Introduction to the High Energy Astrophysics Introductory lecture.

Slides:



Advertisements
Similar presentations
Many different acceleration mechanisms: Fermi 1, Fermi 2, shear,... (Fermi acceleration at shock: most standard, nice powerlaw, few free parameters) main.
Advertisements

GAMMA-RAY COMPACT BINARIES* ASTROPHYSICAL SCENARIOS Félix Mirabel * Neutron stars & Black holes in stellar binary systems that radiate in gamma-rays. (Will.
COSMIC RAY ORIGINS Stella Bradbury, University of Leeds, U.K.  -ray sources the cosmic ray connection detection technique galactic and extragalactic.
The Galactic diffuse emission Sabrina Casanova, MPIK Heidelberg XXth RENCONTRES DE BLOIS 18th - 23rd May 2008, Blois.
Gamma-Ray Bursts & High Energy Astrophysics Kunihito Ioka (KEK) 井岡 邦仁.
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.
High Energy Neutrinos from Astrophysical Sources Dmitry Semikoz UCLA, Los Angeles & INR, Moscow.
25 ii 2011NASM1 Exploring the Crab Nebula with the Hubble, Chandra and Fermi Space Telescopes Roger Blandford KIPAC Stanford.
Neutrinos as probes of ultra-high energy astrophysical phenomena Jenni Adams, University of Canterbury, New Zealand.
Fundamental Issues in High Energy Astrophysics Roger Blandford KIPAC Stanford.
What is High-Energy Astrophysics? What is studied by high-energy astrophysicists: Supernovae Supernovae remnants Pulsars/magnetars Gamma-ray bursts Accreting.
Gamma-Ray Astronomy Dana Boltuch Ph. D
Physics 777 Plasma Physics and Magnetohydrodynamics (MHD) Instructor: Gregory Fleishman Lecture 13. Astrophysical Plasmas 02 December 2008.
Ehud Nakar California Institute of Technology Gamma-Ray Bursts and GLAST GLAST at UCLA May 22.
Gamma-ray Astrophysics Pulsar GRB AGN SNR Radio Galaxy The very high energy  -ray sky NEPPSR 25 Aug Guy Blaylock U. of Massachusetts Many thanks.
The 511 keV Annihilation Emission From The Galactic Center Department of Physics National Tsing Hua University G.T. Chen 2007/1/2.
The ANTARES Neutrino Telescope Mieke Bouwhuis 27/03/2006.
GAMMA-RAY COMPACT BINARIES* ASTROPHYSICAL SCENARIOS Félix Mirabel CEA-Saclay-France * Neutron stars & Black holes in stellar binary systems that radiate.
Cosmic Rays Discovery of cosmic rays Local measurements Gamma-ray sky (and radio sky) Origin of cosmic rays.
Zhang Ningxiao.  Emission of Tycho from Radio to γ-ray.  The γ-ray is mainly accelerated from hadronic processes.
Multi-wavelength AGN spectra and modeling Paolo Giommi ASI.
NEEP 541 Radiation Interactions Fall 2003 Jake Blanchard.
High-Energy Astrophysics
September 26, 2004Lucy Fortson - Extreme Astronomy Short Course Multiwavelength astronomy is extreme astronomy!  OUTLINE o Importance of Multiwavelength.
High energy emission from jets – what can we learn? Amir Levinson, Tel Aviv University Levinson 2006 (IJMPA, review)
Fermi: Highlights of GeV Gamma-ray Astronomy Dave Thompson NASA GSFC On behalf of the Fermi Gamma-ray Space Telescope Large Area Telescope Collaboration.
The “Crab Nebula”: the most famous supernova remnant. distance  2000 pc diameter  3 pc.
High energy Astrophysics Mat Page Mullard Space Science Lab, UCL 6. Jets and radio emission.
Jacques Paul Soft Gamma-Ray Astronomy 23 January 2001 Rencontres de Moriond Les Arcs Expected Impact on VHE Phenomena Panorama in the Coming Years INTEGRAL.
Project Gamma By Wylie Ballinger and Sam Russell Visit For 100’s of free powerpoints.
Lunch discussion on motivations for studying blazar variability Greg Madejski, SLAC Parts of this presentation use slides by Benoit Lott and Jun Kataoka.
The Origin and Acceleration of Cosmic Rays in Clusters of Galaxies HWANG, Chorng-Yuan 黃崇源 Graduate Institute of Astronomy NCU Taiwan.
Cosmic Rays GNEP Teacher Workshop Steve Shropshire, July 2007.
First results of Galactic observations with MAGIC Javier Rico Institut de Física d’Altes Energies Barcelona, Spain XII International Workshop on “Neutrino.
