Supernova Remnants and Cosmic. Rays

Similar documents
Compton Lecture #4: Massive Stars and. Supernovae. Welcome! On the back table:

> News < AMS-02 will be launched onboard the Shuttle Endeavour On May 2nd 2:33 P.M. from NASA Kennedy space center!

Supernova Remnants and GLAST

Radio Observations of TeV and GeV emitting Supernova Remnants

Supernovae. Supernova basics Supernova types Light Curves SN Spectra after explosion Supernova Remnants (SNRs) Collisional Ionization

Supernovae. Supernova basics Supernova types Light Curves SN Spectra after explosion Supernova Remnants (SNRs) Collisional Ionization

Lecture 2 Supernovae and Supernova Remnants

Cosmic Rays - R. A. Mewaldt - California Institute of Technology

Stellar Explosions (ch. 21)

Recent Observations of Supernova Remnants

Neutrino Oscillations and Astroparticle Physics (5) John Carr Centre de Physique des Particules de Marseille (IN2P3/CNRS) Pisa, 10 May 2002

Constraints on cosmic-ray origin from gamma-ray observations of supernova remnants

99 Years from Discovery : What is our current picture on Cosmic Rays? #6 How cosmic rays travel to Earth? Presented by Nahee Park

Particle Acceleration at Supernova Remnants and Supernovae

Revue sur le rayonnement cosmique

Astronomy 1504 Section 002 Astronomy 1514 Section 10 Midterm 2, Version 1 October 19, 2012

Gamma rays from supernova remnants in clumpy environments.! Stefano Gabici APC, Paris

Outline - March 18, H-R Diagram Review. Protostar to Main Sequence Star. Midterm Exam #2 Tuesday, March 23

Astro 1050 Wed. Apr. 5, 2017

Mass loss from stars

Supernova Remnants as Cosmic Ray Accelerants. By Jamie Overbeek Advised by Prof. J. Finley

Cosmic Rays. Discovered in 1912 by Viktor Hess using electroscopes to measure ionization at altitudes via balloon

Introductory Astrophysics A113. Death of Stars. Relation between the mass of a star and its death White dwarfs and supernovae Enrichment of the ISM

Physics HW Set 3 Spring 2015

Cosmic Rays: A Way to Introduce Modern Physics Concepts. Steve Schnetzer

Cosmic Rays. This showed that the energy of cosmic rays was many times that of any other natural or artificial radiation known at that time.

Supernova remnants: X-ray observations with XMM-Newton

Comparing a Supergiant to the Sun

Gamma ray emission from supernova remnant/molecular cloud associations

Low-Energy Cosmic Rays

PERSPECTIVES of HIGH ENERGY NEUTRINO ASTRONOMY. Paolo Lipari Vulcano 27 may 2006

Stars: Their Life and Afterlife

Special Topics in Nuclear and Particle Physics

Pulsar Wind Nebulae: A Multiwavelength Perspective

MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.

Joy of Science Experience the evolution of the Universe, Earth and Life

Potential Neutrino Signals from Galactic γ-ray Sources

Supernovae, Neutron Stars, Pulsars, and Black Holes

A New View of the High-Energy γ-ray Sky with the Fermi Telescope

Midterm Results. The Milky Way in the Infrared. The Milk Way from Above (artist conception) 3/2/10

Particle acceleration in Supernova Remnants

Late stages of stellar evolution for high-mass stars

Stellar Astronomy Sample Questions for Exam 4

Remnants and Pulsar Wind

Cosmic Rays, Photons and Neutrinos

Astronomy 104: Second Exam

Shock Waves. = 0 (momentum conservation)

PACIFIC 2014, Moorea, French Polynesia, Sep Efficient CR Acceleration and High-energy Emission at Supernova Remnants

Life and Death of a Star 2015

High energy radiation from molecular clouds (illuminated by a supernova remnant

Lecture 14 Cosmic Rays

Astronomy Ch. 21 Stellar Explosions. MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.

