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Topic 7. Gamma Camera I

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Title: Topic 7. Gamma Camera I


1
Topic 7. Gamma Camera (I)
  • General Comments
  • Basic Principles of the Anger Camera
  • Types of Gamma Cameras

2
General Comments
  • Why ? rays? (penetrating through the body, easily
    stopped by lead, ß emission or Auger electrons
    can not get out of body)
  • Why NaI(Tl) detector (reasonable compromise
    between efficiency and cost etc. )
  • Historically, ? 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.

3
Basic Principles of the Anger Camera
  • System Components
  • Detector System and Electronics
  • Collimators
  • Event Detection in Gamma Cameras

4
System Components
  • Collimator
  • NaI(Tl) crystal
  • Light Guide (optical coupling)
  • PM-Tube array
  • Pre-amplifier
  • Position logic circuits (differentialaddition
    etc.)
  • Amplifier (gain control etc)
  • Pulse height analyzer
  • Display (Cathode Ray Tube etc).

5
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6
NaI(Tl) Crystal Assembly
7
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)

8
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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12
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

13
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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15
Light Sharing Between PM Tubes
16
Position Circuitry(2)
  • The radiation position is then determined by
    Xk(X-X-)/Z and Yk(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)

17
PM Tubes and Signal Positions
18
PMT Energy Window Correction
19
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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21
Collimators
  • Absorptive collimation is used for most ? 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.

22
Parallel-Hole Collimator
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24
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/Of/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.

25
Pinhole Collimator(2)
  • The size of the imaged area changes with the
    distance between the object and the collimator b
    DD/(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.

26
Parallel Hole Collimator
  • Parallel holes are drilled or cast in lead
  • Sept is the walls between holes and its thickness
    is chosen to prevent ? 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.

27
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)/(fb) 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.

28
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(ft)/(ft-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

29
Parallel vs Converging Collimators
30
Gamma Camera Detection Events
31
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.

34
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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36
Types of Gamma Camera
37
Types of Gamma Camera
38
Types of Gamma Camera
39
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 patients body.
  • Whole body images can be printed on a single film.

40
Whole Body Bone Scan
41
Dynamic Sequence of Planar Images
42
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