Brief explanation of what is PET, the main components for a PET system along with their basic functions. The principle behind PET inclusive of positron emission and emission detection. Acquisition and reconstruction of the collected data to produce the final image. Finally the pros and cons of Positron emission tomography.
2. Outline
Positron Emission Tomography
Definition
Clinical Application
Main System Components
Principle of PET
Image Acquisition
Image Reconstruction
Pros and Cons
Basic Configuration of PET Facility
References
3. What is PET??..
Positron Emission Tomography is an imaging technique
which uses small amounts of radiolabeled biologically
active compounds to help in the diagnosis of disease.
The tracers are introduced into the body, by either injection
or inhalation of a gas.
PET scanner is used to produce an image showing the
distribution of the tracer in the body.
4. Clinical Applications of PET
Oncology
Role in lesion detection, lesion characterization, staging of malignant lesions
and assessment of the therapeutic response
Brain
PET Study the brain's blood flow and metabolic activity. It aid in discovery of
nervous system problems, such as Alzheimer's disease, Parkinson's disease etc.
Heart
PET can help find damaged heart tissue especially after a heart attack and can
help choose the best treatment such as coronary bypass heart surgery for a
person with heart disease.
6. Main System Component…
Detector
Comprised of an 8 x 8 scintillation, inorganic crystals which emits
light photons after the interaction of photons
4 photomultiplier tubes (PMTs)
arranged in a circular pattern
around the patient
8. Main System Component
Septa
Lead or tungsten circular shield mounted between the detector
rings
Limits scattered radiation from the object reaching the detector
(scattered out the transverse plane)
9. Main System Component
Coincidence circuit
Specific electronic circuits "coincidence" circuits pick up gamma
pairs due to the two gamma rays emitted during the positron
annihilation almost simultaneously.
This coincidence is a very strong signature that distinguishes
them from other photons.
On the image it is requested that the signals coming from the
scintillators A and B coincide within 12 billionths of a second
(nanosecond).
10. Main System Component
Cyclotron
A machine used to produce the radioisotopes (radioactive
chemical elements) which are used to synthesize the
radiopharmaceuticals.
The most frequently used radioisotopes in PET are:
Carbon-11
Nitrogen-13
Oxygen-15
Fluorine-18
18FDG (Fluorodeoxyglucose) is the most widely used PET tracer.
11. Main System Component
Table
The bed is capable of moving in and out of the scanner to measure
the distribution of PET radiopharmaceuticals throughout the body,
and it adjusts to a very low position for easy patient access
Computer
A computer analyzes the gamma rays and uses the information to
create an image map of the organ or tissue being studied.
12. Principle of PET
Positron Emission
Positron Emission occurs when the isotope decays and a proton
decays to a Neutron, a Positron and a Neutrino.
After traveling a short distance (3-5mm), the positron emitted
encounters an electron from the surrounding environment.
The two particles combine and "annihilate" each other, resulting
in the emission of two gamma rays in opposite directions of 0.511
MeV each.
14. Principle of PET
Emission Detection
As positron annihilation occurs, the detector detects the isotope's
location and concentration
The resultant light photons are converted to electrical signals that
are registered by the system electronics almost instantly
The reconstruction software then takes the coincidence events
measured at all angular and linear positions to reconstruct an
image
17. Image Acquisition…
• The image acquisition is based on the external detection in
coincidence of the emitted Gamma rays.
• Valid annihilation event requires a coincidence within 12
nanoseconds between two detectors on opposite sides of the
scanner.
• For accepted coincidences, lines of response connecting the
coincidence detectors are drawn through the object and used in
the image reconstruction.
18. Image Reconstruction
Images are created from raw data collected as rays corresponding to each
detected annihilation event
The basic principles of tomographic image reconstruction from projections
of an object is common to CT.
19. Image Reconstruction…
Process…
The detectors collect a series of lines of responses LORs,
A profile of counts versus distance is produced for each angle of LORs
Each profile maps the location of the source in the direction parallel to the
scan profile (however, the source can lie at any depth along the line
perpendicular to that profile)
The source distribution can be obtained by projecting the data from each
scan profile back across the entire image grid. [backprojection]
20. Image Reconstruction…
Back projections of scan profiles at different angles are then added
together (linear superposition), to produce an approximation of the original
radioactivity distribution.
This operation is called linear superposition of back projections (LSBP).
There is an inherent blurring in this technique, which is removed by
performing a filtering operation on the projections or scan profiles
The entire reconstruction process is known as linear superposition of
filtered back projections (LSFBP).
21. Image Reconstruction
PET Reconstruction Algorithms
Filtered Back Projection
Simple
Quick
Streak artifacts
Iterative Reconstruction
Need fast computer
22. Pros and Cons
Advantages
Uniquely shows the chemical functioning
of organs and tissues
Detect functional changes
Study metabolic functions- may be an
alternative to biopsy.
Distinguish between benign and malignant
tumors- reducing unnecessary surgeries
due to misdiagnosis
Determine the spread of disease (cancer)
and function of the heart.
Diagnose early stages of neurological
illness, e.g. Epilepsy, Alzheimer's disease.
Disadvantages
Ionizing radiation
Radioactive compound is short lived.
Radioisotope must be produced in a
laboratory near the PET scanner.
25. References
Alessio AM, Kinahan PE, Cheng PM, Vesselle H, Karp JS. PET/CT scanner instrumentation,
challenges, and solutions. Radiol Clin N Am. 2004;42(6):1017-32.
Phelps ME, HotTman EJ, Mullani NA, Ter-Pogossian MM. Applications of annihilation
coincidence to transaxial reconstruction tomography. J Nucl Med 1975;16:210-224.
Valk PE, Bailey DE, Townsend DW, Maisey MN. Positron Emission Tomography: Basic
Science and Clinical Practice. London: Springer-Verlag; 2003.
Fahey H. F. Data Acquisition in PET Imaging, Journal of Nuclear Medical Technology; June
2002;30(2):39-49
Daghighian F., Sumida. R, Phelps E. M. PET imaging: An overview and instrumentation. J.
Nucl. Med. Technol. 1990;18:5-13.
ShuklaK. A, Kumar U. Positron emission tomography Scan; an overview J Med Phys. 2006
Jan-Mar; 31(1): 13–21. doi: 10.4103/0971-6203.25665
Ranger NT, Thompson CJ, Evans AC. The Application of a masked orbiting transmission
source for attenuation correction in PET. J Nucl Med. 1989;30:1056–68.