Understanding Photodivision and Electrodivision in Electron Beam Oncology

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SUMMARY

The discussion focuses on the mechanisms of neutron production in electron beam oncology, specifically through photodivision and electrodivision. Photodivision refers to the fission of nuclei induced by bremsstrahlung photons, while electrodivision involves the contribution of electrons to neutron production. High-Z materials, particularly tungsten, are highlighted for their effectiveness in producing neutrons when subjected to electron beams, especially at energies exceeding 8-10 MeV. The conversation emphasizes the significance of understanding these processes for optimizing electron beam therapy.

PREREQUISITES
  • Understanding of electron beam oncology principles
  • Knowledge of bremsstrahlung radiation and its applications
  • Familiarity with neutron production mechanisms in high-Z materials
  • Basic concepts of nuclear fission and photodivision
NEXT STEPS
  • Research the role of tungsten in electron beam collimation
  • Study the effects of electron beam energy on neutron production
  • Explore the differences between photodivision and electrodivision processes
  • Investigate the applications of high-Z materials in radiation therapy
USEFUL FOR

Medical physicists, radiation oncologists, and researchers in the field of oncology who are interested in the mechanisms of neutron production and the optimization of electron beam therapies.

lavster
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Im reading a paper about use of electron beams in oncology and it says:

"The mechanism of neutron production in the region of electron beam energies under consideration is determined by photodivision of nuclei by bremsstrahlung photons and the small contribution of electrodivision by electrons".

what is photodivision and electrodivision? is this just fission induced by photons and electrons respectively? or is it a different process altogether?

thanks
 
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Usually, electron-beam oncology is by production of bremsstrahlung (photon) radiation, by stopping the electron beam in a high-Z (usually tungsten) target. High-Z collimators (also tungsten) are used to control the size and shape of the irradiated area. Tungsten is especially useful for a collimator because of its high density.

All elements have a photo-neutron cross section (γ,n) for producing free electrons. With few exceptions, the High-Z materials like tungsten have a lower threshold (6 to 8 MeV) and a higher "giant dipole resonance" peak neutron production cross section, sometimes over 1 barn per atom. This photo-neutron production greatly increases with electron-beam energies over 8-10 MeV, and effectively limits the electron beam energy used for electron-beam oncology. Usually, the direct electroproduction of neutrons is much smaller, when compared to the electron-bremsstrahlung-photoproduction channel..

See thumbnail of neutron yields vs. electron beam energy in thick bremsstrahlung targets. Note that only uranium has a higher photoneutron yield than tungsten.
From http://www.google.com/url?sa=t&sour...puG6CQ&usg=AFQjCNFDwgclxNI5B5_Li3phSoXsuzy69g

Bob S
 

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excellent - thanks! :)
 

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