introduction to the high energy astrophysics introductory lecture

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Introduction to the High Energy Astrophysics Introductory lecture

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Page 1: Introduction to the High Energy Astrophysics Introductory lecture

Introduction to the High Energy Astrophysics

Introductory lecture

Page 2: Introduction to the High Energy Astrophysics Introductory lecture

Cosmic Ray Spectrum

(nuclear component)

Energy eV

„Knee”1 particle/m2 yr

Par

ticl

e F

lux

( m

2 s

sr G

eV )

-1

1 particle/m2 s

„Ankle”1 particle/km2 yr

1 J 61018 eV

Page 3: Introduction to the High Energy Astrophysics Introductory lecture

Zakres wysokichenergii

E

2 .5 P

arti

cle

Flu

x

Energy (eV)

Page 4: Introduction to the High Energy Astrophysics Introductory lecture

SNR

Page 5: Introduction to the High Energy Astrophysics Introductory lecture
Page 6: Introduction to the High Energy Astrophysics Introductory lecture

Black Holes

Page 7: Introduction to the High Energy Astrophysics Introductory lecture
Page 8: Introduction to the High Energy Astrophysics Introductory lecture
Page 9: Introduction to the High Energy Astrophysics Introductory lecture

Pulsary

Page 10: Introduction to the High Energy Astrophysics Introductory lecture
Page 11: Introduction to the High Energy Astrophysics Introductory lecture

Crab Nebula : : wide frequency range electromagnetic

spectrum - 20 decades fotons – over 9

decades !

COMPTEL EGRET

HEGRA100 keV – 100 TeV

CELESTE

Ee ~1015 eV

IC: syn,opt, IR, micro, CMB

B=160 G

SYN

Page 12: Introduction to the High Energy Astrophysics Introductory lecture

Quasars

Page 13: Introduction to the High Energy Astrophysics Introductory lecture

Mkn 421

SYN IC

czas w dniach

eV TeV

keVTeV

High variability: one looks into vicinity of the central black hole

Takahashi et al. 2000

Page 14: Introduction to the High Energy Astrophysics Introductory lecture

Radiosources

Page 15: Introduction to the High Energy Astrophysics Introductory lecture
Page 16: Introduction to the High Energy Astrophysics Introductory lecture
Page 17: Introduction to the High Energy Astrophysics Introductory lecture

Solar magnetosphere

Page 18: Introduction to the High Energy Astrophysics Introductory lecture
Page 19: Introduction to the High Energy Astrophysics Introductory lecture
Page 20: Introduction to the High Energy Astrophysics Introductory lecture

20

Stars

Radio Infrared Visible light X-raysVHE

gamma rays

DustCosmic

electronaccelerators

B

Cosmic proton

accelerators

magnetic fieldadjusts relativeheight of peaks

~

SpectralEnergyDistribution:Energy emitted perlog(E) interval

Page 21: Introduction to the High Energy Astrophysics Introductory lecture

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

109 Hz – radio1011 Hz – far IR1014 Hz – close IR1015 Hz – optical (eV)1016 Hz – UV1018 Hz – X-rays (keV)1021 Hz – soft gamma rays (MeV)1024 Hz – high energy gamma rays (GeV)1027 Hz – very high energy gamma rays (TeV)

108

1029

Page 22: Introduction to the High Energy Astrophysics Introductory lecture

Observational windows of gamma ray astronomy :

LE or MeV : 0.1 -100 MeV (0.1 -10 + 10 -100*)

HE or GeV : 0.1 -100 GeV (0.1 -10 + 10 -100*)

VHE or TeV : 0.1 -100 TeV (0.1 -10 + 10 -100*)

UHE or PeV : 0.1 -100 PeV EHE or EeV : 0.1 -100 EeV

are open in ranges of MeV, GeV, i TeV:

LE,HE – observations from space VHE, .... -observations from the Earth surface

* few scientific results

Page 23: Introduction to the High Energy Astrophysics Introductory lecture

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

Page 24: Introduction to the High Energy Astrophysics Introductory lecture

Synchrotron emission ("SYN")of relativistic electrons spiraling in the magnetic field

222 )sin(2)( BUcP BTsyn

Emission time scale

24

19 )(105.2

Btsyn

Emmitted energy with maximum near (B-4 B/[10-4 G])

24100~3.0 Bc Hz

Dla B-4=1 i E~

GeV -> 108 HzTeV -> 1014 Hz PeV -> 1020 Hz

lat

for above B and E, respectively, ~106, ~103 i ~1 lat

Page 25: Introduction to the High Energy Astrophysics Introductory lecture

Inverse Compton emission ("IC") of relativistic electrons scattering low energy photons

Emission time scale (with Uo,-10 = Uo/[10-10 erg/cm3])

110,0

110, )(10~

Ut TIC lat

oTTIC UcP 2, 3

4

In the Thompson range ( o < mec2 , above: K-N)

Energies of scattered photons2 o

For example, for scattering of CMB photons (o~10-4 eV)and Ee = 1 GeV, 1 TeV, 1 PeV one receives ' = 100 eV, 100 MeV, 100 TeV

Page 26: Introduction to the High Energy Astrophysics Introductory lecture

Cosmic objects of interest for High Energy Astrophysics

quasarsbalzarsSyfert 1Syfert 2AGNMAS jetskpc-scale jetsradio lobeshot spots in radio lobes

neutron starsblack holesNSXBBHXBaccreting X-ray pulsarsrotation powered pulsarsmilisecond pulsarsplerionsSNRcataclysmic variablesmicroquasarsSgr A*stellar winds near O/B

GRBGRB afterglowsoft gamma ray repeatersmagnetars

Solar protuberancesinterplanetary shock wavesEarth magnetosphereCME cosmic rays

high energy neutinos