A Universal Luminosity Function for Radio Supernova Remnants Laura Chomiuk University of Wisconsin--Madison.

Slides:



Advertisements
Similar presentations
H 2 Formation in the Perseus Molecular Cloud: Observations Meet Theory.
Advertisements

From GMC-SNR interaction to gas-rich galaxy-galaxy merging Yu GAO Purple Mountain Observatory, Nanjing, China Chinese Academy of Sciences.
Supernova Remnants Shell-type versus Crab-like Phases of shell-type SNR.
Magnetic Fields in Supernova Remnants and Pulsar-Wind Nebulae S.P. Reynolds et al. Martin, Tseng Chao Hsiung 2013/12/18.
THE ORIGIN OF COSMIC RAYS Implications from and for X and γ-Ray Astronomy Pasquale Blasi INAF/Osservatorio Astrofisico di Arcetri, Firenze.
Modeling photon and neutrino emission from the supernova remnant RX J  Constraints from geometry  Constraints from spectral energy distribution.
Diffusive shock acceleration & magnetic field amplification Tony Bell University of Oxford Rutherford Appleton Laboratory SN1006: A supernova remnant 7,000.
Strange Galactic Supernova Remnants G (the Tornado) & G in X-rays Anant Tanna Physics IV 2007 Supervisor: Prof. Bryan Gaensler.
2009 July 8 Supernova Remants and Pulsar Wind Nebulae in the Chandra Era 1 Modeling the Dynamical and Radiative Evolution of a Pulsar Wind Nebula inside.
X-ray Properties of Five Galactic SNRs arXiv: Thomas G. Pannuti et al.
Acceleration and Escape of Particles in Young Supernova Remnants Vikram Dwarkadas University of Chicago Igor Telezhinsky, Martin Pohl (DESY) May HEDLA.
Emissions from Shells Associated with Dying Radio Sources @ Workshop on East-Asian Collaboration for the SKA /2 Hirotaka Ito YITP, Kyoto University.
Supernova Remnants in the ChASeM33 X-ray Survey of M33 Knox S. Long, William P. Blair, P. Frank Winkler, and the ChASeM33 team.
January 22, Protons (85 %) Nuclei (13%) Electrons/Positrons (2%) Galactic Origin α=2.7.
Mario A. Riquelme, Anatoly Spitkovsky Department of Astrophysical Sciences, Princeton University Generation of magnetic field upstream of shocks: the cosmic.
Magnetic-field production by cosmic rays drifting upstream of SNR shocks Martin Pohl, ISU with Tom Stroman, ISU, Jacek Niemiec, PAN.
Krakow 2008 Damiano Caprioli Scuola Normale Superiore – Pisa, Italy The dynamical effects of self-generated magnetic fields in cosmic-ray-modified shocks.
Measuring the Diffuse Extragalactic Background Light as a function of redshift Cosmic History of Star Formation: Holy Grail of Observational Cosmology.
Joe Giacalone and Randy Jokipii University of Arizona
Facts about SNe and their remnants Evolution of an SNR sensitively depends on its environment. Observed SNRs are typically produced by SNe in relative.
Pasquale Blasi INAF/Arcetri Astrophysical Observatory 4th School on Cosmic Rays and Astrophysics UFABC - Santo André - São Paulo – Brazil.
New evidence for strong nonthermal effects in Tycho’s supernova remnant Leonid Ksenofontov 1 H.J.Völk 2, E.G.Berezhko 1, 1 Yu.G.Shafer Institute of Cosmophysical.
Bell, E. F et al “Nearly 5000 distant Early-type galaxies in COMBO-17: A Red Sequence and its evolution since z~1” Presented by: Robert Lindner (Bob)‏
Spectral analysis of non-thermal filaments in Cas A Miguel Araya D. Lomiashvili, C. Chang, M. Lyutikov, W. Cui Department of Physics, Purdue University.
A Model for Emission from Microquasar Jets: Consequences of a Single Acceleration Episode We present a new model of emission from jets in Microquasars,
MODELING STATISTICAL PROPERTIES OF THE X-RAY EMISSION FROM AGED PULSAR WIND NEBULAE Rino Bandiera – INAF – Oss. Astrof. di Arcetri The Fast and the Furious,
Cosmic Rays Discovery of cosmic rays Local measurements Gamma-ray sky (and radio sky) Origin of cosmic rays.
Optical detection of the emission nebulae in nearby galaxies DEJAN UROŠEVIĆ collaborators: Milica Vučetić, Bojan Arbutina, Konstantin Stavrev, Dragana.
Zhang Ningxiao.  Emission of Tycho from Radio to γ-ray.  The γ-ray is mainly accelerated from hadronic processes.
Radio lobes of Pictor A: an X-ray spatially resolved study G.Migliori(1,2,3), P.Grandi(2), G.C.G.Palumbo(1), G.Brunetti(4), C.Stanghellini(4) (1) Bologna.
Magnetic Fields in Supernova Remnants and Pulsar-Wind Nebulae 2013/12/18 Speaker : Yu-Hsun Cheng Professor: Yosuke Mizuno.
Yutaka Fujita (Osaka U.) Fuijta, Takahara, Ohira, & Iwasaki, 2011, MNRAS, in press (arXiv: )
