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Movies available at: http://www.mso.anu.edu.au/~geoff/CentaurusA and http://www.mso.anu.edu.au/~geoff/PGN09

Centaurus A: Some Core Physics
Credit: Helmut Steinle http://www.mpe.mpg.de/~hcs/Cen-A/

Geoff Bicknell1 Jackie Cooper1 Cuttis Saxton1 Ralph Sutherland1 Stefan Wagner2 1. Research School of Astronomy Astrophysics, ANU 2. Landessternwarte, University of Heidelberg


This talk

· Transition to turbulence · TeV emission · Jet-cloud interactions in core

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Transition to turbulence
Transonic flow

Flaring region: supersonic -> transonic transition

Relativistic supersonic jet

Credit: Hardcastle et al. 2003

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Decelerating relativistic jets (GB ApJ `95)
c2 R= 4p

Perturbation V

Critical Mach Number Mc = 1 + sec2 -
2

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Expect transition to turbulent flow around ~ 0.6 ­ 0.8 Laing and colleagues: Analysis of brightness asymmetries of 8 FR1 jets ­ Transition occurs around 0.8 c

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From GB, ApJ, 1984

·Transition to fully turbulent

flow involves immersed shocks

· Symmetric shocks perturbed
by m=1 KH instability

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TeV emission: Example PKS 2155-304

Credits: Piner, Plant & Edwards

Credits: HESS consortium

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Example of fitting spectrum

ATOM

RXTE Swift

HESS

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Example of fitting spectrum
1 b 2

= = =

2.0 eV 2.5 в 103 eV 3.0 в 10
4

ATOM

RXTE Swift

HESS

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Example of fitting spectrum
1 b 2

= = =

2.0 eV 2.5 в 103 eV 3.0 в 10
4

1 b 2

= 8.5 в 10 = 3.0 в 10 = 1.4 в 10

3 5 6

ATOM

RXTE Swift

HESS

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Example of fitting spectrum
1 b 2

= = =

2.0 eV 2.5 в 10 eV
3

3.0 в 10

4

3e = B 2 me c

1
2

b 2

= 8.5 в 10 = 3.0 в 10 = 1.4 в 10

3 5 6

ATOM

RXTE Swift

HESS

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Example of fitting spectrum
1 b 2

= = =

2.0 eV 2.5 в 10 eV
3

3.0 в 10

4

3e = B 2 me c B R = 0.040 G = 3.3 в 10 = 40

1
2

b 2 cm
-3

= 8.5 в 10 = 3.0 в 10 = 1.4 в 10

3 5 6

ATOM

16

K

RXTE Swift



= 6.5 в 107 cm

HESS

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Shock spectrum
If electrons accelerated at shock and cool in constant magnetic field in a region of size L then volume averaged shock spectrum given by:
Ї N ( ) = = where b = K b a-1 K b a-1 vsh AL a-1 1 - (1 - ) b > b

-(a+1) -(a+1)

< b

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Soft photon spectrum
· Klein-Nishina effects limit soft photons to low energy and
scattering electrons to high energy
<
2

0

(me c2 )2
2 -1 -1

0.26 >

TeV

me c2

2.0 в 106

TeV

· Soft photon input: 0.1 x Blackbody with mean temperature ~
200 K
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AX1C ­ possible site of TeV emission
Hard X-ray synchrotron spectrum indicates reasonable population of high energy electrons

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Centaurus A
Unusual spectrum ­ extending from peak at ~ 100 keV to beyond a TEV

External Inverse Compton "fit"

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Parameters
a=
b

2 0.8 22 1.0 в 10 2 в 10
8 5

= = = = = =

0.2 eV

= 60 = 1.44


1 b 2 B T
dust dust

Energy density = 1.3 в 10 = 200 K = 0.1

8.0 в 10

-4

-10

= 2 в Equipartition ergs cm
-3

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PPMLR simulation code

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PPMLR simulation code
Based upon Godunov method of numerical hydrodynamics

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PPMLR simulation code
Based upon Godunov method of numerical hydrodynamics Piecewise Parabolic Method with Lagrangian remap (PPMLR) and Riemann solver

Many Faces of Centaurus A Sydney July 2009

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PPMLR simulation code
Based upon Godunov method of numerical hydrodynamics Piecewise Parabolic Method with Lagrangian remap (PPMLR) and Riemann solver Originated from VH1 code (University of Virginia and University of Nth Carolina)

Many Faces of Centaurus A Sydney July 2009

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PPMLR simulation code
Based upon Godunov method of numerical hydrodynamics Piecewise Parabolic Method with Lagrangian remap (PPMLR) and Riemann solver Originated from VH1 code (University of Virginia and University of Nth Carolina) Added cooling of thermal gas

Many Faces of Centaurus A Sydney July 2009

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PPMLR simulation code
Based upon Godunov method of numerical hydrodynamics Piecewise Parabolic Method with Lagrangian remap (PPMLR) and Riemann solver Originated from VH1 code (University of Virginia and University of Nth Carolina) Added cooling of thermal gas Code for correcting numerical shock instabilities
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Jet + Disk simulations (Sutherland & GB 2007, ApJS, 173)
Description of the ambient cloudy medium Log-normal density distribution ­ affects the porosity of the medium Kolmogorov power-law of density in Fourier space Both arise naturally in a turbulent medium

Many Faces of Centaurus A Sydney July 2009

Mean density that of an almost Keplerian disk supported vertically by thermal and supersonic turbulent pressure.

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Initial mean density

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Initial mean density

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Initial mean density
2-component dark + luminous matter potential

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Initial mean density
2-component dark + luminous matter potential

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Initial mean density
2-component dark + luminous matter potential

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Parameters of jet and ISM
Relativistic equivalent
-3 43 -2

Scale = 1 kpc M LK n T
hot hot cl cl

= 26 = 2 в 10 = 2.8 в 10 ergs s cm
-1



=

=

5 c2 = 10 4p

= 8.4 в 10 = 10 cm = 10 K
4

-2

n Ї T

= 1.2 в 107 K
-3

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Jet and large scale disk
log (density)

Resolution = 5123
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Jet and large scale disk
log (density)

Resolution = 5123
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Jet and large scale disk
log (density) Evolutionar y phases:

Resolution = 5123
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Jet and large scale disk
log (density) Evolutionar y phases: Flood and channel

Resolution = 5123
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Jet and large scale disk
log (density) Evolutionar y phases: Flood and channel Pseudo-spherical energydriven bubble

Resolution = 5123
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Jet and large scale disk
log (density) Evolutionar y phases: Flood and channel Pseudo-spherical energydriven bubble Rapid jet breakout

Resolution = 5123
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Jet and large scale disk
log (density) Evolutionar y phases: Flood and channel Pseudo-spherical energydriven bubble Rapid jet breakout Classical radio galaxy phase

Resolution = 5123
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Pole-on view

Looking into the eye of the Vulcano

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Pole-on view

Looking into the eye of the Vulcano

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Radio morphology and dynamics

Synchrotron emissivity:
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Radio morphology and dynamics

Synchrotron emissivity:
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Comparison of adiabatic and radiative clouds - Jackie Cooper PhD thesis
Adiabatic

Radiative

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Comparison of adiabatic and radiative clouds - Jackie Cooper PhD thesis
Adiabatic

Radiative

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Comparison of adiabatic and radiative clouds - Jackie Cooper PhD thesis
Adiabatic

Radiative

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Hierarchy of scales (Saxton et al. 2005)

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That's it!

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