Discovery of  rays from Star-Forming Galaxies New class of nonthermal sources/gamma-ray galaxies (concept of temperature breaks down at high energies)
Active Galactic Nuclei & High Energy Neutrino Astronomy 黎卓 北京大学 >TeV JUNO Workshop, IHEP, 2015/7/10.
L EPTONIC NEUTRINOS Arunava Bhadra High Energy & Cosmic Ray Research Ctr. North Bengal University My collaborators: Prabir Banik and Biplab Bijay.
Institute of Radio Astronomy of NASU, Kharkov
MA4: HIGH-ENERGY ASTROPHYSICS Critical situation of manpower : 1 person! Only «free research» based in OAT. Big collaborations based elsewhere (Fermi,
Liverpool: 08-10/04/2013 Extreme Galactic Particle Accelerators The case of HESS J Stefan Ohm ( Univ. of Leicester), Peter Eger, for the H.E.S.S.
Gamma-rays, neutrinos and cosmic rays from microquasars Gustavo E. Romero (IAR – CONICET & La Plata University, Argentina)
260404Astroparticle Physics1 Astroparticle Physics Key Issues Jan Kuijpers Dep. of Astrophysics/ HEFIN University of Nijmegen.
The Universe >100 MeV Brenda Dingus Los Alamos National Laboratory.
1st page of proposal with 2 pictures and institution list 1.
Diffuse Emission and Unidentified Sources
Particle Acceleration GeV-TeV Astrophysics in the GLAST era SLAC Sep Roger Blandford KIPAC.
A Pulsar Wind Nebula Origin for Luminous TeV Source HESS J Joseph Gelfand (NYUAD / CCPP) Eric Gotthelf, Jules Halpern (Columbia University), Dean.
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.
VHE  -ray Emission From Nearby FR I Radio Galaxies M. Ostrowski 1 & L. Stawarz 1,2 1 Astronomical Observatory, Jagiellonian University 2 Landessternwarte.
Science Capabilities - Summary 200  bursts per year  prompt emission sampled to > 20 µs AGN flares > 2 mn  time profile +  E/E  physics of jets and.
RADIATION AND SPECTRA Chapter 4 WAVESWAVES l A stone dropped into a pool of water causes an expanding disturbance called a wave.
Extreme Astrophysics the the > 10 GeV photon energy < cm wavelength > 10 8 TeV particles exist > 10 8 TeV particles exist they should.
High energy Astrophysics Mat Page Mullard Space Science Lab, UCL 1. Overview.
A fast online and trigger-less signal reconstruction Arno Gadola Physik-Institut Universität Zürich Doktorandenseminar 2009.
Hiroyasu Tajima Stanford Linear Accelerator Center Kavli Institute for Particle Astrophysics and Cosmology October 26, 2006 GLAST lunch Particle Acceleration.
COSMIC RAYS. At the Earth’ Surface We see cascades from CR primaries interacting with the atmosphere. Need to correct for that to understand their astronomical.
Active Galaxies Galaxies with extremely violent energy release in their nuclei (pl. of nucleus). → “Active Galactic Nuclei” (= AGN) Up to many thousand.
High Energy Observational Astrophysics. 1 Processes that emit X-rays and Gamma rays.
Gamma-ray bursts Tomasz Bulik CAM K, Warsaw. Outline ● Observations: prompt gamma emission, afterglows ● Theoretical modeling ● Current challenges in.
UHE Cosmic Rays from Local GRBs Armen Atoyan (U.Montreal) collaboration: Charles Dermer (NRL) Stuart Wick (NRL, SMU) Physics at the End of Galactic Cosmic.
Point-like source searches with ANTARES RICAP Conference Rome, June 2007 Juan de Dios Zornoza (IFIC - Valencia)
Tobias Jogler Max-Planck Institut für Physik IMPRS YSW Ringberg 2007 VHE emission from binary systems Outline Binary systems Microquasar Pulsar binaries.
GLAST Observations of Supernova Remnants and Pulsar Wind Nebulae Bryan Gaensler The University of Sydney / Harvard-Smithsonian Center for Astrophysics.
Gamma Rays from the Radio Galaxy M87
MAGIC M.Teshima MPI für Physik, München (Werner-Heisenberg-Institut)
Observation of Pulsars and Plerions with MAGIC
Relativistic outflows and GLAST
Songzhan Chen Institute of High Energy Physics (IHEP) Nanjing
Gamma Ray Emission Mechanisms
Presentation transcript:

