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Nuclear Medicine Principles & Technology_I Dr. Mohammed Alnafea [email protected] Nuclear medicine images 1. Single photon imaging a) Planar 2D image b) Single Photon Emission Computed Tomography (SPECT) 3D image 2. Positrons Emission Tomography (PET). All reveal the spatial and temporal distribution of target-specific pharmaceuticals in the human body. 2 9th lecture Nuclear Medicine Principles & Technology Non-invasive determination of physiologic processes Tracer principle: Radiopharmaceuticals are distributed, metabolized, and excreted according to their chemical structure Display of biological functions as: -Images -Numerical data -Time-activity curves 3 9th lecture Nuclear medicine images Depending on the application, the nuclear medicine data can be interpreted to yield information about physiological processes such as : 1. glucose metabolism. 2. blood volume, flow and perfusion. 3. tissue and organ uptake. 4. receptor binding, and oxygen utilization. 4 9th lecture Tracer Principle 5 9th lecture Common Radio-nuclides 6 Nuclides Half lives TC-99m 6h Tl-201 73 h I-123 13 h I-131 8d 9th lecture Type Energy (keV) 140 70 159 364 Radiopharmaceutical Selection of pharmaceutical based on organ-specific question. Labeling of pharmaceutical with radioactive isotopes. Radiopharmaceuticals should not disturb the process under investigation 7 9th lecture Ideal Radiopharmaceuticals Low radiation dose High target/non-target activity Safety Convenience Cost-effectiveness Only emit gamma Produced by generator 8 9th lecture 9 9th lecture Mechanisms of Localization Compartmental localization and leakage Cell sequestration Phagocytosis Passive diffusion Metabolism Active transport 10 9th lecture Localization (cont.) Capillary blockade Perfusion Chemotaxis Antibody-antigen complexation Receptor binding Physiochemical adsorption 11 9th lecture Half-Life (HL) • Physical Half-Life Time (in minutes, hours, days or years) required for the activity of a radioactive material to decrease by one half due to radioactive decay • Biological Half-Life Time required for the body to eliminate half of the radioactive material (depends on the chemical form) • Effective Half-Life • • The net effect of the combination of the physical & biological halflives in removing the radioactive material from the body Half-lives range from fractions of seconds to millions of years 1 HL = 50% 2 HL = 25% 3 HL = 12.5% 9th lecture 12 Nuclear Imaging 13 9th lecture Interaction of Photons with Matter Pass through unaffected (i.e. penetrate) Absorbed (and transfer energy to the absorbing medium) Scattered (i.e. change direction and possibly lose energy) 14 9th lecture Main Interactions of gamma-rays with matter when used for imaging Photo-electric absorption Compton Scattering 15 9th lecture Photoelectric absorption An incident photon is completely absorbed by an atom in the absorber material, and one of the atomic electrons is ejected. This ejected electron is known as a photoelectron. The electron must be bound to the atom, to conserve energy and momentum. 16 9th lecture The Photoelectric Effect In the photoelectric effect the photon interacts with an orbital electron and disappears, while the electron is ejected from the atom thus ionising it. The energy of the photoelectron is given by Ek = hν – EB Where Ek is the kinetic energy of the ejected electron, hν the energy of the photon and EB the binding energy of the electron. 17 9th lecture Compton Scattering In this case, an incident gamma ray scatters from an outer shell electron in the absorber material at an angle , and some of the gamma ray energy is imparted to the electron. 18 9th lecture All interaction 19 9th lecture General-Purpose Circular Detector High-Performance Circular Detector 20 9th lecture The gamma camera 21 9th lecture Gamma Camera Components Photomultipliers Scintillator Collimator Organ to be imaged Typically: 40cm × 55cm NaI(Tl) scintillator Spatial resolution ~ a few mm Use of large collimator not efficient relatively large radiation dose needed to be given to patient. 22 9th lecture The modern gamma camera consists of: - multihole collimator - large area NaI(Tl) (Sodium Iodide Thallium activated) scintillation crystal - light guide for optical coupling array (commonly hexagonal) of photo-multiplier tubes - lead shield to minimize background radiation 9th lecture 23 Features and parameters of the scintillation crystal The following are the typical features of the scintillation crystal used in modern gamma cameras most gamma cameras use thallium-activated (NaI (Tl)) NaI(Tl) emits blue-green light at about 415 nm the spectral output of such a scintillation crystal matches well the response of standard bialkali photomultipliers . the linear attenuation coefficient of NaI(Tl) at 150 KeV is about 2.2 1/cm . Therefore about 90% of all photons are absorbed within about 10 mm NaI(Tl) is hyrdoscopic and therefore requires hermetic encapsulation 24 9th lecture • NaI(Tl) has a high refractive index ( ~ 1.85 ) and thus a light guide is used to couple the scintillation crystal to the photomultiplier tube • the scintillation crystal and associated electronics are surrounded by a lead shield to minimize the detection of unwanted radiation • digital and/or analog methods are used for image capture 25 9th lecture Camera component 26 9th lecture collimator A crucial component of the modern gamma camera is the collimator. The collimator selects the direction of incident photons. For instance a parallel hole collimator selects photons incident the normal. The action of a parallel hole collimator 9th lecture 27 Pinhole Collimator Other types of collimators include pinhole collimator often used in the imaging of small superficial organs and structures (e.g thyroid,skeletal joints) as it provides image magnification. Detail of the pin-hole collimator 9th lecture 28 Collimator 29 9th lecture Collimator Defines the spatial resolution of the system 30 9th lecture Collimator Septa designed for specific gamma ray energy: e.g. length 35 mm distance 1.5 mm thickness 0.2 mm 31 9th lecture Again Camera components 32 9th lecture Gamma Camera Components 33 9th lecture Principle of Scintillation detector 34 9th lecture Scintillator 35 9th lecture Anger (gamma) camera 36 9th lecture Energy Signal 37 9th lecture Ideal Energy Spectrum 38 9th lecture Projections 39 9th lecture Real Energy Spectrum 40 9th lecture Camera specification Detector size ca. 50 cm x 60 cm ca. 60 photomultiplier tubes per detector Energy resolution @140 keV< 10% Intrinsic spatial resolution: 3,5 -4 mm Extrinsic spatial resolution (Collimator): 8 -20 mm 41 9th lecture Examples 42 9th lecture Nuclear medicine image 43 9th lecture Renal Scan 44 9th lecture My time is up! Any questions ?? 9th lecture 45