x/ -ray instrumentation 1. sources and processes in high-energy astrophysics 1. sources and...
TRANSCRIPT
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
1. Sources and Physical Processes in High Energy
Astrophysics
Xavier Barcons
Instituto de Física de Cantabria (CSIC-UC)
X-ray and -ray instrumentation
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
An apology
• I’m an X-ray Astronomer
• I’ve prepared these lectures in 3 days, by collecting other lectures delivered in post-graduate courses and summer schools
Do not expect much -ray Astronomy
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Acknowledgements• X-ray Astronomy gruop @ IFCA: Francisco
Carrera, Maite Ceballos, Silvia Mateos• XMM-Newton SSC: Mike Watson, Axel
Schwope, Roberto Della Ceca, many others • XEUS SAG: Martin Turner, Günther Hasinger,
Arvind Parmar, Johan Bleeker, many others• Spanish STJ (maybe) team: Lourdes Fàbrega,
Conrado Rillo, Fernando Briones, Carles Ferrer• Other: Andy Fabian, Fred Jansen, Tone Peacock,
Marcos Bavdaz, Alvaro Giménez, Martin Ward
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Index
• Introduction: High-energy Astrophysics from space
• A guided tour through the high-energy Universe• Physical processes in X/-ray Astrophysics:
– Synchrotron radiation
– Bremsstrahlung
– Compton Scattering
– Pairs
– Nuclei
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
The main problem of high-energy astrophysics
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Riccardo Giacconi (Genoa 1931)
1962
2002
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
The beginning of high-energy Astronomy
18-June-1962: Giacconi and collaborators fly an Aerobee rocket beyond 80 km altitude during > 5 minutes with 3 X-ray detectors
Goal: To detect X-rays reflected in the Moon from the Sun
Two surprising discoveries:•An extremely bright X-ray source, which is
totally inconspicuous in the optical (Sco X-1)•Diffuse radiation from all directions in the Universe (the
cosmic X-ray Background)And of course, no trace from the Moon…
… until 1990!
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
A short walk through the high-energy Universe
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
The Solar System
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Venus and Jupiter
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Active coronal starsCapellaAB Dor
EPIC-MOS
RGS
Sco
Pup
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Star formation
HST Chandra
Chandra
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Supernova Remnants (Cas-A)
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
N132D SNR
Fe line
OVII
OVIII
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
SNRs and PulsarsCrab Nebula and Pulsar
ChandraOptico
Pulsar
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Isolated neutron stars
First detection of X-ray cyclotron absorption lines in an isolated neutron star: Measurement of the magnetic field
B~8 x 1010 Gauss
Bignami et al 03
Cyclotron lines
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Accreting binaries
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Low-Mass X-ray binariesBlackbody+Comptonising region
Church & Balucinska-Church 01
Parmar et al 2002
Cottam et al 02
Gravitationally redshifted lines
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Be/X-ray binaries: High LX/Lopt
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The Galaxy in Soft X-rays
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
The Galaxy in 26Al
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Shadowing and the local ISM
• Shadowing of background soft X-rays by objects located at various distances
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
The Galactic Centre in X-rays
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
The galactic centre in rays
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Normal galaxies: Diffuse emission and X-ray binaries
NGC 253M 31
Chandra
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Galaxies: LMC
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Diffuse emission from galaxy clusters
ComaComa VirgoVirgo
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
The X-ray spectra of custers
• Thermal bremsstrahlung kT=1-10 keV (107-108 K)
• Fe K emission feature at 6.7 keV: Highly ionised gas
• Other emission lines at soft X-ray energies (Fe L, Mg, Si)
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Clusters: Temperature and metallicity
Coma Sérsic 159-03
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Cooling flows? Not any moreFe L
O VIII
Mg XII
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics(Chris Done, Univ of Durham)
The High-energy view of The High-energy view of AGNAGN
C. Done, Durham U
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
The High-energy AGN spectrume+e-annihilation
Saturated pair cascade
Compton Reflection hump
Fluorescence
Absorption
Soft excess
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
The X-ray spectrum of AGN
Reprocessed radiation from the disk’s atmosphere
Reflection (Fe line and Compton hump)
Absorbers
Soft excess (direct disk radiation)
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Ionized absorbers
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
The variety of Fe K line profiles
Nandra (2001)
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Relativistic line in MCG-6-30-15
Iwasawa et al. (1996, 1999)
1994 1997
< >t < >t
Mín Flare
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Gamma-Ray Bursts (GRBs)
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
The X-ray background
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
The XMM-Newton observation of the Lockman Hole
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Physical Processes in High-energy Astrophysics
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Synchrotron Radiation (I)
Ingredients:• Magnetic field B• Relativistic electrons
(Lorentz factor >>1)
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Synchrotron Radiation (II)
Cyclotron radiation:Electron with velocity vin a magnetic field Bhas a gyro frequency
B=eB
4mc
