MEDRADSC 2F03 Lecture Notes - Lecture 12: Photocathode, Ionization Chamber, Phosphorescence

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Energy is deposited in matter by ionization/scintillation
Energy is converted into thermal energy
Photons are tiny so the amount of energy deposited in matter is very small, so detectors need signal
amplification.
Methods of Detecting Radiation:
Light emission
Scintillation
o The intensity of light emitted is proportional to the amount of energy absorbed in the crystal
o Electron charge emission
o Gas-filled detectors (ionization chamber):
Consists of a cylinder of gas between 2 electrodes, ionization occurs and creates an arena for
the electrical impulses to be collected/measured
Dosimeter: indicate net amount of energy deposited in the detector by multiply interactions
Luminescence, Fluorescence, Phosphorescence
Luminescence: the ability of a material to emit light in response to excitation
o Wavelength: characteristic of luminescent material
Fluorescence: the ability to emit light instantly in response to excitation
o Prompt emission of light (within 10-8sec of stimulation)
o Fluorescent material:
Cesium Iodide (CsI), little balls of light, used in Image Intensifier
(II)fluoroscopy
X-ray exits pt and is transmitted through the glass
envelope and interacts with the input phosphor, which
emits light to the photocathode
Photocathode electrons move to anode, electrons go
through towards the output phosphor
Phosphorescence: the ability of a material (TLD or imaging plate) to delay
emission of light in response to excitation
o Electrons are trapped in some localized energy state
o TLD/CR imaging plates- exposed to x-rays/stored
o Thermoluminescence Dosimetry Steps:
Exposure to ionizing radiation
Heated
Will give off light in proportion to the dose
Measurement of the intensity of emitted light
Record with a Photomultiplier Tube (PMT)
o Lithium Fluoride (LiF)
Characteristic colour
Can be subdivided based on timing of response
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Document Summary

Energy is deposited in matter by ionization/scintillation: energy is converted into thermal energy, photons are tiny so the amount of energy deposited in matter is very small, so detectors need signal amplification. Idc: (-1 and +1, want it close to 0: agfa: (logarithmic mean, 1. 7-2 lgm, fuji: (s number, 150-250, as it increases, the dose goes down (backwards)) Phototimers: aec, coated with phosphor, pmt phototimer (aec) Increase in signal of the pmt depends on the number of dynodes, and the gain/amplification at each dynode: pmt gain = gn (g = dynode gain/amplification, n = # of dynodes) Digital radiography: radiographic imaging technology producing digital projection images such as those using: Indirect: psp (in cr, ir: direct, ampophous selenium, amorphous silicon, metal oxide semiconductor-field transistor (mosfet) charge-coupled device (ccd) In digital radiography, a digital computer is used to process attenuation data collected from pts using. Idc: f number: not enough exposure= grainy image.

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