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NEEP 541 Radiation Interactions

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Neutrons can be captured, form compound nucleus; then ... Electron mean kinetic energy, eV. 6. 1. 10 - 1000. Plasma density, cm-3. Solar wind. Plasma sheet ... – PowerPoint PPT presentation

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Title: NEEP 541 Radiation Interactions


1
NEEP 541Radiation Interactions
  • Fall 2003
  • Jake Blanchard

2
Outline
  • Elementary Particles
  • Electrons
  • Ions
  • Neutrons
  • Photons
  • Radiation in Space
  • Photon Interactions
  • Charge Transfer

3
Elementary Particles
  • Photons
  • no mass
  • no charge

4
Elementary Particles
  • Electrons
  • Light
  • negatively charged
  • Rest mass0.51 MeV
  • Protons
  • Mass about 1837 times that of an electron
  • Positive charge
  • Neutron
  • Slightly heavier than proton
  • No charge

5
Neutrons
  • Flux is neutrons/area/time
  • Equivalent to beam intensity

6
Fission Energy Spectrum
7
Neutrons
  • Collisions are elastic or inelastic
  • Neutrons can be captured, form compound nucleus
    then nucleus emits neutrons, protons, gammas, or
    fission products
  • These products are recoils

8
Recoil and PKA spectra
recoils
PKAs
9
Gammas
  • Mean gamma energies are on the order of 100 eV
  • Negligible effect on displacements

10
Electrons
  • Charge implies short range, but low mass implies
    longer range
  • Most energy transfer is to other electrons in
    target
  • Collisions are coulomb
  • Must be relativistic to cause displacements (gt
    0.2 MeV)
  • Low temperature irradiation leads to homogeneous
    vacancy and interstitial distribution over about
    1 mm

11
Positive Ions
  • Light ions He, H, D (gt 1 MeV)
  • Heavy ions (lt1 MeV)
  • Fission products (100 MeV)
  • Inelastic losses low at low energy
  • Electrons dominate at high energy
  • Damage is narrower because range is smaller

12
Radiation in Space
  • Energies from keV to TeV
  • Particles are trapped by Earths magnetic field
    or pass through solar system
  • Trapped radiation is broad spectrum of charged
    particles (radiation belts)
  • Cosmic Rays are low fluxes of heavy ions beyond
    TeV
  • Solar Flares produce protons with energies to
    hundreds of MeV
  • Space is also pervaded by plasma of electrons and
    protons with energies around 100 keV

13
Energies
14
Belts
15
Plasma Conditions
Equilibrium Potentials at Increasing Altitude Equilibrium Potentials at Increasing Altitude
Ionosphere a few tenths of a volt negative
Magnetosphere normally, a few volts positive in eclipse, may become highly negative
Solar Wind a few volts positive
Interstellar Space a few volts positive or negative
16
More Plasma
Parameter Plasmasphere Plasma sheet Solar wind
Plasma density, cm-3 10 - 1000 1 6
Electron mean kinetic energy, eV 1 1000 15
Ion mean kinetic energy, eV 1 6000 10
Electron random current density, µA/m² 0.25 - 25 0.85 0.62
Ion random current density, µA/m² 0.006 - 0.6 0.05 0.012
Electron Debye length, m 2.5 - 0.25 240 12
17
Van Allen Belts
Inner Zone (lt 2.5RE) Outer Zone (gt 2.5RE)
Proton flux dominates About 10 times higher electron flux in outer zone than inner zone
Electron energies lt 5 MeV Electron energies around 7 MeV
Electron and proton fluxes peak at 1.5RE to 2.0RE Electron flux peaks at about 5RE
18
Cosmic Rays
  • 85 protons, 14 alpha particles
  • 1 nuclides with Zgt4 (ions of Zgt26 are rare)
  • energies from 0 to over 10 GeV
  • Most heavy ions are H, He, C, and O with peak
    energies around 1 GeV.
  • Cosmic rays have low flux but higher energy

19
Solar Flares
  • heaviest doses at solar maximum (10-12 yrs)
  • Flares produce heavy ions and protons (90,
    remainder is He, heavy ions, electrons)
  • Heavy ion fluxes from solar flares are generally
    less than galactic background but can be 4 times
    greater
  • Hheavy ion spectrum is less energetic than
    galactic cosmic ray spectrum
  • Solar protons are energetic (10 MeV to 1 GeV)
  • Protons from a single flare produce fluences up
    to 2x1010 p/cm2

20
Radiation Interactions
  • What happens when energetic particles interact?
  • Elastic Scattering
  • Inelastic Scattering
  • Bremsstrahlung Radiation
  • Accelerating charged particles emit radiation
  • Amplitude of radiation is proportional to
    acceleration

21
Photon Interactions
  • Photoelectric Effect low energy
  • Photon interacts with target electrons and is
    absorbed
  • Electron is ejected
  • Electron energy is photon energy minus binding
    energy
  • Binding energy reappears as x-rays

22
Photon Interactions
  • Compton Effect
  • Elastic scattering between photon and target
    electron
  • Electrons emitted in spectrum with average about
    2/3 of maximum

23
Photon Interactions
  • Pair production
  • Threshold energy is 1 MeV
  • Photon disappears and electron-positron pair is
    formed

24
Attenuation Coefficients
  • Measure of absorption of beam impinging on
    absorbing medium
  • Units are inverse length
  • Total attenuation coefficient is sum of
    contributions from three photon interaction
    effects

25
Attenuation of Photons in Air
26
Attenuation of Photons in Lead
27
Attenuation of Photons in Al
28
Charge Transfer
  • Radiation interactions result in the transfer of
    charge from one location to another
  • Electrons from photon interactions tend to be
    emitted with a forward bias, so there is a net
    charge transfer in the forward direction
  • For 1.3 MeV photons on Si, current is on the
    order of 10-21 C/photon (Compton scattering)

29
Forward Electron Current
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