Evolution of High Mass Stars

Ultra High Energy Cosmic Rays I

Recent discoveries from TeV and X- ray non-thermal emission from SNRs

Cosmic Ray Astronomy. Qingling Ni

Lecture 23 Stellar Evolution & Death (High Mass) November 21, 2018

Particle Acceleration in the Universe

Summary of Last Lecture Next 5 Slides. See Supernova remnants: the X-ray perspective for an excellent review article JaccoVink, 2012 A&ARv

Sound Waves Sound Waves:

Exploring the Ends of the Rainbow: Cosmic Rays in Star-Forming Galaxies

The Birth Of Stars. How do stars form from the interstellar medium Where does star formation take place How do we induce star formation

Number of Stars: 100 billion (10 11 ) Mass : 5 x Solar masses. Size of Disk: 100,000 Light Years (30 kpc)

Fermi: Highlights of GeV Gamma-ray Astronomy

The Death of Stars. Today s Lecture: Post main-sequence (Chapter 13, pages ) How stars explode: supernovae! White dwarfs Neutron stars

² The universe observed ² Relativistic world models ² Reconstructing the thermal history ² Big bang nucleosynthesis ² Dark matter: astrophysical

10/26/ Star Birth. Chapter 13: Star Stuff. How do stars form? Star-Forming Clouds. Mass of a Star-Forming Cloud. Gravity Versus Pressure

The role of ionization in the shock acceleration theory

Supernovae Through the Ages

High Energy Astrophysics

This class: Life cycle of high mass stars Supernovae Neutron stars, pulsars, pulsar wind nebulae, magnetars Quark-nova stars Gamma-ray bursts (GRBs)

The Physics of Cosmic Rays

Astronomy 113. Dr. Joseph E. Pesce, Ph.D. Dr. Joseph E. Pesce, Ph.D.

Questions 1pc = 3 ly = km

X-ray Hotspot Flares and Implications for Cosmic Ray Acceleration and magnetic field amplification in Supernova Remnants

Observations of supernova remnants

Outline. Stellar Explosions. Novae. Death of a High-Mass Star. Binding Energy per nucleon. Nova V838Mon with Hubble, May Dec 2002

High Energy Astrophysics: A View on Chemical Enrichment, Outflows & Particle Acceleration. (Feedback at work)

Cosmic Pevatrons in the Galaxy

Chapter 14 Our Star Pearson Education, Inc.

Lec 7: Classification of Stars, the Sun. What prevents stars from collapsing under the weight of their own gravity? Text

X-Ray Spectroscopy of Supernova Remnants. Introduction and Background:

Brock University. Test 1, February, 2017 Number of pages: 9 Course: ASTR 1P02 Number of Students: 480 Date of Examination: February 6, 2017

Short Course on High Energy Astrophysics. Exploring the Nonthermal Universe with High Energy Gamma Rays

Propagation in the Galaxy 2: electrons, positrons, antiprotons

X Rays must be viewed from space used for detecting exotic objects such as neutron stars and black holes also observing the Sun.

Gamma-ray Astrophysics

Gravity Waves Gravity Waves

Stars with Mⵙ go through two Red Giant Stages

Einführung in die Astronomie II

ASTRONOMY 1 EXAM 3 a Name

18. Stellar Birth. Initiation of Star Formation. The Orion Nebula: A Close-Up View. Interstellar Gas & Dust in Our Galaxy

L = 4 d 2 B p. 4. Which of the letters at right corresponds roughly to where one would find a red giant star on the Hertzsprung-Russell diagram?

L = 4 d 2 B p. 1. Which outer layer of the Sun has the highest temperature? A) Photosphere B) Corona C) Chromosphere D) Exosphere E) Thermosphere

Brock University. Test 1, January, 2015 Number of pages: 9 Course: ASTR 1P02 Number of Students: 500 Date of Examination: January 29, 2015

The Large Area Telescope on-board of the Fermi Gamma-Ray Space Telescope Mission

10/17/ A Closer Look at the Sun. Chapter 11: Our Star. Why does the Sun shine? Lecture Outline

LIFE CYCLE OF A STAR

Chapter 21 Stellar Explosions

Type II Supernovae Overwhelming observational evidence that Type II supernovae are associated with the endpoints of massive stars: Association with

Transcription:

Stars: Their Life and Afterlife Supernova Remnants and Cosmic 68 th Rays Brian Humensky Series, Compton Lecture #5 November 8, 2008 th Series, Compton Lecture #5

Outline Evolution of Supernova Remnants Cosmic Rays Supernova Remnants and their Radiation

Key Points to Take Away SNRs produce many kinds of thermal and nonthermal radiation Each tells us something about conditions in progenitor, SN, or SNRS Cosmic rays bombard the earth all the time, and carry a significant fraction of the energy budget of the galaxy SNRs long thought to be the source of cosmic rays but definitive proof is still lacking Shock acceleration seems the likely mechanism, but Max energy? Unambiguous proof of nuclear cosmic ray acceleration?

