Interactions of x- and γ- rays with matter: classical Scattering, photo-absorption/photoelectric effect, Compton scattering, pair- production & Photodisintegration
Radioactive decay law & Activity
Attenuation of radiation – absorption coefficients; attenuation of homogeneous and heterogeneous beams
Spectral lines are highly atom-specific, and can be used to identify the chemical composition of any medium capable of letting light pass through it (typically gas is used)
A discrete quantity of energy proportional in magnitude to a particular frequency (γ) of EM radiation and corresponding to a single photon or to a transition of an atom between two internal energy states
X-rays are produced when rapidly moving electrons that have been accelerated through a potential different of the order 10^3 - 10^6 volts strike a metal target
Electron are "boiled off" from the heated cathode by the principle of thermionic emission and these electrons accelerated towards the anode (the target) by a large potential different Vac
The most energetic photon (with λ and γ) is produce when all the electron's kinetic energy goes to produce on photon (bremsstrahlung limits)
Compton scattering (inelastic or non-classical) is the predominant interaction of x-ray photons in the diagnostic energy range with soft tissue
This interaction is most likely to occur between photons and outer ("valence") shell electrons, which are loosely bounded in the outer shell electron cloud
The ejected electron is called a Compton or recoil electron and scattered photon is called a Compton photon
The energy of the incident photon (Ei) is equal to the sum of the energy of the scattered photon (Esc) and the kinetic energy of the ejected electron (Ee-)
The freed electron possesses excess kinetic energy (Ek) and is capable of ionizing atoms
In diagnostic radiology, the probability of occurrence of Compton scattering relative to that of the photoelectric absorption is not influence increase as the energy of the x-ray photon increases