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Non-imaging devices  in Nuclear Medicine Pawitra Masa-at 4937092 SIRS/M March 23, 2007
Type of non-imaging device ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Radionuclide dose calibrators
Gas-Filled  Detectors I ; Ionization chamber region P ; Proportional region GM ; Geigur-Mueller region
[object Object],[object Object],[object Object],Ionization  Chamber
Ionization  Chamber HV + - Negative ion Positive ion 1234 Electrometer The response is proportional to ionization rate (activity, exposure rate)
Dose calibrators   ( Activity meter ) ,[object Object],[object Object],[object Object]
Dose calibrators ,[object Object],[object Object]
Dose calibrators SC97 Proportionality between the number of photons emitted and the ionization current Well-shaped ionization chamber filled with a gas of high atomic number (e.g. Xenon) and kept under pressure
Dose calibrators ,[object Object],[object Object],[object Object],[object Object],[object Object]
ACTIVITY MEASUREMENT Setting  Measured activity Tc-99m 1.00 Co-57 1.19 In-111 2.35 Tl-201 1.76 Ga-67 1.12 I-123 2.19 I-131 1.43 Measured activity/True activity of Tc.99m if the indicated settings are used
Geometric efficiency The quotient: number of photons reaching the detector over the number of photons emitted from the sample Increasing geometric efficiency
SAMPLE HOLDER (reproducible geometry)
Quality control of the dose calibrator. ,[object Object],[object Object],[object Object],[object Object],[object Object]
Sealed sources for calibration of activity meters ,[object Object],[object Object],[object Object],[object Object],Co-57, Ba-133, Cs-137, Co-60
Sealed sources for calibration of activity meters 1.9 5.27 y 1173, 1332 Co-60 7.4 30 y 662 Cs-137 9.3 10.7 y 81, 356 Ba-133 185 271 d 122 Co-57 Activity (MBq) Half-life Photon energy  (keV) Radionuclide
Measurement of precision and accuracy Source  (sealed) : Cs-137 or Co-57 Procedure:  Select settings for the radionuclide and adjust background. Insert source in holder and make 10 measurements. Data analysis :  To assess  precision , calculate for each source (i) the percentage difference between the measured activity A i  and their mean A mv . (+/-5%) To assess  accuracy , calculate the percentage difference between the mean activity and the certified activity. (+/- 10%).
Measurement of reproducibility Measure the activity of a sealed reference source e.g. every morning. Use Tc-99m  settings.
Measurement of reproducibility ,[object Object],[object Object],[object Object]
Measurement of linearity Use a radionuclide with short half-life e.g. Tc-99m Make repeated measurements during several half-lives.
Type of non-imaging device ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
[object Object],[object Object]
[object Object],[object Object]
The gamma well counter ,[object Object],[object Object],[object Object],[object Object]
Examples of use of sample counters RIA 125 I Kidney clearance 51 Cr Vitamin B12 deficiency 57 Co, 58 Co Ferrokinetic studies 59 Fe Total body water 3 H Blood volume 125 I,  51 Cr,  99m Tc Biomedical research   3 H,  14 C
Gamma counter HV Ampl. PHA Timer Scaler Rate- meter Gain  Base  Window Voltage Detector  Sample Lead shield  PM-tube
Scintillation detector Amplifier PHA Scaler Proportionality between the signal and the energy absor- bed in the detector
Pulse height analyzer UL LL Time Pulse height (V) The pulse height analyzer allows only pulses of a certain height (energy) to be counted. counted not counted
Pulse-height distribution NaI(Tl)
The  T hyroid  P robe ,[object Object],[object Object],[object Object]
Probe system HV Ampl. PHA Timer Scaler Rate- meter Gain  Base  Window Voltage Recorder Collimator PM D
Quality control of any scintillation detector   system ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Window setting Energy window setting depends on the energy resolution of the detector and the photon energies
Gamma counter Different design of the detector
COUNT LOSSES ( LINEARITY OF ACTIVITY RESPONSE) ,[object Object],[object Object]
Liquid scintillation  counter
Liquid scintillation counter ,[object Object],[object Object],[object Object]
Liquid scintillation counter ,[object Object],[object Object],[object Object],[object Object]
Liquid scintillation counter PM PM Coinc Ampl PHA Scaler Timer No window 100% geometric efficiency Sample mixed with scintillation solution
Liquid scintillation counter ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],Operational considerations
Thank you  Pawitra Masa-at   4937092 SIRS/M March 23, 2007

