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Understanding Neutron Radiography Post Exam Reading VIII-Part 2a of 2A

Understanding Neutron Radiography Post Exam Reading VIII-Part 2a of 2A

Understanding Neutron Radiography Post Exam Reading VIII-Part 2a of 2A

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The electron and positron, once liberated within the medium are dissipated<br />

through successive interactions within the medium. The electron is quickly<br />

absorbed, however the fate <strong>of</strong> the positron is not so straight forward. As it<br />

comes to a rest, it combines with a neighbouring electron and the two<br />

particles neutralise each other in a phenomenon known as annihilation<br />

radiation. Here, the two particles are converted back into two photons <strong>of</strong><br />

electromagnetic radiation, each <strong>of</strong> 0.511 MeV energy travelling at 180<br />

degrees to each other (a concept utilised in positron emission tomography -<br />

PET). These photons are then absorbed or scattered within the medium.<br />

Pair production in reality does not become the dominant process in water<br />

below about 30 MeV (due to its dependence on the 'Z' <strong>of</strong> absorber) and is<br />

therefore <strong>of</strong> less importance in the low atomic number s<strong>of</strong>t tissue elements. In<br />

industrial radiography where high atomic number elements are irradiated, pair<br />

production can become the major attenuation process assuming the incident<br />

radiation energy exceeds 1.022 MeV.<br />

Charlie Chong/ Fion Zhang<br />

http://radiopaedia.org/articles/pair-production

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