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Compton Scattering in Strong Magnetic Fields

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Compton Scattering in Strong Magnetic Fields Department of Physics National Tsing Hua University G.T. Chen 2006/5/4 Outline Motivation Relativistic Landau Level ... – PowerPoint PPT presentation

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Title: Compton Scattering in Strong Magnetic Fields


1
Compton Scattering in Strong Magnetic Fields
  • Department of Physics
  • National Tsing Hua University
  • G.T. Chen
  • 2006/5/4

2
Outline
  • Motivation
  • Relativistic Landau Level
  • Compton Scattering
  • Results
  • Discussion and Future Work

3
Motivation
  • The isolated neutron star 1E1207.4-5209
  • Four absorption features are seen in the pn
    spectrum at the harmonically spaced energies of
    0.7kev , 1.4kev , 2.1kev , 2.8kev

A. De Luca et al. ,AA ,2004
4
Motivation
  • Using three independent statistical analyses
    indicated that there is no third or four line.
    (Kaya Mori et al.,ApJ,2005)
  • Spectral lines
  • observed timing B 2.6 x1012 G
  • cyclotron lines B 8 x1010 G (electron)
  • B 1.6 x1014 G
    (proton)
  • ? We attempt to construct a model finding
  • the origin of these lines

5
Motivation
  • Compton Scattering
  • Bremsstrahlung

6
Relativistic Landau Level
7
Relativistic Landau Level
  • Dirac equation with magnetic field (
    )
  • Choose Landau gauge

8
Relativistic Landau Level
  • Assume
  • ?


9
Relativistic Landau Level
  • Energy eigenvalue
  • or

10
Compton Scattering
11
Compton Scattering
  • Feynman diagrams of Compton scattering

12
Compton Scattering
  • S-matrix
  • and
  • where

13
Compton Scattering
  • The differentiate cross section

14
Compton Scattering
  • Integrate final electron momentum

15
Compton Scattering
16
Compton Scattering
  • Integrate over the final photon azimuth and
    average over initial yields

17
Compton Scattering
  • We assume the distribution of initial electrons
    is 1D relativistic thermal distribution
  • K1modified Bessel fn. of the 2nd kind
  • T the electron temperature parallel to the
    field

18
Compton Scattering
  • From the energy conservation and parallel
    momentum conservation, we have
  • where

19
Compton Scattering
  • Redistribution function
  • Apply into our case, because of the delta
    function of energy, the integration over momentum
    reduces to a summation.

20
Compton Scattering
  • Therefore, the Compton scattering differentiate
    cross section

21
Compton Scattering
  • 1

22
Results
23
Results
  • 1
  • 2

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29
Discussion Future Work
  • The relativistic calculation is given major
    correction
  • ? The appearance of higher harmonics

?The energy shift of the resonance ?The decrease
below the Thomson value at wgtwc
30
Discussion Future Work
  • Cold plasma ? hot plasma
  • Vacuum polarization should be included

31
Discussion Future Work
  • Two photon process

32
gtgtThank Youltlt
33
Compton Scattering
  • is the inverse of the half-life of the
    electron state j

H. Herold et al. ,AA, 1982
34
Compton Scattering
35
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Compton Scattering
37
?
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