| Positron
Emission Tomography (PET) is an imaging modality that
can provide functional, metabolic and chemical information
to complement the more conventional, structural imaging
studies. PET essentially records the concentration of
positron emitting radioisotopes in a 3-D volume by obtaining
external measurements of the radiation emitted by these
isotopes. The data is generally acquired as a scaled
image of a cross-section of the object to be studied
( i.e. transaxially). The intensity of each picture
element or picture unit (pixel) is proportional to the
isotope concentration at that position in the object.
The most commonly used positron emitting radionuclides
are carbon, nitrogen, oxygen, and fluorine. These
radionuclides, which emit positrons, are normal components
of human tissues either individually or when coupled
with some other compound. PET, therefore, can provide
an in-vivo study of naturally existing compounds in
the human body.
A positron is a positively charged electron that is
emitted from the nucleus of a radionuclide. Once emitted
this positron (or anti-electron) travels several millimeters
until it meets a free electron from the surrounding
atoms, at which time an annihilation event takes place.
The masses of the electron and positron are converted
to electromagnetic radiation. Due to conservation
of energy and momentum, two "annihilation" photons
appear (two gamma rays). The total energy of these
two photons will equal the rest mass of the original
electron and positron (511 keV) and they will be emitted
in a 180 degree opposite direction to one another.
A ring of detectors surrounds the patient and when
two 511 keV gamma rays are simultaneously recorded
by opposing detectors, an annihilation event is known
to have taken place on or about a line connecting
the centers of the two detectors. PET, therefore,
uses the principle of annihilation coincidence detection.
To
be recorded as an annihilation coincidence event,
the gamma rays detected by the opposing detectors
must occur within a very short interval of time called
the coincidence window, which is usually ten to twenty
nanoseconds. The PET scanner continuously records
the coincidence events, and this data must be manipulated
to generate images. In the past, filter back projection
was used, but a newer technique called iterative reconstruction
is favored because it eliminates some of the artifacts
generated with filtered back projection. The reconstructed
data can be displayed in a three dimensional rotating
volume as well as standard tomographic slices in the
transaxial, coronal, and sagittal planes.
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