Nuclear Medicine - Imaging Systems

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    IMAGING SYSTEMS

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    Imaging in Nuclear Medicine

    Radionuclide Imaging

    Gamma Camera

    PrinciplesSystem Components (Design)

    Detector SystemCollimators

    OperationHow Image is Formed

    Event Detection

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    Basic Performance Characteristics: Gamma Came

    Intrinsic Spatial Resolution

    Detection Efficiency

    Energy Resolution

    Limitations of DetectorNon-linearity

    Non-uniformity

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    SPECT

    Principles

    PET

    Principles

    PET ImagingHybrid Systems

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    IMAGING IN NUCLEAR MED

    Radionuclide imagingUse of radionuclides

    Oral or IV

    Recorded via external

    radiation detectorsEnergy range ~ 80 to 500

    keV

    Photon annihilation ~ 511keV

    Alpha particles and electrons Cannot penetrate tissues

    Bremsstrahlung

    More penetrating

    Weak intensity

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    IMAGING IN NUCLEAR MED

    Imaging Detector

    must have good detection efficiency for -rays

    must be able to discriminate energy (for rays w/positional info)

    NaI(Tl)Sodium Iodide doped with Thulium

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    GAMMA CAMERA

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    GAMMA CAM

    Anger Scintillation Camera

    Hal Ange

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    GAMMA CAMERA: DETES System Components

    Scintillation Crystal Light guide

    Photomultiplier tubes

    Collimator

    Analog-to-Digital Converter (ADC)

    Computer Monitor

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    GAMMA CAMERA: SCINTILLC

    Thallium dopedSodium IodideCrystal NaI(Tl)

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    GAMMA CAMERA: SCINTILLC

    Thallium doped Sodium Iodide Crystal NaI(Tl)Thickness: 6 to 12.5 mm

    Tradeoff between: Detection efficiency and Intrinsic sparesolution

    Size: 60 x 40 cm

    Diameter (round crystals): 25 to 50 cm diameter

    Highly reflective material (e.g. T maximize light output

    Hermetically sealed in Al-casin protection from moisture

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    GAMMA CAMERA: PM TUBELIGHT

    Photomultiplier Tubes

    Round PMT: arranged in hexagonal pattern tomaximize the area of NaI(Tl) crystal covered

    Typical diameter: 5 cm

    Most modern cameras: 30100 PMTs

    Use of hexagonal or square cross-sections of PMTs eliminates the use of

    light guides

    Light guides Channels light away from the gaps

    between PMTs

    increases collection efficiency Improves uniformity of light

    collection as function of position

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    GAMMA CAMERA: COLLIM

    CollimatorNarrows or aligns a beam or particle

    Allows the focusing of gamma cameras

    Pinhole Parallel Hole Diverging

    Basic Collimator types

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    GAMMA CAMERA: HOW IMFO

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    GAMMA CAMERA: HOW IMFO

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    GAMMA CAMERA: HOW IMFO

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    GAMMA CAMERA: HOW IMAGE IS

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    GAMMA CAMERA: EVENT DETE

    (A) Valid Event

    (B) Detector Scatter Event

    (C) Object Scatter Event

    (D) Septal Penetration

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    GAMMA CAMERA:PERFORMANCECHARACTERISTICS

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    PERFORMANCE CHARACTEINTRINSIC SPATIAL RESO

    Spatial Resolution

    Measure of sharpness and detail of image

    Ability of the camera to separate two objects as tmoved closer to each other

    Intrinsic Spatial Resolution

    Limit of spatial resolution achievable by the detecelectronics

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    PERFORMANCE CHARACTEINTRINSIC SPATIAL RESO

    Decreasing gamma-ray energydecrease in intrinsic resolution

    Lower energy gamma raysproduce fewer light photons per

    scintillation event

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    PERFORMANCE CHARACTEINTRINSIC SPATIAL RESO

    Increasing crystal thicknessdecrease in intrinsic resolution

    Thicker detectors result in greater spreadingof scintillation light before it reaches the PMtubes.

    Greater likelihood of detecting multiple

    Compton-scattered eventsparticularly inhigh energy radionuclides.

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    PERFORMANCE CHARACTEINTRINSIC SPATIAL RESO

    Increasing efficiency of collection of scintillation pho

    Improves intrinsic resolution

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    PERFORMANCE CHARACTEDETECTION EFFIC

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    PERFORMANCE CHARACTEENERGY RESO

    Energy resolutionAbility of the detector to accurately determine the energy

    incoming radiation

    Ex: For a 10% Energy Resolution:

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    DETECTOR LIMITA

    Image NonlinearityResults when X- and Y- position signals do not change linearly with d

    distant of radiation source across the face of the detector.

    Pincushion Distortion Barrel Distortion

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    DETECTOR LIMITA

    Image Non-uniformity

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    SPECT: SINGLE PHOTON

    EMISSION COMPUTEDTOMOGRAPHY

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    SPECT: PRINPrinciples

    Similar to planar imagingusing gamma camera

    Captures multiple 2Dimages (projection) frommultiple angles

    Tomographicreconstruction is applied tothe projections

    Yields a 3D dataset

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    SPECT: PRIN

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    SPECT: IM

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    PET: POSITRON EMISSIOTOMOGRAPHY

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    PET: PRIN

    Functional imaging technique

    Detects gamma rays indirectly

    Emitted by a positron-emitting radionuclide

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    PET: PRIN

    Positron Emission and Annihilation

    Positron annihilates with electron Two 511 keV photons

    Photons are anti-parallel

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    PET: PRIN

    Annihilation CoincidenceDetectionEach detector generates

    a timed pulse when itregisters an incidentphoton

    When pulses are withinthe timed window, theyare consideredcoincident

    Coincident events areassigned to a lineresponseprovidespositional informationwithout using a physicalcollimator

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    PET: PRIN

    Coincident Events

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    PET IMA

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    PET IMA

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    HYBRID SYSTEMS:SPECT/CT AND PET/CT

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    WHY USE HYBRID SYS

    SPECT AND PET Provides functional information

    using radiotracers Designed to measure

    physiologic or metabolicparameters

    Anatomical information isimportant to determine thelocation of activity

    X-Ray CT Consists of x-ray tube with a

    detector array mounted on arotating gantry

    Can provide anatomicalinformation

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