Evolution of Supernova Remnants

The Free Expansion Phase Particle acceleration Hot compressed external gas mass á ejecta Interstellar gas (Type Ia) Shock SN Ejecta OR Wind from exploded star, with compressed gas shells (Type Ib/c or Type II) Hot compressed SN ejecta Shock expands at 10-20 * 10 3 km/s flfew % speed of light (3 * 10 5 km/s) Ambient matter is swept up, compressed, and heated

The Taylor-Sedov Phase Hot compressed external gas mass p ejecta Particle acceleration Reverse shock Interstellar gas (Type Ia) Shock SN Ejecta OR Wind from exploded star, with compressed gas shells (Type Ib/c or Type II) Hot compressed SN ejecta Shock slows to few * 10 3 km/s fl Ejecta compressed, heated fl Reverse shock propagates back into ejecta

The Snow Plow or Radiative Phase When the SNR s s shell cools to d 10 6 K, electrons begin to recombine with heavy atoms (oxygen, silicon, )) to form ions Enhances SNR s s ability to cool by radiating As cooling continues, more and more ions form fl more cooling fl snowball effect Shell shrinks, gets denser fl expansion slows, stops Phase lasts a few hundred thousand years ( few * 10 5 years) Shell visible in radio (synchrotron) and optical (synch, thermal)

Dispersal Eventually expansion speed drops below sound speed in ISM (~20 km/s) no longer a shock Random motions of ISM disrupt SNR SNR gradually mixes with ISM Heavy elements synthesized in supernova enrich the ISM

Cosmic Rays

What are Cosmic Rays? Cosmic rays are high-energy charged particles that strike the earth from all directions ~85% protons, ~12% helium nuclei, ~1% heavier nuclei, ~2% electrons and positrons Why are they interesting? Sample of matter from outside our Solar System Teach us about the composition, evolution, dynamics of the galaxy Particle physics discoveries

Charged Particles Surround Us Early 1900 s: Radioactivity recently discovered Natural radioactivity exists in the earth all around us X-rays, gamma rays, electrons/positrons, protons, neutrons, alpha particles Produced by smoke detectors, bananas, radon, and other every-day items Energetic particles ionize atoms that they interact with fl ionizing radiation

Discovering Cosmic Rays Ionizing radiation from natural radioactivity should decrease with altitude Air provides insulation Viktor Hess tested this with a balloon flight in 1912 Up to 5 km Rate of ionizing radiation dropped till 1.5 km, then began rising again! Radiation coming from space! Coined cosmic rays by Robert Millikan in 1925 Rate Altitude

Fast Forward ~90 Years: CR Spectrum Galactic Cosmic Rays Power Law spectrum: Flux μ E -α (straight line on log-log plot) Extragalactic Cosmic Rays

Where Do They Come From? (Nuclear) cosmic rays are a major component of the galaxy s energy budget! They diffuse slowly from their sources through the galaxy in a random walk. And gradually leak out of the galaxy, with a typical timescale of ~ 10 million years fl CR power loss ~ 5 * 10 40 erg/s Can be supplied by SNe: luminosity of ~ 10 42 erg/s on average ~10 51 erg released in SN / 50 yrs ~ 10 9 s Radiation Cosmic Rays Star Light Cosmic Microwave Background Galactic Magnetic Fields Energy Density (ev/cm 3 ) 1.0 0.3 0.3 0.2 fi Can we prove that cosmic-ray nuclei are accelerated in SNRs?