Introduction to the High Energy Astrophysics Introductory lecture

Cosmic Ray Spectrum (nuclear component) Energy eV „Knee ” 1 particle/m 2 yr Particle Flux ( m2 s sr GeV ) -1 1 particle/m 2 s „Ankle ” 1 particle/km 2 yr 1 J  6  eV

Zakres wysokich energii E 2.5 Particle Flux Energy (eV)

SNR

Black Holes

Pulsary

Crab Nebula : : wide frequency range electromagnetic spectrum - 20 decades  fotons – over 9 decades ! COMPTEL EGRET HEGRA 100 keV – 100 TeV CELESTE E e ~10 15 eV IC: syn, opt, IR, micro, CMB B=160  G SYN

Quasars

Mkn 421 SYN IC czas w dniach eVTeV keV TeV High variability: one looks into vicinity of the central black hole Takahashi et al. 2000

Radiosources

Solar magnetosphere

20 Stars RadioInfraredVisible lightX-rays VHE gamma rays Dust Cosmic electron accelerators B Cosmic proton accelerators magnetic field adjusts relative height of peaks  ~  S pectral E nergy D istribution : Energy emitted per log(E) interval

Astronomical osbervation cover a wide range of electromagnetic waves with characteristic frequencies or photon energies: Astronomy uses observations of electromagnetic signals spanning over 20 decades in frequency 10 9 Hz – radio Hz – far IR Hz – close IR Hz – optical (eV) Hz – UV Hz – X-rays (keV) Hz – soft gamma rays (MeV) Hz – high energy gamma rays (GeV) Hz – very high energy gamma rays (TeV)

Observational windows of gamma ray astronomy : LE or MeV : MeV ( *) HE or GeV : GeV ( *) VHE or TeV : TeV ( *) UHE or PeV : PeV EHE or EeV : EeV are open in ranges of MeV, GeV, i TeV: LE,HE – observations from space VHE,.... -observations from the Earth surface * few scientific results

Basic emission processes with CR particles Elektrons: - Synchrotron emission („SYN”) - inmverse Compton emission („IC”) - nonthermal bremsstrahlung (usually not significant) Protons: - interactions p-p pions photons 

Synchrotron emission ("SYN") of relativistic electrons spiraling in the magnetic field Emission time scale Emmitted energy with maximum near (B -4  B/[10 -4 G]) Hz Dla B -4 =1 i E~ GeV -> 10 8 Hz TeV -> Hz PeV -> Hz lat for above B and E, respectively, ~10 6, ~10 3 i ~1 lat

Inverse Compton emission ("IC") of relativistic electrons scattering low energy photons Emission time scale (with U o,-10 = U o /[ erg/cm 3 ]) lat In the Thompson range ( o  < m e c 2, above: K-N) Energies of scattered photons For example, for scattering of CMB photons (  o ~10 -4 eV) and E e = 1 GeV, 1 TeV, 1 PeV one receives  ' = 100 eV, 100 MeV, 100 TeV

Cosmic objects of interest for High Energy Astrophysics quasars balzars Syfert 1 Syfert 2 AGN MAS jets kpc-scale jets radio lobes hot spots in radio lobes neutron stars black holes NSXB BHXB accreting X-ray pulsars rotation powered pulsars milisecond pulsars plerions SNR cataclysmic variables microquasars Sgr A* stellar winds near O/B GRB GRB afterglow soft gamma ray repeaters magnetars Solar protuberances interplanetary shock waves Earth magnetosphere CME cosmic rays high energy neutinos