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Non-Imaging Devices in Nuclear Medicine

  • 1. Non-imaging devices in Nuclear Medicine Pawitra Masa-at 4937092 SIRS/M March 23, 2007
  • 2.
  • 4. Gas-Filled Detectors I ; Ionization chamber region P ; Proportional region GM ; Geigur-Mueller region
  • 5.
  • 6. Ionization Chamber HV + - Negative ion Positive ion 1234 Electrometer The response is proportional to ionization rate (activity, exposure rate)
  • 7.
  • 8.
  • 9. Dose calibrators SC97 Proportionality between the number of photons emitted and the ionization current Well-shaped ionization chamber filled with a gas of high atomic number (e.g. Xenon) and kept under pressure
  • 10.
  • 11. ACTIVITY MEASUREMENT Setting Measured activity Tc-99m 1.00 Co-57 1.19 In-111 2.35 Tl-201 1.76 Ga-67 1.12 I-123 2.19 I-131 1.43 Measured activity/True activity of Tc.99m if the indicated settings are used
  • 12. Geometric efficiency The quotient: number of photons reaching the detector over the number of photons emitted from the sample Increasing geometric efficiency
  • 14.
  • 15.
  • 16. Sealed sources for calibration of activity meters 1.9 5.27 y 1173, 1332 Co-60 7.4 30 y 662 Cs-137 9.3 10.7 y 81, 356 Ba-133 185 271 d 122 Co-57 Activity (MBq) Half-life Photon energy (keV) Radionuclide
  • 17. Measurement of precision and accuracy Source (sealed) : Cs-137 or Co-57 Procedure: Select settings for the radionuclide and adjust background. Insert source in holder and make 10 measurements. Data analysis : To assess precision , calculate for each source (i) the percentage difference between the measured activity A i and their mean A mv . (+/-5%) To assess accuracy , calculate the percentage difference between the mean activity and the certified activity. (+/- 10%).
  • 18. Measurement of reproducibility Measure the activity of a sealed reference source e.g. every morning. Use Tc-99m settings.
  • 19.
  • 20. Measurement of linearity Use a radionuclide with short half-life e.g. Tc-99m Make repeated measurements during several half-lives.
  • 21.
  • 22.
  • 23.
  • 24.
  • 25. Examples of use of sample counters RIA 125 I Kidney clearance 51 Cr Vitamin B12 deficiency 57 Co, 58 Co Ferrokinetic studies 59 Fe Total body water 3 H Blood volume 125 I, 51 Cr, 99m Tc Biomedical research 3 H, 14 C
  • 26. Gamma counter HV Ampl. PHA Timer Scaler Rate- meter Gain Base Window Voltage Detector Sample Lead shield PM-tube
  • 27. Scintillation detector Amplifier PHA Scaler Proportionality between the signal and the energy absor- bed in the detector
  • 28. Pulse height analyzer UL LL Time Pulse height (V) The pulse height analyzer allows only pulses of a certain height (energy) to be counted. counted not counted
  • 30.
  • 31. Probe system HV Ampl. PHA Timer Scaler Rate- meter Gain Base Window Voltage Recorder Collimator PM D
  • 32.
  • 33. Window setting Energy window setting depends on the energy resolution of the detector and the photon energies
  • 34. Gamma counter Different design of the detector
  • 35.
  • 37.
  • 38.
  • 39. Liquid scintillation counter PM PM Coinc Ampl PHA Scaler Timer No window 100% geometric efficiency Sample mixed with scintillation solution
  • 40.
  • 41. Thank you Pawitra Masa-at 4937092 SIRS/M March 23, 2007

Notas del editor

  1. This image shows the importance to use the correct setting of the instrument. It should be read as follows; If the sample to measure contains Tc99m and the setting of the activity meter is for e.g. I-123 then the measured activity will be 2.19 times the correct value.
  2. The image should be used to point out the importance of reproducible geometry .
  3. This is an example of an automatic sample holder which guaranties reproducible geometry
  4. Another way to document the result is by using the first measurement as standard and then calculate the expected activity at different times and hence plot the measured activity vs the calculated activity. The measurements can also be performed using specially designed attenuators, meaning that all the measurements can be made within a very short time.
  5. It is important to explain why there is a proportionality between the photon energy absorbed in the detector and the pulse height
  6. Explain the origin of the scattered photons (detector and sample) and the completely absorbed photons.
  7. Why use a limited window (B) instead of one that covers the whole pulse height distribution (A)?