= 2.8/ MHz/Gauss
d
dt=4/3 T c (v/c)2 2 UB
Power radiated by an isotropic distributionof electrons
T=6.65 10-25 cm2
UB=B2
8
Discrete spectrum:concentrated around B and higher order harmonics
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Synchrotron radiation: continuum
• Growing importance of higher order harmonics
• Relativistic beaming: Emission within a cone of opening angle <2/ around the electron’s velocity
• Doppler effect: The time lapse in which the observer receives the radiation is smaller than the pulse emission time (obs=2em)
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Jet of electrons with Lorentz factor :
dd = B
31/2e3
mc2F(/c)
c=3eB
4mc2 sin
B
0
0.2
0.4
0.6
0.8
1
0 1 2 3 4 5 6
x
F(x
)
Continuum centeredaround c
Synchrotron radiation: continuum
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
For an isotropic distribution of electrons with a power law in energies:
dN() -p d
dd
-(p-1)/2
Spectrum of Synchrotron radiation
Power law emission, extending to X-rayand -ray energies with index -(p-1)/2
Synchrotron radiation: continuum
Self-absorbed Synchrotron
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Bremsstrahlung (I)
Ingredients:• Totally or partially ionised
gas • Temperature T> 106 K
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Bremsstrahlung (II)
Electrons deviate from their trajectory when passingclose to an ion, accelerate and therefore radiate
b
velectron
Ion
Cutoff frequency: 0=v/2b
d
d const, for << 0
d
d e -/0, for >> 0
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Thermal bremsstrahlung
For a thermal distribution at temperature T
d
dV d Z2 ni ne T-1/2 g(,T) e-/kT
Ion’s atomicnumber
Temperature (K) Gaunt factor
d
dt dV = 1.43 10-41 Z2 T1/2 ni ne g(T) erg cm-3 s-1
(1+(kT/mc2)) (relativistic correction)
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Electron-positron pairs
Ingredients:
• Photons with energy > mc2
• “Compact” source
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Electron-positron pairs
Energetic condition for two photons to give rise to an electron-Positron pair (at rest):
E1 E2 > (mc2)2
0
0.05
0.1
0.15
0.2
0.25
0.3
0.6
0.9
1.2
1.5
1.8
2.1
2.4
2.7 3
3.3
3.6
3.9
4.2
4.5
4.8
(E1*E2)**(1/2) (MeV)
Sec
ció
n E
ficaz
The cross section isMaximal at ~ 1MeVAnd takes the value ~ 0.25 T
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Electron-positron pairs
Compactness: Optical depth of photon-photon collisions
=n R > 1
Photon density at~mc2
Crosssection
Size of emission region
Compactness parameter: =L T
Rmc3
~ /60 > 1
The compactness parameter must be >> 10
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Scattering Compton (I)Ingredients:
• Electrons
• PhotonsThomson classical h << mc2
Compton
Inverse h < mc2
Direct h > mc2
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Scattering ThomsonPhoton-electron interaction without energy transfer
d
dt d
3
8c T U sin2 =
d
dt= T c U
* For non-relativistic electrons
* For relativistic electrons:The Klein-Nishina cross section KN is a function of =h/mc2
KN~ T{1-2h/mc2+…} if h << mc2
KN~ (3/8)T (mc2/h){ln(2h/mc2)+1/2} if h >> mc2
Decreaseswith
h/mc2
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Compton effect
Transfer of energy between photons and electrons
Electron at rest: Eout=Ein
1+Ein/mc2(1-cos )
Moving electron: Eout~ 2 Ein
d
dt =(4/3) T c U (v/c)2 2
Power radiated by Compton effect
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
ComptonizationThe interaction of photons with a thermal electron gasChanges the photon energy at each collision
E
E
4kT-E
mc2=
The energy of the photonstends to equilibrate with thetemperature of the electrons
Compton depth: T= T dx ne
Number de collisionsper photon (Ncol):
~ T if T < 1
~ T2
if T >> 1
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Comptonization
Comptonization parameter: y=kT
mc2
Ncol
After Ncol collisions Eout=Ein e4y
Comptonized radiation tends to the Equilibrium Bose-Einstein distribution:
Planck spectrum if there is radiation-matterEquilibrium or otherwise a Wien spectrum
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Compton cooling
d
dt =(4/3) T c U (v/c)2 2
Compton energyloss for =mc2
For relativistic electrons ( >>1), the Compton coolingtime is:
tcool= /(d/dt)=tesc
3
In a compact source, electrons cool before escaping
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
A high-energy spectrum for compact sources
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Atoms and ionsEmission processes in Astrophysical plasmas T < 108 K:•Bremsstrahlung•Bound-bound emission lines (dominant up to 5 107 K)•Radiation recombination continua (capture
of a free electron to a bound state T< 107 K)•Di-electronic recombination lines (capture of a free electron
giving rise to a doubly excited state)•Two-photon continuum (Simultaneous emission of two photons from a meta-stable state)
Absorption processes in Astrophysical plasmas T < 108 K:•Photoionisation (free a bound electron) •Resonance absorption lines (bound-bound transition)
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Models of Astrophysical plasmas Ionisation Examples
Coronal <<1 collisions Stellar coronae SNR Intracluster gas
Nebular <1 Photo- ionisation
AGNs Planetary nebulae
Thick >>1 collisions Dense stars
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
The He-like triplet
1s2 1S
1s 2s 1S
1s 2p 1P1s 2p 3P
1s 2s 3S
Res
onan
ce E
1
Inter
combin
ation
E1+
M2
Forbidden M1
Nm
Nk
Coll excit
Ng
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Plasma diagnostics using He-like triplets
R=P(mg)
P(kg)
Forbidden
Interchange=
R=mg
kg
(1+ne/ncrit)-1
Ncrit=Amg kg
Smk (kg+mg)
A function of density
I
Akg
kg
Amg
mg
FSmk
: recombination, A: transition probs
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Photoelectric absorption
Absorption cross-section:
abs()7.8 10-18LL
( )3 Z4
n5cm2 for >LL
OVII K: 0.739 keVOVIII K: 0.874 keVFe I K: 7.1 keV
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Nuclear emission lines
Solar flare
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X/-ray instrumentation
1. Sources and processes in high-energy Astrophysics
Nuclear emission lines from SNeSN 1987A