phy232topic7.ppt

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Topic 7. Gamma Camera (I) • General Comments • Basic Principles of the Anger Camera • Types of Gamma Cameras

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Transcript of phy232topic7.ppt

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Topic 7. Gamma Camera (I)

• General Comments

• Basic Principles of the Anger Camera

• Types of Gamma Cameras

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General Comments

• Why γ rays? (penetrating through the body, easily stopped by lead, β emission or Auger electrons can not get out of body)

• Why NaI(Tl) detector (reasonable compromise between efficiency and cost etc. )

• Historically, γ ray imaging started from matrix detectors of late 40s to rectilinear scanner, and to the Anger scintillation camera of late 50s which is the most used today.

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Basic Principles of the Anger Camera

• System Components

• Detector System and Electronics

• Collimators

• Event Detection in Gamma Cameras

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System Components

• Collimator

• NaI(Tl) crystal

• Light Guide (optical coupling)

• PM-Tube array

• Pre-amplifier

• Position logic circuits (differential&addition etc.)

• Amplifier (gain control etc)

• Pulse height analyzer

• Display (Cathode Ray Tube etc).

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NaI(Tl) Crystal Assembly

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Detector System and Electronics(1)

• Typical detector in Anger camera: NaI(Tl) crystal with 1.25cm thick x 30-50 cm in diameter (thinner for low energies, 6mm)

• Thinner crystal is preferred for Anger camera in order to get better intrinsic resolution therefore better image (sacrifice intrinsic efficiency)

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Detector System and Electronics(2)

• Optical coupling materials (silicon fluid, grease, or lucite light pipes) are placed between the NaI(Tl) crystal and the array of photomultiplier tubes --called light guide or pipe

• Array of PM tubes (37,61,75 or 91, round, hexagonal or square shapes) arranged in hexagonal pattern

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Detector System and Electronics(3)

• Part of the signal processing circuitry (preamplifier, pulse height analyzers, amplifier, pulse pile-up rejection etc.) is attached to each PM tube and sealed in a light-tight protective housing

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Position Circuitry(1)

• The photomultiplier tubes are divided into horizontal halves to obtain X+ and X- signals and vertical halves to obtain Y+ and Y- signals.

• Four summing matrix circuits are used to sum up for x+,x-,y+ and y- signals from each TM tubes where each of these signals is the product of signal amplitude and position factor.

• A separate summing circuit is used to sum up a total signal Z from all PM tubes (signal amplitude only, no position factor)

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Light Sharing Between PM Tubes

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Position Circuitry(2)

• The radiation position is then determined by X=k(X+-X-)/Z and Y=k(Y+-Y-)/Z where k is a scale constant, Z is the total signal amplitude and proportional to the incoming radiation energy.

• The positional signals X and Y must be normalised by total signal Z because X and Y themselves depend on the both signal and positional factors (different radiation energy gives different signal amplitude at the same position)

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PM Tubes and Signal Positions

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PMT Energy Window Correction

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Pulse Height Displays

• Pulse height analyzer is used to analyse the Z signal and if accepted, signal will be displayed on the monitor (CRT etc.) at the position determined by X and Y.

• Two kind of display modes can be used to display the energy spectrum, namely, Z pulse display and multi-channel analyzer display.

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Collimators

• Absorptive collimation is used for most γ ray image formation (inefficient method for utilisation of radiation)

• Four basic collimator types are used with Anger camera and similar camera-type imaging device: pinhole, parallel hole, diverging and converging collimators.

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Parallel-Hole Collimator

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Pinhole Collimator(1)

• A cone shape lead with a small pinhole of a few millimeter in diameter, about 20-25 cm from the pinhole aperture to the detector.

• The image is inverted and could be magnified or minified depend on the object position: I/O=f/b where I and O are image and object sizes respectively, f is the distance between the pinhole and the detector, b is the distance between the object and the pinhole.

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Pinhole Collimator(2)• The size of the imaged area changes with

the distance between the object and the collimator b: D’=D/(I/O) where D is the diameter of the detector and D’ is the images area.

• Image size changes with the distance between the object and the collimator b, therefore, image is distorted in 3 dimension.

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Parallel Hole Collimator• Parallel holes are drilled or cast in lead

• Sept is the walls between holes and its thickness is chosen to prevent γ rays from crossing from one hole to the next.

• Image is the same size as the source distribution to the detector.

• Slant-hole collimator is a titled parallel holes collimator.

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Diverging Collimator• Diverging from the collimator face towards the object.

• The converging point is about 40-50cm behind from the collimator.

• Image is minified: I/O=(f-t)/(f+b) where f is the distance between the front of the collimator and the converging point, t is the thickness of the collimator and b is the distance between the object and the front of the collimator.

• Useful image area becomes larger as the image becomes more minified. Image size depends on the object distance b (image has distortion).

• Useful for small detector to image large organ.

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Converging Collimator• Holes converge to a point in front of the collimator (about

40-50 cm from the collimator)

• Images are magnified & non-inverted if the objects are placed between the converging point and the collimator surface: I/O=(f+t)/(f+t-b). (image distortion due to b dependence)

• Images are inverted & magnified if the objects are placed between the converging point and twice the convergence length and an inverted & minified image beyond that distance (not often used).

• Useful for using large detector to image small organs

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Parallel vs Converging Collimators

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Gamma Camera Detection Events

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Image Display and Recording Systems(1)

• Persistence CRT: displays light spots that do not fade immediately

• Non-persistence CRT: display images for film decording

• Polaroid film is convenient in use but expensive. It is a positive type and has limited range of optical densities (limit both contrasts and latitude, the useful exposure range)

• Transparency film is a negative film type (darker for greater exposure) and has better contrasts and latitude than Polaroid film

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Image Display and Recording Systems(2)

• Polaroid cameras often have three separate lenses, with different lens aperture opening, to provide three deferent densities on a single film simultaneously.

• Laser film printers are now replacing the old film making practice in nuclear medicine.

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Stationary or Mobile

• Anger camera can be sued for static or dynamic imaging

• Stationary cameras are designed to be at a fixed location while mobile camera has wheels.

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Types of Gamma Camera

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Types of Gamma Camera

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Types of Gamma Camera

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Scanning Camera• Scanning Anger cameras are used for

whole body imaging

• Either detector or patient support table may be set to move

• Diverging collimator may be used to cover entire width of the patient’s body.

• Whole body images can be printed on a single film.

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Whole Body Bone Scan

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Dynamic Sequence of Planar Images

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