Shock Acceleration Shock waves + strong magnetic fields increase the energy of cosmic rays over time From particle s s perspective, each time it crosses the shock it experiences a head-on collision with magnetic domains Energy gain ΔE/E shock speed / speed of light ~ 1 % Shock Particle Hot, compressed swept-up gas External medium

Shock Acceleration Cosmic ray gains ~ 1 % energy on each crossing Confined near shock: scatters off turbulent magnetic fields Can cross 1000 s s of times! Timescales: for a 10 μg G magnetic field and 10 3 km/s shock speed, can accelerate a proton to 1 GeV in ~ 1 month 1 TeV in ~ 100 years 1 PeV in ~ 10 5 years (~lifetime of an SNR) Predicts power-law spectrum naturally! Acceleration is faster for stronger magnetic fields faster shock speeds Maybe can reach knee of CR spectrum?!? Hard to say Hot, compressed swept-up gas Shock Particle External medium

Radiation from Supernova Remnants

Bremsstrahlung and Synchrotron Radiation Charged particles radiate when they are accelerated Bremsstrahlung: radiation when an electron passes through the electric field of an atom braking radiation X-ray e - Synchrotron: radiation when an electron s path is curved by a magnetic field X-ray e - Ÿ B X-ray nucleus Produced by electrons in hot (t 10 6 K) gas fl thermal bremsstrahlung fl X-rays fl Useful for extracting temperature, density of gas in SNRs Produced by cosmic-ray electrons Very efficient cooling mechanism! fl Multi-TeV electrons produce X-rays fl cool quickly radiate at acceleration site fl MeV/GeV electrons produce radio fl cool slowly electrons can diffuse

SN 1006 Today: X-raysX Rims: synchrotron radiation from electrons accelerated by the shock front Interior: filled with hot gas - multimillion degrees Exterior: low-density interstellar medium

SN 1006 Composite Image X-rays show thin, sharp filaments in contrast to fuzzy radio intensity related to electron energy Red Radio Yellow Optical Blue X-rays

SNR G1.9+0.3: The Baby of the Galaxy Near the galactic center, ~ 28k light years away. Young! ~100-150 150 yrs old Dust and absorption made the SN itself undetectable Expanding at ~14 * 10 3 km/s fastest known SNR Diameter ~ 7 light years Very bright synchrotron radiation accelerating electrons No thermal bremsstrahlung observed yet No TeV gamma-ray signal seen (or expected yet) Red X-rays Blue Radio

Very High Energy Radiations Inverse Compton Scattering: cosmic-ray electrons γ-ray e - low-e photon e - Pion production / decay: cosmic-ray nuclei CR π 0 Ø γ + γ π Ø μ + ν O e + ν 1 H π Gamma rays and neutrinos provide a smoking gun for acceleration of cosmic ray nuclei in SNRs! Caveats: flgamma signal can be faked by cosmic-ray electrons flneutrino signal not yet detected

Cas A and Cosmic Rays Cassiopeia A is a young SNR, ~ 320 yrs old First SNR detected in TeV gamma rays! By HEGRA in 2001 since detected by VERITAS and MAGIC as well Still not clear whether it accelerates nuclei or only electrons. Chandra X-ray image

TeV Gamma Rays from SNRs: RX J1713 ~ 1000-yr yr-old SNR about 3300 light years away 1º diameter Observed by the HESS gamma-ray observatory 2003-2005 2005 First time detailed images of an extended object made in TeV gamma rays! (several more since)

TeV Gamma Rays from SNRs: RX J1713 Spectrum of TeV gamma rays produced by the cosmic rays in the SNR Follows power law up to few TeV, and then softens reaching maximum energy of cosmic rays in RX J1713? Key question: are the cosmic rays electrons or protons? Hard to answer conclusively! Need to extend spectrum to higher AND lower energies!

IC 443 A Snow Plow Remnant expanding shell impacting a cloud of atomic hydrogen giant molecular cloud hot gas fills the interior pulsar wind nebula breakout into lower-density region Red Optical Blue X-rays

What Kinds of CRs does IC 443 Accelerate? VERITAS TeV gamma-ray observations combined with multiwavelength observations: Red Optical Blue X-rays

Summary SNRs produce many kinds of thermal and nonthermal radiation Each tells us something about conditions in progenitor, SN, or SNRS Cosmic rays bombard the earth all the time, and carry a significant fraction of the energy budget of the galaxy SNRs long thought to be the source of cosmic rays but definitive proof is still lacking Shock acceleration seems the likely mechanism, but Max energy? Unambiguous proof of nuclear cosmic ray acceleration? SNRs inject a large quantity of power (kinetic energy, cosmic rays, heat) into the Interstellar Medium, with strong impacts on the local environment and the galaxy Next Week!