A multi-colour survey of NGC253 with XMM-Newton Robin Barnard, Lindsey Shaw Greening & Ulrich Kolb The Open University.
First It’s Hot & Then It’s Not Extremely Fast Acceleration of Cosmic Rays In A Supernova Remnant Peter Mendygral Journal Club November 1, 2007.
22 nd February 2007 Poonam Chandra Unusual Behavior in Radio Supernovae Poonam Chandra Jansky Fellow, National Radio Astronomy Observatory Astronomy Department,
Particle Acceleration by Shocks Brian Reville, Klara Schure,
Gas mixing and Star formation by shock waves and turbulence Claudio Melioli Elisabete M. de Gouveia Dal Pino (IAG-USP)
Radio Emission in Galaxies Jim Condon NRAO, Charlottesville.
Gilles Maurin – CEA Saclay - MODE10 - SNR session - November 2010 Geometry of acceleration in the bipolar remnant of SN1006 with XMM-Newton Gilles Maurin,
Outline Cosmic Rays and Super-Nova Remnants
A Pulsar Wind Nebula Origin for Luminous TeV Source HESS J Joseph Gelfand (NYUAD / CCPP) Eric Gotthelf, Jules Halpern (Columbia University), Dean.
Expected Gamma-Ray Emission of SN 1987A in the Large Magellanic Cloud (d = 50 kpc) E.G.Berezhko 1, L.T. Ksenofontov 1, and H.J.Völk 2 1 Yu.G.Shafer Institute.
Bremen, Germany Patrick Slane (CfA) COSPAR 2010: E19 Fermi Studies of Collaborators: D. Castro S. Funk Y. Uchiyama J. D. Gelfand O. C. de Jager A. Lemiere.
Turbulence and Magnetic Field Amplification in the Supernova Remnants Tsuyoshi Inoue (NAOJ) Ryo Yamazaki (Hiroshima Univ.) Shu-ichiro Inutsuka (Kyoto Univ.)
E.G.Berezhko, L.T. Ksenofontov Yu.G.Shafer Institute of Cosmophysical Research and Aeronomy Yakutsk, Russia Energy spectra of electrons and positrons,
The GRB Luminosity Function in the light of Swift 2-year data by Ruben Salvaterra Università di Milano-Bicocca.
1 Radio – FIR Spectral Energy Distribution of Young Starbursts Hiroyuki Hirashita 1 and L. K. Hunt 2 ( 1 University of Tsukuba, Japan; 2 Firenze, Italy)
Dejan Urošević Department of Astronomy, Faculty of Mathematics, University of Belgrade Supernova remnants: evolution, statistics, spectra.
The impact of magnetic turbulence spectrum on particle acceleration in SNR IC443 I.Telezhinsky 1,2, A.Wilhelm 1,2, R.Brose 1,3, M.Pohl 1,2, B.Humensky.
Searching for the Synchrotron Cosmic Web with the Murchison Widefield Array Bryan Gaensler Centre for All-sky Astrophysics / The University of Sydney Natasha.
SNRs and PWN in the Chandra Era – S. OrlandoBoston, USA – July 2009 S. Orlando 1, O. Petruk 2, F. Bocchino 1, M. Miceli 3,1 1 INAF - Osservatorio Astronomico.
Don Ellison, NCSU, Future HE-Observatory, SNR/CR Working Group Magnetic Field Amplification in Astrophysical Shocks 1)There is convincing evidence for.
Population Studies of the Unidentified EGRET Sources In collaboration with A. V. Olinto, V. Pavlidou, C. Brown, and B. D. Fields Image Credit: EGRET Team/NASA/Honeywell.
Cosmic Masers Chris Phillips CSIRO / ATNF. What is a Maser? Microwave Amplification by Stimulated Emission of Radiation Microwave version of a LASER Occur.
1 Lei Bai George Rieke Marcia Rieke Steward Observatory Infrared Luminosity Function of the Coma Cluster.
On the Galactic Center being the main source of Galactic Cosmic Rays as evidenced by recent cosmic ray and gamma ray observations Yiqing Guo, Zhaoyang.
Time-Dependent Spectra of Cosmic Rays escaped from SNRs Igor Telezhinsky, DESY, Zeuthen, Germany. Vikram Dwarkadas, University of Chicago, Chicago, USA.
7. Electromagnetic Waves 7A. Plane Waves Consider Maxwell’s Equations with no sources We are going to search for waves of the form To make things as general.
The Physics of Cosmic Ray Acceleration Tony Bell University of Oxford SN1006: A supernova remnant 7,000 light years from Earth X-ray (blue): NASA/CXC/Rutgers/G.Cassam-Chenai,
Diffusive shock acceleration: an introduction
HMXB, ULX and star formation
Supernova Progenitors From Stellar Populations And Supernova Remnants
A large XMM-Newton project on SN 1006
Are Diffuse High Energy Neutrinos from Starburst Galaxies Observable?
Cosmic rays, γ and ν in star-forming galaxies
Equipartition calculation for supernova remnants
The origin nuclear X-ray emission in the nuclei of radio galaxy-FR Is
Cosmic-ray acceleration by forward and reverse shocks in young SNR
Center for Gravitational Wave Physics Penn State University
PARTICLE ACCELERATION IN STRONG SHOCKS: INFLUENCE ON THE SUPERNOVA REMNANT EVOLUTION IN RADIO Dejan Urošević Department of Astronomy, Faculty of Mathematics,
Presentation transcript:

