Abstract
The application of a radiotracer technique to measure physiologic parameters, such as pulmonary circulation, dates back to 1927. Despite considerable advances in the application of radiotracer technique for interrogating physiologic and pathophysiologic cardiopulmonary conditions in the early twentieth century, the spatial resolution of the scintigraphic instruments used to measure tracer concentration in the heart, lungs, and blood was limited. The advent of single-photon emission CT (SPECT) in the late 1970s and positron emission tomography (PET) in the 1980s dramatically changed the clinical utility of radiotracer technique for the assessment of myocardial perfusion, viability, and function.
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Keywords
- Positron Emission Tomography
- Myocardial Blood Flow
- Cadmium Zinc Telluride
- SPECT Camera
- Radiotracer Technique
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The application of a radiotracer technique to measure physiologic parameters, such as pulmonary circulation, dates back to 1927. Despite considerable advances in the application of radiotracer technique for interrogating physiologic and pathophysiologic cardiopulmonary conditions in the early twentieth century, the spatial resolution of the scintigraphic instruments used to measure tracer concentration in the heart, lungs, and blood was limited. The advent of single-photon emission CT (SPECT) in the late 1970s and positron emission tomography (PET) in the 1980s dramatically changed the clinical utility of radiotracer technique for the assessment of myocardial perfusion, viability, and function.
Both SPECT and PET technologies use similar reconstruction processes to obtain tomographic images of the heart. However, they differ in the type of radiopharmaceuticals and kind of instrumentation used to acquire cardiac images. SPECT allows a noninvasive evaluation of myocardial blood flow by extractable tracers such as 201Tl- and 99mTc-labeled perfusion tracers. PET, on the other hand, allows a noninvasive assessment of regional blood flow, function, and metabolism using physiologic substrates prepared with positron-emitting isotopes such as carbon, oxygen, nitrogen, and fluorine. Radioisotopes commonly used with SPECT emit γ-rays of varying energies and have relatively long physical half-lives. The localization of γ-rays emitted by single-photon–emitting radiotracers in the heart is conventionally accomplished by an Anger scintillation camera (gamma camera), which converts the γ-rays to light photons via sodium iodide scintillation detectors. The gamma camera limits the direction of photons entering the detector by a collimator and then positions each event electronically. More recently, new designs of high-speed SPECT cameras have been introduced, which utilize a series of small, pixilated solid-state detector columns with cadmium zinc telluride or CSI (Tl) crystals, which provide considerably more information for each detected γ-ray. In addition, the design of the solid-state detector design with wide-angle tungsten collimators combined with a novel image reconstruction algorithm provide true three-dimensional, patient-specific images localized to the heart. Compared with the conventional SPECT cameras, the high-speed SPECT systems can provide up to an eightfold increase in count rates, thereby reducing imaging times significantly from 14 to 15 min with a conventional Anger camera to 5–6 min with the newer solid-state cameras, while achieving a twofold increase in spatial resolution from 9 to 12 mm for Anger cameras to 4.3–4.9 mm for cadmium zinc telluride cameras. The radioisotopes used for optimal scintigraphic registration with SPECT cameras are limited to those that emit γ-rays with an energy range that is suitable for the gamma camera and related single-photon devices such as 201Tl, 99mTc, and 123I. Although clinically useful, estimates of relative myocardial blood flow by SPECT are significantly affected by attenuation artifacts that are not reliably corrected for when compared to PET attenuation correction algorithms.
Positron-emitting radioisotopes commonly used with PET emit two γ-rays, 511 keV each, and have relatively short physical half-lives. When the high-energy positron is emitted from a nucleus, it travels a short distance and collides with an electron. The result is complete annihilation of both the positron and the electron, and the conversion of the combined mass to energy in the form of electromagnetic radiation (two γ-rays, 511 keV energy each). Because the γ-rays are perfectly collinear (discharged at 180° to each other) and travel in opposite directions, the PET detectors can be programmed to register only events with a temporal coincidence of photons that strike directly at opposing detectors. This results in improved spatial (4–6 mm) and temporal resolution. Moreover, the PET system is more sensitive than a SPECT system (higher count rate) and provides a more robust soft tissue attenuation correction. The consequence of these advantages with PET is the possibility for a quantitation of the tracer concentration in absolute units.
Myocardial Perfusion, Uptake, and Clearance
Image Interpretation and Quantitation
SPECT Techniques: 201TI
SPECT Techniques: 99mTc-labeled Perfusion Tracers
PET Tracers and Techniques
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Dilsizian, V., Dilsizian, V. (2013). SPECT and PET Myocardial Perfusion Imaging: Tracers and Techniques. In: Dilsizian, V., Narula, J. (eds) Atlas of Nuclear Cardiology. Springer, New York, NY. https://doi.org/10.1007/978-1-4614-5551-6_2
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