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Topic 5' Counting Systems I

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... product of intrinsic efficiency and photo-fraction ep=efp ... photopeak efficiency may be used to estimate the photo-peak counting rate. Sample Volume Effects ... – PowerPoint PPT presentation

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Title: Topic 5' Counting Systems I


1
Topic 5. Counting Systems (I)
  • NaI(Tl) well counter
  • Liquid and gas flow systems

2
NaI(Tl) Well Counter
  • Detector characteristics
  • Detection Efficiency
  • Sample volume effects
  • Assay of absolute activity
  • Shielding and background
  • Energy calibration
  • Multiple radionuclide source counting
  • Deadtime
  • Automatic multiple-sample systems
  • Applications

3
Detector Characteristics
  • Standard well counter (4.5x5cm crystal and
    1.6x3.8 well)
  • Background shielding (gt5cm lead)
  • Energy resolution 10-15 FWHM for 137Cs (poor
    light transfer between NaI(Tl) crystal and PM
    tubes-- light reflection and scattering within
    well surface)

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5
Well Counter
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Detection Efficiency
  • High geometric efficiency (near 100)
  • Good for counting of small sample activity
  • Intrinsic efficiency e depends on crystal
    thickness and ? ray energy (e100 for 1.3-4.5
    well thickness and ? ray energy less than 150
    keV).

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Detection Efficiency (2)
  • Photo-peak fraction decreases with increasing ?
    ray energy (scattering increases as ? ray energy
    increased within 0-2 MeV)
  • Photo-peak fraction increases with increasing
    well detector size (more multiple scattered
    photons added into the photopeak)

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Detection Efficiency (3)
  • Intrinsic photopeak efficiency is the product of
    intrinsic efficiency and photo-fraction epefp
  • Intrinsic photopeak efficiency may be used to
    estimate the photo-peak counting rate.

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14
Sample Volume Effects
  • Geometric efficiency of the well counter depends
    on the sample positioning
  • Geometric efficiency will decrease if the sample
    is displaced on top of the well.
  • For a constant activity, increase the volume by
    diluting the solution will decrease the counting
    rate
  • For a constant activity concentration, increase
    the volume will increase the counting rate and
    reach a maximum when the sample exceeds the top
    of the well.

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16
Assay of Absolute Activity
  • Two methods are used for the determination of
    absolute activity from the counting rate
    calibration table and calibration (standard)
    source
  • Long-lived radionuclides are used as calibration
    (mock) source 137Cs for 131I, 129I for 125I
    and 57Co for 99mTc.
  • Samples absolute activity X is given by X
    ?A(mock)R(sample)/R(mock), where A is mock
    activity and ? the ratio of emission frequencies

17
Shielding and Background
  • External sources of background radiation are
    minimised by surrounding the detector with lead
  • The thickness of the lead is typically 2.5-7.5cm.

18
Energy Calibration
  • Single channel analyzer attached to well counter
    is generally calibrated with 137Cs (1000
    divisions for 1Mev)
  • Adjust the amplifiers gain until maximum
    counting rate is observed with the window setting
    from 642 to 682 (662 is the centre).
  • 137Cs calibration is not accurate for energies
    below 100 keV because the non-linear energy
    response of NaI(Tl) detectors (re-calibration
    with low energy source)

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20
Multiple Radionuclide Source Counting
  • There is a crosstalk interference if multiple
    radionuclide source is counted simultaneously.
  • Correction is required in order to determine the
    true counts for each radionuclides photopeak.
  • The count ratios of its photo-peak to other
    radionuclides photo-peak energies should be
    measured by using single radionuclide sample and
    for each radionuclide involved.
  • For a two radionuclides system, the true counts
    for each radionuclide are Nt1(N1-R12N2)/(1-R12R21
    ) and Nt2(N2-R21N1)/(1-R12R21) where R12 and R21
    are the count ratios of pure sample at these two
    photo-peak energies (R12 from pure sample 2 etc.)

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22
Deadtime
  • Deadtime could be easily a problem for well
    counter because its high detection efficiency
  • For a small activity of 1 µCi with a deadtime 4
    µsec, about 5,000 cps could be lost if the
    detection efficiency is 100 (use
    RtRtexp(Rtt)).
  • Well counter is therefore good for detection of
    small radioactivity.

23
Automatic Multiple-Sample Systems
  • Automatic multiple sample systems are necessary
    for counting large number of samples or repeated
    tests
  • The main problem of the multiple sample well
    counters is the background shielding on top of
    the wells
  • SCA, MCA and computers are all being used for the
    interface with the detectors.

24
Multiple-Sample System
25
Multi-Sample Through-Hole System
26
Relative Efficiency
27
Applications
  • NaI(Tl) well counters are mainly used for in
    vitro assay in nuclear medicine (? or x rays)
    radioactivity in blood and urine sample,
    radiopharmaceutical quality control etc.
  • NaI(Tl) can also be used for ß emission by
    detecting bremsstrahlung radiation.

28
Liquid and Gas Flow Counting
  • NaI(Tl) well counters can be used in conjunction
    with gas or liquid chromatographs (identification
    of different chemical compounds)
  • Chromatographs are used to separate and identify
    different chemical compounds by selective
    retention or movement of chemical species in
    certain media
  • Different radioactive species are identified by
    comparing radioactivity with the flowing chemical
    species (mass signals).

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