Xiang Liu, Ligong Mi, et al. Xinjiang Astronomical Observatory (Former Urumqi Observatory),
S. Jorstad / Boston U., USA A. Marscher / Boston U., USA J. Stevens / Royal Observatory, Edinburgh, UK A. Stirling / Royal Observatory, Edinburgh, UK M.
Spectra of partially self-absorbed jets Christian Kaiser University of Southampton Christian Kaiser University of Southampton.
The Fundamental Plane of Astrophysical Black Holes WU Xue-Bing (Peking University) Collaborators: WANG Ran (PKU) KONG Minzhi (NAOC)
I.Introduction  Recent evidence from Fermi and the VLBA has revealed a strong connection between ɣ -ray emission in AGNs and their parsec-scale radio.
SUNYAEV-ZELDOVICH EFFECT. OUTLINE  What is SZE  What Can we learn from SZE  SZE Cluster Surveys  Experimental Issues  SZ Surveys are coming: What.
S. Jorstad / Boston U., USA /St. Petersburg State U., Russia A.Marscher / Boston U., USA M. Lister / Purdue U., USA A. Stirling / U. of Manchester, Jodrell.
BL LAC OBJECTS Marco Bondi INAF-IRA, Bologna, Italy.
The MOJAVE Program: Studying the Relativistic Kinematics of AGN Jets Jansky Postdoctoral Fellow National Radio Astronomy Observatory Matthew Lister.
Is the dependence of spectral index on luminosity real in high-z QSO samples? Answer: No! Su-Min Tang, Shuang-Nan Zhang Tsinghua Center for Astrophysics.
Polarization of AGN Jets Dan Homan National Radio Astronomy Observatory.
Populations Studies in the Fermi Era D. Gasparrini on behalf of M. Ajello and Fermi Lat collaboration.
The Quasar : A Laboratory for Particle Acceleration Svetlana Jorstad IAR, Boston U Alan Marscher IAR, Boston U Jonathan Gelbord U. Durham Herman.
From the Black Hole to the Telescope: Fundamental Physics of AGN Esko Valtaoja Tuorla Observatory, University of Turku, Finland Metsähovi Radio Observatory,
Exploringthe μJy and nJy Sky with the EVLA and the SKA Ken Kellermann NRAO East Asia SKA Workshop December 3, /2/20111KASI, Daejeon, Korea.
KVN V LBI E xtragalactic Co mpact R adio S ource S urvey Lee, Sang-Sung 2009EastAsiaVLBIWorkshop 2009EastAsiaVLBIWorkshop.
AGN: Linear and Circular Polarization
The hard X-ray Extra-Galactic sky with INTEGRAL/IBIS High-z QSOs A.De Rosa on behalf of the INTEGRAL/AGN survey team.
The Evolution of AGN Obscuration Ezequiel Treister (ESO) Meg Urry (Yale) Julian Krolik (JHU)
Radio-Loud AGN Model (Credit: C.M. Urry and P. Padovani ) These objects also have hot, ADAF-type accretion flows, where the radiative cooling is very.
The dependence on redshift of quasar black hole masses from the SLOAN survey R. Decarli Università dell’Insubria, Como, Italy A. Treves Università dell’Insubria,
Ezequiel Treister Advisors: Meg Urry (Yale) José Maza (U. de Chile)
Anita Reimer, HEPL/Stanford University GLAST-lunch talk, 23 February 2006 On the diffuse AGN contribution to the extragalactic  -ray background (EGRB)
The University of Sheffield Joanna Holt 20 th October 2006 Emission line outflows: the evidence for AGN-induced feedback Clive Tadhunter.
Unification -- 2 Where next?. Recap of current status Emission from nuclear relativistic jets is important in all radio-loud objects. Axisymmetric dust.
The luminosity-dependent evolution of the radio luminosity function Emma Rigby University of Nottingham Collaborators: P. Best, M. Brookes, J. Dunlop,
Brigthest Cluster Galaxies Unique class of objects  most luminous  most massive  extended source  some BCG shows multiple nuclei → galaxy merger →
Tools for computing the AGN feedback: radio-loudness and the kinetic luminosity function Gabriele Melini Fabio La Franca Fabrizio Fiore Active Galactic.
The Radio Properties of Type II Quasars PLAN Type II quasars Motivations Our sample Radio observations Basic radio properties Compare our results with.
Hydrodynamics of Small- Scale Jets: Observational aspects Esko Valtaoja Tuorla Observatory, University of Turku, Finland Metsähovi Radio Observatory, Helsinki.
Average Fe Kα emission from distant AGN
The Dichotomy of Seyfert Galaxies at Hardest X-rays
Radio Loud and Radio Quiet AGN
Catching Blazars in their ordinary life
ACTIVE GALACTIC NUCLEI
Total intensity radio variations in blazars
On behalf of the Radio-Agile AGN WG
Deriving and fitting LogN-LogS distributions An Introduction
Special Theory of Relativity
The black hole fundamental plane: revisit with a larger sample of radio and X-ray emitting broad line AGNs Zhao-Yu Li Astronomy Department, Peking University.
Relativistic outflows and GLAST
Junior Research Fellow,
The origin nuclear X-ray emission in the nuclei of radio galaxy-FR Is
Cosmic evolution of AGN in several X-ray bands
Lecture 7: Jets on all scales Superluminal apparent motions.
Radio-loud quasars in SDSS DR3
Center for Astrophysics
Cosmological parameters with radio galaxies
Janie K. Hoormann University of Queensland 23 April 2019
An MHD Model for the Formation of Episodic Jets
Variability Study of Fermi Blazars
Borislav Nedelchev et al. 2019
Presentation transcript:

The Lorentz Factor Distribution and Luminosity Function of Relativistic Jets in AGN Yuan Liu and Shuang Nan Zhang Center for Astrophysics Tsinghua University

Introduction FR II FSRQ Radio luminosity function of AGN Doppler beaming effect FR II (as the intrinsic luminosity function) beamed luminosity function FR II FSRQ (Urry & Padovani 1991, 1992, 1995)

Introduction Luminosity function Flux limit Lorentz factor distribution Flux limit (Lister & Marscher 1997, Simulation results)

Introduction -1.75< a< -1.5

For a single power law intrinsic luminosity functon The inverse problem The maximum likelihood method The probability density function of apparent velocity for the given observed luminosity and redshift The observed luminosity function For a single power law intrinsic luminosity functon “3=1+2”

Examples deboosting

Examples

The luminosity and redshift sample (MOJAVE survey 15GHz)

The result of the apparent velocity

The result of the apparent velocity Different parent populations?

The result of the observed luminosity z>0.1

The goodness of fit

The goodness of fit

The goodness of fit

Comparison with previous studies Padovani & Urry (1995) Lister (1997) -1.75< a< -1.5 Simulation results

Application Intrinsic luminosity function Kinetic luminosity function +Black hole mass density Jet production efficiency (Heinz et al. 2007)

Summary We determine simultaneously the intrinsic luminosity function and the Lorentz factor distribution. The shape of the intrinsic luminosity function is the same with the observed luminosity function of FR II The low and high redshift groups divided by z = 0.1 are likely to be from different parent populations.