A Universal Luminosity Function for Radio Supernova Remnants Laura Chomiuk University of Wisconsin--Madison

Are SNRs fundamentally the same across galaxies? The brightest SNR in M33 is ~10 times less luminous than the brightest SNR in NGC Lacey & Duric (2001)

Radio SNRs in Other Galaxies NGC cm NGC 4449 H  SNR H II region Background source 8 SNRs found in NGC 4449 by Chomiuk & Wilcots (2009).

SNRs in 19 Nearby Galaxies LMCSMC IC 10 M 33NGC 1569 NGC 300 NGC 4214NGC 2366 M 82 NGC 7793 NGC 253 NGC 4449 M 81 M 83 NGC 4736 NGC 6946 NGC 4258 M 51 Arp 220

Cumulative Luminosity Functions

Composite SNR Luminosity Function  =  0.07

LF scaling factor (assuming  = -2.13) Approximately linear relation: Arp 220: outlier?

We can rewrite dN/dL as: dN/dt is the production rate of SNRs,  SFR. dL/dt describes the luminosity evolution of SNRs. Therefore, the SNR LF can be described as:

From Berezhko & Volk (2004) 3 cm cm cm -3 Some Approximations Radio SNRs are in the adiabatic phase. In the adiabatic phase, the CR energy does not depend on time or ISM density. E CR /E SN  constant.

Therefore, it is the magnetic field that determines dL/dt. Standard prescription for magnetic field amplification: Making these simplifications, we find an expression for the time evolution of synchrotron luminosity: And for the luminosity function:  = -2.1 A very good fit to the data!

The L max --SFR relation Best fit to data Prediction for statistical sampling from Monte Carlo simulations Just a statistical sampling effect?

Cas A on the L max --SFR relation Only a 3% probability that a galaxy with L max  L Cas A has a SFR > 2 M  /year

Conclusions The SNR LF is remarkably similar across galaxies. It is consistent with a power law of constant index and scaling  SFR. The SNR LF is well fit with models of diffusive shock acceleration + magnetic field amplification, given a few simplifying assumptions. Galaxies with higher SFRs host more luminous SNRs; this can be completely explained by statistical sampling effects. The luminosity of Cas A implies that current estimates of the Milky Way SFR may be too high.

Model the SNR LFs as power laws The four “best” galaxies (N SNR >20) all have similar best-fit  : weighted mean  =  0.10 M  0.17 M  0.25 NGC  0.29 M  0.26

Is there a dependence on ISM density? Line marks theoretical prediction: A/SFR   0 0.5

There are claims that B 2   0 v s 3 instead of   0 v s 2. From Vink (2004). This would predict dL/dN  L Decidedly not in agreement with the SNR LF data.